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https://www.jiskha.com/questions/14752/i-really-need-help-with-this-question-i-keep-doing-it-wrong-so-can-anyone-help-me-please | [
"# Management Accounting\n\nI really need help with this question. I keep doing it wrong so can anyone help me please.\n\n------------------------------------------------------------ -------\n\nThe maori novelty company makes a variety of souvenirs for visitors to New Zealand. The Otago division manufactures stuffed kiwi birds using a highly automated operation. A recently installed activity based costing system has four acitivities:\n\nActivity CostDriver Rate\n\nMaterials handling Kilograms of materials \\$1.20 per kg\n\nProduction setup # of setup \\$60 per setup\n\nCuttting, sewing etc # of units \\$0.40 per unit\n\nPackaging and shipping #of orders \\$10 per order\n\nTwo products are called Standard kiwi and giant kiwi. They require 0.20 and 0.40 kg, respectively, at a material cost of 1.30 for standard kiwis and 2.20 for giant kiwis. One computer controlled assembly line makes all the products. When a production run of a different product is started, a setup procedure is required to reprogram the computers and make other changes in the process. Products are packed and shipped separately so a request from a customer for, say, 3 different products is considered 3 different orders Ausiland Waterfront market just placed an order for 100 standard kiwis and 50 giant kiwis.\n\n1. Suppose the products made for Ausiland Waterfront required “AWM” to be printed on each kiwi. Because of the automated process, printing the initials takes no extra time or materials but it requires a special production setup for each product. Compute the cost of production.\n\n1. 👍 0\n2. 👎 0\n3. 👁 165\n\n## Similar Questions\n\n1. ### CHEM\n\nFor a molecule of fluorous acid, the atoms are arranged as HOFO. What is the formal charge on each of the atoms? Enter the formal charges in the same order as the atoms are listed. For this question I tried entering: +1,-2,+3,-2\n\nasked by K on November 26, 2007\n2. ### math\n\nA test had 200 questions .Each correct answer carried 2 marks.Each wrong answer carried -1/2 marks and unanswered question fetched no marks .Ajay attempted all the question in the test and he scored 360 marks.What would his marks\n\nasked by rachel on November 28, 2014\n3. ### Chemistry\n\nOF2(g) + H2O(g) -> O2(g) +2HF(g) ΔH°rxn = -318 kJ Using bond energies, calculate the bond dissociation energy of the O-F bond, in OF2. This is the question and I got 438 as the answer, which is wrong. I don't know what I did\n\nasked by Kat on May 1, 2011\n4. ### chemistry\n\nI keep getting wrong answers for this question. Determine the pH of an HF solution of each of the following concentrations. a) .280 M b) 5.3*10^-2 M c) 2.50*10^-2 M No Ka has been given. I haven't attempted b or c yet because I\n\nasked by maura on March 29, 2012\n5. ### toxicology- can someone re work this question?\n\nHi, I have to answer this question \"why do we say that metabolism is the factor that most accounts for differences among species in the toxicity of some xenobiotics? I don't understand what the question means- I understand all the\n\nasked by brian on February 20, 2008\n1. ### Maths\n\nThere was a question: A gallon jug of milk is 3/4 full. After breakfast, you drink 1/12 of the milk. What fraction is the gallon is left? And here was my answer: 1/12 drank --> 11/12 left 3/4*11/12=11/16 But I got the question\n\nasked by Nana on October 28, 2013\n2. ### math11\n\nSolve the non linear equation x^2=3x+4 graphically using a calculator, Write the equations of the graphs you used to find the solution. I got this question wrong what would be my Y1= and Y2= equations. Not sure what I'm doing\n\nasked by Juliet on October 19, 2010\n3. ### math11\n\nSolve the non linear equation x^2=3x+4 graphically using a calculator, Write the equations of the graphs you used to find the solution. I got this question wrong what would be my Y1= and Y2= equations. Not sure what I'm doing\n\nasked by Juliet on October 19, 2010\n4. ### Simplfing Fractions\n\nThree problems I need to know if I am correct or not if not I will place how I got the answer and maybe some one can show me where I messing up aT Simplify 1+2/3 over top 2+1/2 My answer was 2/3 to me it does not seem right If I\n\nasked by Toni on June 1, 2007\n5. ### Chemistry\n\nFor a 0.47 M solution of LiClO compute the pH. Hi. I am confused about this question. I calculated the pH...but my answer is wrong. what am I doing wrong??? pH=-log(0.47) pH=0.33\n\nasked by J on November 13, 2016\n6. ### algebra\n\nSolve for s in this equation. Depreciation. D=C-s/n This is my answer D-C=C-s/n-c D-C=-s/n -n(D-C)=-s/n*(-n) -nD+nC=s s=n(C-D) Please chack to see if this is correct Looks fine to me. A slightly shorter (by 2 lines) rearragement\n\nasked by jessica on April 4, 2007"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.95106614,"math_prob":0.67211837,"size":3127,"snap":"2020-24-2020-29","text_gpt3_token_len":937,"char_repetition_ratio":0.13896894,"word_repetition_ratio":0.15834768,"special_character_ratio":0.29645026,"punctuation_ratio":0.094827585,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9774055,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-07-10T09:30:55Z\",\"WARC-Record-ID\":\"<urn:uuid:19b89830-7e39-46f6-9c80-ae9b1b0768b9>\",\"Content-Length\":\"25016\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:2f942100-a11d-4a4c-8904-5e9f28a92a87>\",\"WARC-Concurrent-To\":\"<urn:uuid:30451683-f54b-4d23-8196-90f22f965e93>\",\"WARC-IP-Address\":\"66.228.55.50\",\"WARC-Target-URI\":\"https://www.jiskha.com/questions/14752/i-really-need-help-with-this-question-i-keep-doing-it-wrong-so-can-anyone-help-me-please\",\"WARC-Payload-Digest\":\"sha1:WZJS65AKYHATUFLTPE2NRZZMI4EDJ2MH\",\"WARC-Block-Digest\":\"sha1:ZQHLBXQUCJC5SJ7YIBIDPOWNUVIT3TY4\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-29/CC-MAIN-2020-29_segments_1593655906934.51_warc_CC-MAIN-20200710082212-20200710112212-00025.warc.gz\"}"} |
https://studylib.net/doc/10587983/id-1050-practice-exam-3 | [
"# ID 1050 Practice Exam 3",
null,
"```ID 1050 Practice Exam 3\nDiscrete Data\nThe set of questions below all use the following set of data points taken from a discrete sample:\n1, 2, 3, 4, 4, 4, 5, 5, 6, 6.\n1) Make a bar graph of this data using the blank graph provided.\n2) What is the mean of this distribution?\na) 10\nb) 4\nc) 4.5\nd) 9\n5) What is the standard deviation of this sample\ndata set?\na) 1.63\nb) 1.55\nc) 4.00\nd) 2.67\n3) What is the median of this distribution?\na) 10\nb) 4\nc) 4.5\nd) 9\n6) What is the variance of this distribution?\na) 1.63\nb) 1.55\nc) 4.00\nd) 2.67\n4) What is the mode of this distribution?\na) 10\nb) 4\nc) 4.5\nd) 9\n7) What is the skewness of this distribution?\na) 1.22\nb) 4.00\nc) 1.41\nd) 0.00\nDefinitions\n8) A set of classes or groups based on name only,\nwithout a mathematical value or order (example:\nhair color):\na) A nominal scale\nb) An ordinal scale\nc) An interval scale\n10) A set of classes or groups based on their\nmathematical value relative to an absolute zero\n(example: height):\na) A nominal scale\nb) An ordinal scale\nc) A ratio scale\n9) A set of classes or groups based on relative rank\nonly, without a mathematical value (example:\nrelative dominance):\na) A nominal scale\nb) An ordinal scale\nc) A ratio scale\n11) The entire set of people or objects one wishes to\ncharacterize is called the _______. The subset\nthat is actually measured is called the ________.\na) Population; sample\nb) Sample; population\nR. Gist\n1 of 4\nVer. D, Rev. 1\nID105 Exam 3\nContinuous Data\nThe set of questions below are all taken from the following set of data which comes from a\nsample which is continuously distributed:\n1.1, 1.2, 1.3, 1.8, 2.4, 2.5, 3.7, 4.1, 4.8, 5.3\n12) Draw a histogram of this data. Use the number of classes and the class width that is shown on the following\nblank graph:\n13) What is the mean of this data?\na) 2.82\nb) 2.40\nc) 1.50\nd) 1.70\n16) What is the standard deviation of this sample\ndata set?\na) 2.41\nb) 1.50\nc) 1.55\nd) 4.56\n14) What is the median of this data?\na) 2.40\nb) 2.45\nc) 2.50\nd) 2.82\n17) What is the variance of this data?\na) 2.41\nb) 1.50\nc) 1.55\nd) 4.56\n15) What is the mode of this data?\na) 2.45\nb) 2.40\nc) 1.50\nd) 1.70\n18) What is the skewness of this data?\na) 1.50\nb) 4.50\nc) 0.85\nd) -1.75\nMore Definitions\n19) When you look at the graph of a set of data and\nnotice that there is a pronounced tail going off to\nthe left, you can be pretty convinced that the data\nhas ________.\na) Negative skewness\nb) Positive skewness\nc) No skewness\n22) Variables that can take on any real number value\n(integer or decimal) are:\na) Discrete variables\nb) Skewed variables\nc) Continuous variables\nd) Standard variables\n20) The measures of central tendency are:\na) The mean\nb) The mode\nc) The median\nd) All of the above\nR. Gist\n21) The measures of the spread or precision of the\ndata are:\na) The standard deviation and the variance\nb) The mean and the variance\nc) The skewness and the variance\nd) The mean and the skewness\n2 of 4\nVer. D, Rev. 1\nID105 Exam 3\nThe Normal Curve\nThe set of questions below are based on the following normal curve. This particular curve\nrepresents the scores of a large population on a standard SAT exam. The mean is 500 (=500)\nand the standard deviation is 100 (=100). The percentages given below represent the\npercentage of the population between the values on the horizontal axis.\n23) On the standard SAT exam, Debbie scores 600.\nWhat percentage of all people taking this test\nwill score higher than Debbie?\na) 0.5%\nb) 2.5%\nc) 16%\nd) 84%\n26) What is the highest grade someone else could\nhave and still be in the lowest 16% of everyone\ntaking the test?\na) 300\nb) 400\nc) 500\nd) 600\n24) Using Debbie as an example, you can say that\nher grade lies at the ______ percentile.\na) 0.5 th\nb) 2.5 th\nc) 16 th\nd) 84 th\n27) What percentage of all people taking the exam\nscored at least a 300?\na) 2.5%\nb) 16%\nc) 84%\nd) 97.5%\n25) What is the lowest grade someone else could\nhave and still be in the top 84% of all people\ntaking the test?\na) 300\nb) 400\nc) 500\nd) 600\n28) What percentage of all people taking the exam\nscored between 400 and 600?\na) 34%\nb) 68%\nc) 16%\nd) 2.5%\nR. Gist\n3 of 4\nVer. D, Rev. 1\nID105 Exam 3\nThe Standard Normal Curve\nThe next set of questions is based on the standard normal curve. Use the z-score table at the\n29) What area is under the curve to the right of a\nz-score of 0.8?\na) 0.212\nb) 0.455\nc) 0.500\nd) 0.882\n30) What area is under the curve to the right of a\nnegative z-score of z= -1.0?\na) 0.104\nb) 0.308\nc) 0.500\nd) 0.841\nThe next set of questions is based on normally distributed data representing the age of a certain\npopulation of 1000 individuals. The data has an average of 50 (=50) and a standard deviation\nof 10 (=10). [Recall that z=(x-)/] Using the z-score table at the bottom of this page, answer\nthe following:\n31) What percentage of the\npopulation is above an age\nof 50?\na) 20 %\nb) 50 %\nc) 70 %\nd) 99.5%\n32) What percentage of the\npopulation is between 35\nand 65 years old?\na) 6.7 %\nb) 30.8 %\nc) 68.0 %\nd) 86.6 %\n33) How many in the\npopulation are between 35\nand 65 years old?\n____________________________________________________________________________\nZ-Score Table\n(A)\nz-score\n0.0\n0.1\n0.2\n0.3\n0.4\n0.5\n0.6\n0.7\n0.8\n0.9\n1.0\n1.1\n1.2\n1.3\n1.4\n1.5\nR. Gist\n(B)\nArea between z\nand the mean\n0.000\n0.040\n0.079\n0.118\n0.155\n0.192\n0.226\n0.258\n0.288\n0.316\n0.341\n0.364\n0.385\n0.403\n0.419\n0.433\n(C)\nArea beyond\nz\n0.500\n0.460\n0.421\n0.382\n0.345\n0.309\n0.274\n0.242\n0.212\n0.184\n0.159\n0.136\n0.115\n0.097\n0.081\n0.067\n(A)\nz-score\n1.6\n1.7\n1.8\n1.9\n2.0\n2.1\n2.2\n2.3\n2.4\n2.5\n2.6\n2.7\n2.8\n2.9\n3.0\n4 of 4\n(B)\nArea between z and\nthe mean\n0.445\n0.455\n0.464\n0.471\n0.477\n0.482\n0.486\n0.489\n0.492\n0.494\n0.495\n0.496\n0.497\n0.498\n0.499\n(C)\nArea\nbeyond z\n0.055\n0.045\n0.036\n0.029\n0.023\n0.018\n0.014\n0.011\n0.008\n0.006\n0.005\n0.004\n0.003\n0.002\n0.001\nVer. D, Rev. 1\n```"
] | [
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"https://s2.studylib.net/store/data/010587983_1-d7234a42e7603e055ef89f0a39b2ba23-768x994.png",
null
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https://mammothmemory.net/physics/transformers/transformer--energy-can-not-be-lost-or-gained/transformer-energy-can-not-be-lost-or-gained.html | [
"",
null,
"# Transformer – energy cannot be lost or gained\n\nNow we know that doubling the coils doubles the voltage and therefore:\n\nV_1/V_2=(Number\\ \\turns\\ \\1)/(Number\\ \\ turns\\ \\2)\n\nWe must also remember that:\n\nPower can not be lost or gained\n\nIf Power=VI and power can not be lost or gained it follows that if voltage is increased, current is reduced and vice versa. Remember:\n\nV\\o\\l\\t\\a\\g\\e\\ \\1xxCurrent\\ \\1=Primary\\ \\Power=S\\e\\c\\o\\n\\d\\a\\r\\y\\ \\Power=V\\o\\l\\t\\a\\g\\e\\ \\2xxCurrent\\ \\2\n\n(NOTE: Secondary power is slightly less due to small inefficiencies, but they are ignored here)\n\nThis is an easy way for you to remember that:\n\n V_1xxI_1=V_2xxI_2\n\n 1000 v and 1 Amp equals 1000 watts 1 volt and 1000 Amps equals 1000 watts 500 v and 2 Amps equals 1000 watts 5 v and 200 Amps equals 1000 watts\n\nTherefore because\n\n V_1I_1=V_2I_2\n\n V_1/V_2=I_2/I_1"
] | [
null,
"https://mammothmemory.net/images/mobile-home.svg",
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https://education.nsw.gov.au/teaching-and-learning/learning-from-home/learning-at-home/learning-packages/year-5-and-6-learning-packs/maths/package-3-lets-get-magical | [
"Package 1-3: Let’s get magical!\n\nIn this activity your child will use magic tricks to develop mathematical reasoning and practise their skills in mental computation.\n\nWeek 2 - Package 3 - Year 5 and 6 Mathematics - Let’s get magical!\n\nThings you need\n\nIdeal Back up\n\nPencils or markers\n\nPaper\n\nNumbered cards 0-9\n\nUNO cards\n\nWhy is this activity important?\n\nMagic tricks provide great opportunities for students to develop mathematical reasoning and practise their skills in mental computation. This trick is helpful for practising addition and subtraction facts. It also helps students develop skills in choosing efficient strategies for solving addition and subtraction problems. Practising the magic trick multiple times helps students develop confidence, consolidate skills in mental computation and helps them see the maths underlying the magic.\n\nBefore you start\n\nYou need some pens and a piece of paper.\n\nNumbered cards are required for the optional activities.\n\nWhat your child needs to know and do\n\nStudent needs to be able to add and subtract 3-digit numbers.\n\nWatch the video Let's get magical!\n\nWhat to do next\n\n• Choose a 3-digit number where each digit is smaller than the previous one (but they don’t have to be in order. For example, 982 or 531.)\n\n• Then, reverse the digits and subtract the second number from the first one. So, if I had chosen 531, I would now work out 531 – 135. The answer is 396. (If you get 99, record your answer as 099.)\n\n• Next, reverse your new number. For example, from 396 I can make 639.\n\n• Finally, add these last two numbers together. For example, 396 + 639.\n\n• Here comes the magic...\n\nActivity too hard? Activity too easy?\n\nComplete a different magic trick (‘Predict your puzzle’), detailed below\n\nTry using a different strategy to do the calculations for the magic trick. For example, you might like to use a calculator. Then, explore what happens if you follow the same rules but starting with a 2-digit number (for example, 76 or 82).\n\nComplete several times to practice using mental strategies with 2-digit numbers. Then try the trick again with 3 digit-numbers.\n\nInvestigate what happens with this magic trick using 4-digit numbers and 5-digit numbers. Complete several times to practice.\n\nWork together to explore which mental computation strategies are the most efficient when adding and subtracting.\n\nYou can also work together to investigate how this magic trick works!\n\n• Try another starting number and test it out again...is the final answer still 1089?\n\n• Explore what happens if you use the same process, starting with a 2-digit number or a 4-digit number...\n\n• Why do you think this might be happening?\n\nNow try this magic trick!\n\n1. Choose a number in the grid and circle it.\n\n2. Choose another number which is not in the same row or column as the first number and circle it.\n\n3. Pick a third number which is not in the same row or column as either of the other numbers you have circled.\n\n4. Pick a fourth number which is in no other column or row as the other circled numbers.\n\n5. Add all 4 numbers which are circled together.\n\n1 2 3 4\n\n5\n\n6\n\n7\n\n8\n\n9\n\n10\n\n11\n\n12\n\n13\n\n14\n\n15\n\n16\n\n1. Try this puzzle again.\n\n2. Share it with a family member.\n\n3. Explore....how does this work?\n\n1 2 3 4\n\n5\n\n6\n\n7\n\n8",
null,
"9\n\n10",
null,
"11\n\n12\n\n13",
null,
"14\n\n15\n\n16\n\nExample: 3 + 8 + 10 + 13= 34"
] | [
null,
"https://lh5.googleusercontent.com/9BBd7jc0Yz2sbtnFdDIkNtvf4pBYPdWRZNJVhYUIo0JQsRWyVL5gzCsfpso6PHfQbLi5g0gb27etlF7TyMj3L3CCw5minHDJ7fKfqsRzdnmVnm1j6IFNxpt3QrwdTtepziJYeWI",
null,
"https://lh5.googleusercontent.com/9BBd7jc0Yz2sbtnFdDIkNtvf4pBYPdWRZNJVhYUIo0JQsRWyVL5gzCsfpso6PHfQbLi5g0gb27etlF7TyMj3L3CCw5minHDJ7fKfqsRzdnmVnm1j6IFNxpt3QrwdTtepziJYeWI",
null,
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https://link.springer.com/article/10.1007/s10346-016-0783-6 | [
"## Introduction\n\nLandslides starting from unstable slopes affect the safety of life as well as of private and public assets. Computer models are employed to identify potentially unstable areas in order to facilitate decision-making at various levels. Whilst statistical models explore the relationships between the spatial patterns of landslide occurrence and a set of predictor layers, physically based models attempt to reproduce or to predict the physical mechanisms involved (Guzzetti et al. 1999; Van Westen 2000; Guzzetti 2006; VanWesten et al., 2006). Physically based models are frequently employed to estimate landslide susceptibility at the scale of small catchments (VanWesten et al., 2006). As long as shallow landslides are considered, these approaches mostly rely on the infinite slope stability model. It is commonly used in raster-based geographic information system (GIS) environments to derive a factor of safety for each pixel. However, the infinite slope stability model is unconditionally suitable only for those areas where shallow translational landslides with a length-to-depth ratio L/D >16–25 are expected (Griffiths et al. 2011; Milledge et al. 2012). As shallow landslides are most commonly triggered by extreme hydrometeorological events, such modelling tools are often coupled with more or less complex hydraulic models (e.g., Montgomery and Dietrich 1994; Van Westen and Terlien 1996; Burton and Bathurst 1998; Pack et al. 1998; Wilkinson et al. 2002; Xie et al. 2004a; Baum et al. 2008; Godt et al. 2008; Muntohar and Liao 2010; Mergili et al. 2012).\n\nFor areas with deep-seated landslides, models assuming spherical, ellipsoidal or complex sliding surfaces reproduce the stability situation in a more appropriate way. Whilst they are standard in geotechnical engineering, their implementation with GIS is non-trivial so that catchment-scale applications are less commonly applied (e.g. Xie et al. 2003, 2004b, 2006; Jia et al. 2012; Mergili et al. 2014a, b).\n\nEven simple slope stability or hydraulic models rely on parameters which are highly uncertain in their horizontal and vertical distribution. One possible concept to account for parameter uncertainty is the probability of failure (Tobutt 1982) which has started to complement the conventional factor of safety with increasing computational power, considering parameter spaces using random or regular sampling of uncertain parameters (Mergili et al. 2014a). Various authors have introduced and used different types of probability density functions (pdfs) of geotechnical (El-Ramly et al. 2005; Petrovic 2008; Mergili et al. 2014a) and geohydraulic parameters (Mesquita et al. 2002, 2007; Mesquita and Moraes 2004) which can be employed for parameter sampling. Whilst such functions are a smart way to deal with uncertain information, they are not necessarily transferable between different locations and therefore commonly suffer from small sample sizes and, consequently, weakly supported means and standard deviations.\n\nAs the challenge of uncertain parameters is encountered in many fields of geosciences, various approaches have been developed in the previous decades to test the sensitivity of the model results or the model performance to the input parameters or to optimize (calibrate) the input parameters in order to bring the model results in line with reference observations. Testing one parameter at a time is thereby considered inappropriate as both the optimum value and the sensitivity may strongly interrelate with the values of other parameters (Saltelli and Annoni 2010). Multi-parameter strategies are therefore required (e.g., Duan et al. 1992; Eberhart and Kennedy 1995; Hay et al. 2006; Vrugt et al. 2008; Fischer 2013). Optimized parameters or parameter sets, however, are not necessarily meaningful from a physical point of view. Particularly when calibrating many parameters at once, a good model performance in terms of reproducing the observation can be achieved despite a poor process understanding. The sensitivity of local-scale slope stability model results to selected input parameters was tested, e.g. by Griffiths and Fenton (2004) or by Wang et al. (2010). Guimarães et al. (2003) and Formetta et al. (2015) have applied parameter optimization strategies at catchment scale.\n\nAlmost all documented parameter sensitivity and optimization strategies target at discrete parameter values. We think that, particularly at broader scales, sensitivity analysis and optimization of parameter values is inappropriate as it disregards the inherent fine-scale spatial variability of the parameters. Instead, we suggest performing sensitivity analysis and optimization of parameter ranges.\n\nThe present article demonstrates such a strategy, employing a modification of the probability of failure concept. We investigate how the considered ranges of geotechnical and geohydraulic input parameters influence the results and performance of GIS-based catchment-scale slope stability models. For this purpose, we apply the infinite slope stability model, the sliding surface model of the tool r.slope.stability and the software Transient Rainfall Infiltration and Grid-Based Regional Slope-Stability Model (TRIGRS) to the Quitite and Papagaio catchments, Rio de Janeiro, Brazil. The findings are thought to be useful to identify suitable parameterization strategies for future slope stability modelling efforts.\n\nNext, we introduce the study area (“Study area and data” section) and describe the components of the proposed work flow (“Methods” section). We then demonstrate (“Results” section) and discuss (“Discussion” section) the results obtained before drawing our conclusions (“Conclusions” section).\n\n## Study area and data\n\nThe study area includes the two landslide-prone Quitite and Papagaio watersheds located in the western part of the city of Rio de Janeiro, Brazil (Fig. 1). Together, they cover an area of 4.4 km2, extending between 12 and 995 m a.s.l. The climate in the area is tropical humid (Guimarães et al. 2009). Due to influence by ocean moisture, the area receives a higher amount of rainfall than the central part of Rio de Janeiro (Hurtado Espinoza 2010). Granitic bedrock dominates both watersheds. The homogeneous, colluvial yellow soil is characterized by sandy-clay features (Hurtado Espinoza 2010; Galindo 2013; Galindo and Campos 2014) and a depth of 1–3 m (Guimarães et al. 2003). Native forest is still the dominant type of vegetation whilst the anthropogenic influence on the land cover is of limited importance (Guimarães et al. 2003; Hurtado Espinoza 2010).\n\nGuimarães et al. (2003) optimized values of effective cohesion c’ (kN m−2), normalized to depth d, effective angle of internal friction φ’ and specific weight of the saturated soil γ s (kN m−3) using published parameters for geomorphologically comparable adjacent areas and back-calculations with the software SHALSTAB. These authors arrived at best fit values of c’/d = 2 kN m−3, φ’ = 45° and γ s = 15 kN m−3, but they also indicated that, in general, low values of c’/d, high values of φ’ and values from 15 to 17.5 kN m−3 for γ s would be appropriate for the area. They proposed a general frame of parameter values realistic for the area (in the sense of a parameter space) summarized in Table 1 and, with some modifications, applied to tests A and B (see “Methods” and “Results” sections). Hurtado Espinoza (2010) measured a dry specific weight around 15 kN m−3 for some undisturbed samples taken at 1 m depth. The same authors stated that the slopes in the lower areas would be weaker whilst those in the higher areas would be stronger.\n\nValues of soil saturated conductivity K s were measured by Fernandes et al. (2001) using Guelph’s permeameter. The results showed a high variability with values ranging from 10−6 to 10−4 m s−1 as well as some important discontinuities in the profiles, possibly influencing groundwater flow.\n\nWe consider a landslide event related to intense rainfall on 13 and 14 February 1996. Within 48 h, 394.3 mm of rainfall was registered at the Alto da Boa Vista station, and 245.9 mm at the Jacarepaguá station, both located in close vicinity to the Quitite and Papagaio catchments and operated by the National Meteorological Institute (INMET; Conti 2012). A landslide inventory developed by Guimarães (2000) is used in the present work. According to this inventory, the rainfall event has triggered 93 landslides, occupying 0.14 km2 (3.1% of the entire area). Table 2 summarizes the main characteristics of the landslide inventory. Most landslides occurred in the native forest areas dominating the study area. Shallow landslides, debris flows and debris avalanches were most common. The sliding surfaces of most landslides coincided with the soil-rock interface (Guimarães et al. 2003; Miqueletto and Vargas, 2009; Hurtado Espinoza 2010). The landslide inventory displays the entire extent of the directly affected areas without distinguishing between release, transit and deposition areas.\n\nBesides the geotechnical and geohydraulic information and the landslide inventory, we use a 2-m resolution digital elevation model (DEM).\n\n## Methods\n\n### Work flow and software\n\nFigure 2 illustrates the general work flow of the study. We compute the slope failure susceptibility index (SFSI) (dimensionless number in the range 0–1) based on sets of factor of safety (FOS) values derived through the controlled variation of selected key parameters within a defined parameter sub-space. This procedure is repeated for various sub-spaces. The resulting SFSI values are evaluated against the inventory of observed landslides, and the findings are compared and interpreted.\n\nIn a first step, we vary the geotechnical parameters (tests A and B) and in a second step, we vary the geohydraulic parameters (test C). Test D uses a simple statistical model for the sake of comparison. Test A builds on the infinite slope stability model, test B on the sliding surface model of the tool r.slope.stability (Mergili et al. 2014a, b), designed as a raster module of the open source GRASS GIS software (Neteler and Mitasova 2008; GRASS Development Team 2016). Test C makes use of TRIGRS (Transient Rainfall Infiltration and Grid-Based Regional Slope-Stability Model; Baum et al. 2008), which is a grid-based tool simulating the permanent and transient rainfall influences on slope stability. Python scripting is used to derive SFSI, and the R Project for Statistical Computing (R Core Team, 2016) is employed for the evaluation of the results. Test D relies entirely on Python and R scripting.\n\n### Geotechnical model\n\nSlope stability modelling commonly builds on the limit equilibrium theory (Duncan and Wright 2005): a factor of safety (FOS) is computed as the ratio between resisting forces R and driving forces T:\n\n$$\\mathrm{FOS}=\\frac{R}{T}$$\n(1)\n\nWhen FOS = 1, the slope is in static equilibrium. Values of FOS <1 indicate potential failure (in reality, such slopes do not exist), values of FOS >1 indicate stable slopes. The use of this method requires the prior definition of a slip surface, and the soil is considered as rigid material.\n\nFor GIS-supported catchment-scale analyses of slope stability, the infinite slope stability model is most commonly employed (Montgomery and Dietrich 1994; Pack et al. 1998; Xie et al. 2004a; Baum et al. 2008). It assumes (i) a uniform slope of infinite length, and (ii) a plane, slope-parallel failure surface. As inter-slice forces do not have to be considered, it is conveniently applied on a pixel-to-pixel basis. Based on Eq. (1), FOS can be expressed in various ways. For fully saturated soil, the equation may be formulated as follows (modified after Baum et al. 2008):\n\n$$\\mathrm{FOS}=\\frac{ \\tan \\phi}{ \\tan \\alpha}+\\frac{c- u \\tan \\phi}{\\gamma_s d \\sin \\alpha \\cos \\alpha}$$\n(2)\n\nwhere α is the slope angle, u (N m−2) is the pore water pressure, γ s (N m−3) is the specific weight of the saturated soil and d (m) is the depth of the sliding surface.\n\nIn the present work, we use the infinite slope stability model implemented with r.slope.stability and with TRIGRS. Alternatively, we also apply the sliding surface model of r.slope.stability. Thereby, the slope stability is tested for a large number of randomly selected ellipsoid-shaped potential sliding surfaces, truncated at the depth of the soil. R and T are summarized over all pixels intersecting a given sliding surface, and FOS is computed for each surface in a way analogous to Eqs. 1 and 2, applying a modification of the Hovland (1977) model. Finally, the minimum value of FOS resulting from the overlay of all sliding surfaces is applied to each pixel. For a more detailed description of the sliding surface model of r.slope.stability, we refer to Mergili et al. (2014a, b).\n\n### Geohydraulic model\n\nIn TRIGRS, FOS is computed for one or more user-defined depths. The Richard’s equation is used to calculate the soil transient infiltration for saturated and unsaturated soil conditions (Iverson 2000):\n\n$$\\frac{\\partial \\psi}{\\partial t}\\frac{d\\theta}{d\\psi}=\\frac{\\partial }{\\partial x}\\left[{K}_L\\left(\\psi \\right)\\left(\\frac{\\partial \\psi}{\\partial x}- \\sin \\alpha \\right)\\right]+\\frac{\\partial }{\\partial y}\\left[{K}_L\\left(\\psi \\right)\\left(\\frac{\\partial \\psi}{\\partial y}\\right)\\right]+\\frac{\\partial }{\\partial z}\\left[{K}_z\\left(\\psi \\right)\\left(\\frac{\\partial \\psi}{\\partial z}- \\cos \\alpha \\right)\\right]$$\n(3)\n\nwhere ψ (m) is pressure head, θ is soil volumetric water content, t (s) is time, K L (m s−1) is lateral soil conductivity and K z (m s−1) is soil conductivity in z direction.\n\nTo solve the Richards equation, TRIGRS uses an approach developed by Iverson (2000), considering homogeneous soil, isotropic flow, relatively shallow depth, one-dimensional vertical downslope flow and soil moisture close to saturated conditions (Baum et al. 2008; Park et al. 2013), following the heat conduction approach described by Carslaw and Jaeger (1959). We refer to Baum et al. (2008) for a detailed description of the procedure.\n\nFor computing the groundwater level, TRIGRS compares the infiltrated water volume V I and the maximum drainage capacity of the soil V D. If V D ≥ V I, the water table remains constant. Otherwise, the water table rises, depending on K s and the transmissivity T. For unsaturated conditions, the maximum value of ψ is the new water level multiplied with β (value set according to the adopted flow condition). The amount of water exceeding the maximum infiltration rate is considered surficial runoff. However, surficial runoff is not taken over from one time step to the next (Baum et al. 2008).\n\n### Slope failure susceptibility index\n\nThe slope failure susceptibility index (SFSI) in the range 0–1 refers to the fraction of geotechnical and/or geohydraulic parameter combinations resulting in FOS <1, out of an arbitrary number of tested parameter combinations. This means that SFSI for a given pixel increases with each parameter combination where FOS <1 and, finally, low values of FOS correspond to high values of SFSI. The principal concept of the SFSI is identical to the concept of the slope failure probability yielded by r.slope.stability (Mergili et al. 2014a). However, we refer to it as a susceptibility index in the context of the present study as we simply use a uniform probability density function throughout all the computations. Such a distribution does not necessarily capture the real-world parameter distribution (which is unknown) and its use does therefore not justify applying the concept of probability in a strict sense.\n\n### Statistical model\n\nIn test D, a statistical model is applied for the purpose of comparison, employing the slope angle as the only predictor layer (Table 3). We keep the statistical model as basic as possible in order to evaluate the performance of a simplistic statistical approach in comparison to the physically based models (“Geotechnical model” to “Slope failure susceptibility index” sections). This allows us to conclude on the need of using more complex physically based models for catchment-scale landslide susceptibility analysis. Thereby, we overlay a classified slope map with the map of the observed landslide release areas (ORA; “Model evaluation” section) and, for each slope class, compute the fraction f C of observed landslide release pixels related to all pixels. SFSI—referred to as release probability by Mergili and Chu (2015) who employed a comparable approach—is then computed by applying f C to all pixels of the corresponding slope class. Thereby, it is important to use two different areas for the derivation of f C and for the computation and evaluation of SFSI (“Test layout” section).\n\n### Model evaluation\n\nThe landslide inventory for the Quitite and Papagaio watersheds displays the entire observed landslide impact areas (OIAs), i.e. the release, transit and deposition areas without any differentiation. We approximate the ORA as the upper third part of each OIA polygon. Depending on the test (“Test layout” section and Table 3), either the OIA map or the ORA map is overlaid with the corresponding SFSI map. When using the ORA map, the lower two-thirds portion of the OIA is not considered for evaluation. The true positive (TP), true negative (TN), false positive (FP) and false negative (FN) pixel counts are derived for selected levels of SFSI. An ROC curve is produced by plotting the true positive rates TP/(TP + FN) against the false positive rates FP/(FP + TN) derived with each combination of parameters. The area under the ROC curve AUROC indicates the predictive capacity of the model: AUROC = 1.0 (the maximum) means a perfect prediction, AUROC = 0.5 (corresponding to a straight diagonal line) indicates a random prediction, i.e. model failure. AUROC refers to the entire area used for model evaluation.\n\nIn addition, we introduce a conservativeness measure:\n\n$$\\mathrm{FoC}=\\frac{\\mu_{\\mathrm{SFSI}}}{r_{\\mathrm{OP}}}$$\n(4)\n\nwhere μSFSI is the average of SFSI over the entire study area, and r OP is the observed positive rate, i.e. the fraction of observed landslide pixels out of all pixels in the study area. If FoC >1, the model overestimates the landslide susceptibility, compared to the observation whilst values FoC <1 indicate an underestimation of the landslide susceptibility.\n\n### Test layout\n\nTables 3 and 4 summarize the main characteristics of each test and the parameter values and ranges considered.\n\nIn a first step (tests A1–A4 and B), the sensitivity of SFSI and the associated model performance to the geotechnical parameters c′ and φ′ and the shape of the sliding surface is explored, assuming fully water-saturated soils, and the depth of the sliding surface corresponding with the soil depth. The infinite slope stability model and the sliding surface model implemented in r.slope.stability are employed for this purpose. We introduce a two-dimensional parameter space constrained by lower boundaries of c′ = 0 kN m−3 and φ′ = 21°, and upper boundaries of c′ = 24 kN m−3 and φ′ = 45° (Fig. 3a; Table 4). This parameter space accounts for the full ranges of c′ and φ′ considered representative for the area (“Study area and data” section). We note that the resulting values of FOS vary according to φ′ and c′/d, so that the value of FOS obtained with d = 3 m and with a given value of c′ is identical (infinite slope stability model) or similar (sliding surface model) to the value of FOS with other values of c′ and d, but the same c′/d ratio. The dry specific weight of the soil γ d = 13.5 kN m−2 and the volumetric saturated water content θ s = 40 vol.% are set to constant values. We neglect the weight of the trees and the effects of their root systems on the cohesion: sliding surfaces are assumed to develop beneath the rooting depth.\n\nThe ranges of both c′ and φ′ are (i) considered in their entire extent; (ii) subdivided into two sub-ranges of equal extent and (iii) subdivided into three sub-ranges of equal extent (Fig. 4a, b). Considering all possible combinations of sub-ranges of the two parameters results in 36 partly overlapping parameter sub-spaces with 25 corner points. SFSI is computed for each parameter sub-space, with ten sampled parameters in each dimension (Fig. 4c). This procedure may be extended to three or more dimensions or repeated at a finer level by employing the sub-space with the best model performance as the entire space for the next level. For reasons to be explained in the “Results” section, only one level is applied in the present work. This work flow is repeated for two assumptions of soil depth and two versions of the landslide inventory used for evaluation, resulting in a total of four sub-tests (Table 3).\n\nTest C explores the sensitivity of SFSI and the associated model performance to K s and the initial depth of the water table d i (m). We introduce a two-dimensional parameter space constrained by lower boundaries of K s = 10−7 m s−1 and d i = 0 m and upper boundaries of K s = 10−4 m s−1 and d i = 3 m (Fig. 3b; Table 4). The ranges of values used are based on works of Saxton and Rawls (2006) and Guimarães et al. (2003). We set γ s = 16 kN m−2, θ s = 40 vol.%, θ r = 5 vol.%, c′ = 4.5 kN m−2, φ′ = 45° and d = 3 m to constant values. The choice of these values is supported by data from Guimarães et al. (2003) and Hurtado Espinoza (2010). We further assume constant values of diffusivity (D = 200K s ; Park et al., 2013) and initial infiltration rate (I 0 = 1.3 10−6 m s−1; Conti 2012).\n\nIn a way analogous to the geotechnical parameters, the ranges of both K s and d i are (i) considered in their entire extent, (ii) subdivided into two sub-ranges of equal extent and (iii) subdivided into three sub-ranges of equal extent, resulting in 36 partly overlapping parameter sub-spaces with 25 corner points. SFSI is computed for each parameter sub-space, with five sampled parameters in each dimension. The landslide inventory used for evaluation is ORA.\n\nThis procedure is repeated for four combinations of rainfall duration and type of pluviograph (Table 3). We assume rainfall durations of 6 and 10 h and a total rainfall amount derived from the measurements at the Jacarepaguá and Boa Vista stations on 13 and 14 February 1996 (Conti 2012). The Thiessen method is applied for estimating the precipitation in the catchment, and 20% of interception are deduced (Coelho Netto 2005). The total rainfall considered for the analysis is 144 mm in all the scenarios C1–C4.\n\nIn test D, we apply the statistical model introduced in the “Statistical model” section for the purpose of comparison (Table 3). f C is derived for one of the two catchments. SFSI is then computed for the other catchment and evaluated against the corresponding ORA. The entire procedure is repeated in the reverse way, so that a clear separation between the model development and model evaluation areas is ensured.\n\n## Results\n\n### Tests A and B: geotechnical parameterization\n\nFigure 5 illustrates the results of test A in terms of model performance (AUROC) and conservativeness (FoC). Assuming a constant soil depth, the model performs significantly better when considering only the ORA (test A2; AUROC ≤ 0.741; Fig. 5b) instead of the entire OIA (test A1; AUROC ≤ 0.691; Fig. 5a). This result clearly indicates that the OIA is unsuitable as reference for evaluation, and an appropriate inventory sub-setting is essential. Focusing on Fig. 5b, we note that the model performance in terms of AUROC is insensitive to the variation of the geotechnical parameterization within much of the tested ranges. In particular, the sub-spaces along a diagonal line from medium-high values of c′ and low values of φ′ to low values of c′ and high values of φ′ display almost identical AUROC values to the entire parameter space and to those sub-spaces including broad ranges of c′ or broad ranges of φ′ with medium-low values of c′. Only those sub-ranges limited to high values of c′ or low values of c′ and φ′ yield significantly lower AUROC values. These sub-ranges result in poorly patterned relatively non-conservative and extremely conservative predictions, i.e. they display very low and very high FoC values, respectively. In general, the model results are very conservative, indicated by FoC > > 1. At a lower level of AUROC—and a lower level of FoC caused by a higher number of OP pixels—similar patterns are observed in Fig. 5a.\n\nVarying d as a function of the topographic wetness index exerts contrasting effects on the patterns of AUROC, depending on whether the OIA or the ORA is used as reference. With the ORA as reference (Test A4; Fig. 5d), the sub-spaces with low values of c′ perform comparable to test A2 (Fig. 5b). This is not surprising as the influence of d on FOS increases with c′ (with c′ = 0, d has no influence). However, AUROC and also FoC decrease significantly with increasing c′, resulting in a very poor performance associated to those sub-spaces with high c′, and a reduced performance associated to those sub-spaces with broad ranges of c′, compared to Fig. 5b. This trend clearly indicates that most ORA pixels spatially coincide with areas of relatively low topographic wetness index and therefore low values of d (Table 3) resulting in high values of FOS and low values of SFSI in cohesive soils.\n\nThe reverse effect occurs when using the entire OIA as reference (test A3; Fig. 5c): many pixels in the lower portions of the landslide polygons coincide with high values of the topographic wetness index. Consequently, d and the resulting values of SFSI are comparatively high for many of the OP pixels, resulting in an improved model performance, compared to the tests A1 – A3 (AUROC ≤ 0.742; Fig. 5b). However, since most of the lower parts of the landslide polygons do most likely not represent release areas, the increased performance represents an artefact of inappropriate assumptions rather than an indicator for model success.\n\nConsidering the findings outlined, we identify test A2 as most representative. Even though the full parameter space yields an insignificantly lower value of AUROC than do some of the sub-spaces, there is no basis to support the choice of a particular sub-space in this specific case. The parameter values used and optimized by Guimarães et al. (2003) are mostly located within the parameter sub-spaces with the higher values of AUROC, indicating a certain plausibility of the results (Fig. 5b). Figure 6a shows the spatial patterns of SFSI derived in the tests A1 and A2 with the full parameter space of c′ and φ′. We note that the results of those tests are similar in terms of SFSI, as only the reference information for validation is varied. The same is true for the SFSI maps derived through the tests A3 and A4 (Fig. 6b).\n\nThe spatial patterns of SFIS derived with the sliding surface model of r.slope.stability (test B) are illustrated in Fig. 6c. Applying the full parameter space of c′ and φ′ along with constant soil depth and the ORA as reference, the associated value of AUROC is almost identical to the value yielded with the infinite slope stability model (0.735 vs. 0.734 in test A2). Thereby, the results yielded with the sliding surface model are more conservative: FoC = 59.5, compared to a value of 48.3 yielded with the infinite slope stability model (Fig. 5b).\n\n### Test C: geohydraulic parameterization\n\nFigure 7 illustrates the performance (AUROC) and conservativeness (FoC) of the model results for the various parameter sub-spaces of K s and d i. Firstly, we note that the results are largely insensitive to the four assumptions of rainfall duration and hydrograph shape (C1–C4): the patterns yielded are identical for all four scenarios, even though the numbers vary slightly. Within each scenario, the model performance responds highly sensitive to variations of K s and d i: it peaks at AUROC = 0.719–0.724 for the upper sub-range of the hydraulic conductivity (K s = 10−5–10−4 m s−1) and the lower sub-range of the initial depth of the water table (d i = 0–1 m). However, the model performance drops only slightly when the full range of both parameters K s and d i is applied (AUROC = 0.711–0.712). Figure 8 presents the SFSI maps produced in test C1 with the full space of K s and d i. The SFSI maps resulting from tests C2, C3 and C4 are almost similar to the map resulting from test C1 and are therefore not shown.\n\nConstraining the model input to the lower ranges of hydraulic conductivity or to deeper initial water tables leads to a significant drop in the model performance. Considering K s ≤ 10–5.5 leads to model failure (AUROC = 0.494), independently of the range applied for d i and the rainfall scenario. In this case, FoC = 3.9 (blue font colour in Fig. 7). As expected, FoC is highest for the configurations with high K s and shallow d i and lowest for the configurations with low K s and deep d i. Its maximum coincides with the best model performance (FoC = 48.0–48.9).\n\nThese outcomes reflect the fact that, with K s ≤ 10–5.5, too little water propagates through the soil to substantially influence slope stability. The effect is similar with higher values of K s if the initial water table is too deep. A shallower initial water table and higher values of K s facilitate increased values of u over broad parts of the study area and, consequently, lead to less stable slopes (Eq. 2) and higher values of FoC. Only combinations of high K s and deep di lead to a sufficient signal to reproduce the observed landslide release patterns with a fair performance. As for tests A and B, all results are very conservative also for test C (FoC > > 1).\n\n### Test D: statistical model\n\nThe statistical model yields an average AUROC value of 0.737 (values of 0.736 and 0.738 for the two catchments) whilst, as prescribed by the approach chosen, FoC ≈ 1. The model performance corresponds remarkably well to the performance of the physically based models (tests A2 and B in particular), underlining the fact that the slope angle strongly dominates also the pattern of SFSI derived with the physically based models (Fig. 9).\n\n## Discussion\n\nWe have demonstrated that the performance of the physically based-derived slope failure susceptibility index SFSI in our study area reacts conditionally sensitive to variations in the considered spaces of selected geotechnical and geohydraulic input parameters and state variables. Those parameter configurations yielding insufficient pattern in terms of simulated landslide vs. non-landslide areas lead to a significantly poorer performance. With regard to the geotechnical information, comparable AUROC values are displayed throughout much of the parameter space considered relevant for the study area (Guimarães et al. 2003), except for those sub-spaces with low c′ and low φ′ (μSFSI close to 1) and those areas with high c′ and high φ′ (μSFSI close to 0). This constellation underlines a well-known negative relationship between c′ and φ′. Model performance in terms of AUROC responds very sensitive to variations in K s and d i within the tested ranges but insensitive to the variations in the rainfall scenarios applied. Whilst the findings for the geotechnical parameters are claimed to be broadly valid, those for K s and d i may strongly depend on the assumed rainfall duration and intensity in relation to the water capacity of the soil. In this sense, the pattern displayed in Fig. 7 might change for different rainfall events.\n\nOur findings suggest that any further parameter optimization efforts in terms of AUROC may be obsolete: the pattern of SFSI derived with the entire parameter space performs approximately as well in reproducing the observed landslide areas as the patterns of SFSI derived with various sub-spaces do. Applying broad ranges of the key parameters for physically based catchment-scale landslide susceptibility modelling is on the “safe” side as it yields results comparable in quality to those derived with the best-fit narrower ranges. Acknowledging the fact that geotechnical and geohydraulic parameters are spatially highly variable, uncertain and often poorly known, applying a narrow parameter space—or even a singular combination of parameters—bears a considerable risk to be off target. The direct effects of the vegetation (not accounted for in the present study) increase the level of uncertainty particularly in forested areas.\n\nThe conservativeness of the result in terms of FoC strongly depends on the parameter sub-spaces used as input. μSFSI is generally much higher than r OP, indicating that the model results tend to be very conservative. The ideal result should correspond to FoC = 1. Theoretically, this could be achieved by increasing the upper thresholds of the geotechnical parameters, i.e. to make the parameter spaces considered broader. However, substantially higher parameter thresholds are not realistic for the soil materials involved. We believe that the key for bringing μSFSI in line with r OP consists in appropriately capturing the fine-scale spatial variation of the geotechnical parameters: sliding surfaces most likely coincide spatially with geotechnically susceptible areas, layers or interfaces, spaced in a more or less irregular way. We consider it almost impossible to parameterize such patterns in a deterministic way. In this context, we note that in Figs. 6 and 8, some landslides coincide spatially with areas of low SFSI. Such mispredictions are most probably related to localized patches of low soil strength, increased water input or increased hydraulic conductivity or the effects of the vegetation. Whilst the variation in the local slope angle explains much of the pattern of SFSI, the residual part is most likely explained by fine-scale spatial variations of the soil and, possibly, the vegetation.\n\nConsequently, physically based landslide susceptibility maps can be produced with a minimum amount of geotechnical data but in this case only provide relative results. There is no benefit in dedicating major resources to the detailed investigation of the geotechnical and geohydraulic parameters for catchment-scale landslide susceptibility maps without accounting in detail for the spatial variation of those parameters. Various studies emphasize the major challenges in capturing the spatial variability of the key parameters such as c′ and φ′ (Mergili et al. 2015), K s (Mesquita et al. 2002, 2007; Mesquita and Moraes 2004) or soil depth (McBratney et al. 2003; Frohn and Müller 2015). More precisely, at this time, there are no means to appropriately regionalize the key input parameters of slope stability models. We have demonstrated that ad-hoc assumptions of parameter variations (soil depth) may result in a decreased model performance or, in combination with inappropriate reference data (an inventory including transit and deposition areas), may pretend an improved model performance. Notwithstanding any possible future progress in this field, we highlight two strategies to deal with the challenges identified:\n\n1. 1.\n\nAccepting the limitations described and interpreting the outcomes of physically based landslide susceptibility models in a relative way. The SFSI as suggested in the present work is one possibility to do so; other ways were introduced earlier with SHALSTAB (Montgomery and Dietrich 1994) or SINMAP (Pack et al. 1998). In principle, all slope stability software tools can be used to derive relative indices from multiple results.\n\n2. 2.\n\nUsing probabilistic approaches to deal with the spatial parameter variation, i.e. resulting in the identification of the possible size of weak regions (Fan et al. 2016). Fibre bundle models may then be used to simulate the associated patterns of slope failures (Cohen et al. 2009). However, this method also relies on various assumptions of spatial parameter variability.\n\nOne may argue that also statistical models—employing a black box in terms of relating predictor layers to a landslide inventory—would do the job of producing relative landslide susceptibility maps. In fact, those approaches may be considered a more honest strategy, compared to physically based calculations with uncertain or even unknown geotechnical and geohydraulic parameters. We have shown that even a simplistic statistical model—employing the local slope as the only predictor layer—performs comparable to the more complex physically based models used. This finding reflects the dominant effect of the slope also in the physically based models, as long as the majority of the other key parameters is assumed constant in space. It reminds of the statement of Box (1976) that it would be simple and evocative models pushing science forward rather than over-elaborated, over-parameterized ones. However, it is clear that statistical models would hardly do the work for dynamic analyses such as—with the data usually available—predicting the slope stability response to a particular rainfall event.\n\n## Conclusions\n\nWe have tested the sensitivity of catchment-scale slope stability model results to variations in the geotechnical and geohydraulic parameters. In contrast to many previous studies, we have focused on parameter spaces instead of combinations of parameter values. The results produced with broad parameter sub-spaces show comparable levels of performance in terms of AUROC to those produced with narrow sub-spaces, even though the results vary considerably in terms of FoC. In general, the SFSI maps are classified as very conservative (FoC > > 1). It seems obsolete to optimize the parameters tested by means of statistical procedures.\n\nConsidering the uncertainty inherent in all geotechnical and geohydraulic data, and the impossibility to capture the spatial distribution of the parameters by means of laboratory tests in sufficient detail, we conclude that landslide susceptibility maps yielded by catchment-scale physically based models should not be interpreted in absolute terms. We suggest that efforts to develop better strategies for dealing with the uncertainties in the spatial variation of the key parameters should be given priority in future slope stability modelling efforts. Even though we consider it likely that many of our results are valid for most types of landslides or geological settings, more tests including a broad spectrum of situations would be necessary to confirm all statements."
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.81445265,"math_prob":0.911602,"size":52960,"snap":"2022-40-2023-06","text_gpt3_token_len":12906,"char_repetition_ratio":0.14731097,"word_repetition_ratio":0.04504617,"special_character_ratio":0.23999244,"punctuation_ratio":0.12641472,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9762082,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-01-27T05:57:54Z\",\"WARC-Record-ID\":\"<urn:uuid:70e63239-f632-49b4-9468-34a1a3fa1471>\",\"Content-Length\":\"329822\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:f56408dd-141b-4b33-b2f5-6d99459354be>\",\"WARC-Concurrent-To\":\"<urn:uuid:e9490c69-b6e2-45de-9b1d-520d886c36a8>\",\"WARC-IP-Address\":\"146.75.32.95\",\"WARC-Target-URI\":\"https://link.springer.com/article/10.1007/s10346-016-0783-6\",\"WARC-Payload-Digest\":\"sha1:K4QTEHA2AJUWJYDENYVOG6N5GHV45G2Y\",\"WARC-Block-Digest\":\"sha1:4LQYT3KZGVZVZSUIWSMERAMA6FMGZ4OI\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-06/CC-MAIN-2023-06_segments_1674764494936.89_warc_CC-MAIN-20230127033656-20230127063656-00428.warc.gz\"}"} |
https://gis.stackexchange.com/questions/169167/geojson-to-spatial-geography-in-sql-server-2012-fix-orientation-of-polygon/169236 | [
"# GeoJson to Spatial Geography in sql server 2012, fix orientation of polygon\n\nI've download from Mapzen many geoJson files related to countries with their respective administration level. Then I've parsed all the geoJson files and saved them to my sql server 2012 as geography spatial data.\n\nI've then done a check of the Luxemburg map and noticed some strange results. Some of the maps where created correctly, with the corresponding inner area:",
null,
"In other cases the area of the selected boundary was the outer:",
null,
"I do know that there is the left-hand convention for storing inner area of a polygon in sql server as spatial data. Clearly fixing each polygon one by one will be a waste of time.\n\nGeoJson files aren't bounded to the left-hand rule, so I need a way to fix the coordinates orientation of the polygon before storing them in the db.\n\nI want the orientation fix logic to be done in the c# code (MVC) not by the sql server.\n\nI've read about a possible solution for convex polygons that handels the issue with cross-product, but still this doesn't work.\n\n1. How can I solve this issue?\n2. Is there a program that fixes the geoJson orientation of the polygons?\n3. Is there an algorithm based on a mathematical principle?\n4. Without going to the fuss of checking the orientation and all the extra coding, is there a site where I can download world data coordinates with all the administrative levels that use the left-hand convention for polygons?\n\nCode used to get cross product\n\n``````public decimal GetCrossProductZDirectionAndLength(VectorCoordinate coordA, VectorCoordinate coordB, VectorCoordinate coordC)\n{\n//***********************************************\n//This method gets the cross product\n//for vectors:\n//BA X BC\n//***********************************************\ndecimal crossProductDirectionLength = 0;\n\n//These vector coordinates are relative to the origin (0,0,0)\nVectorCoordinate vectorCoordinateBA = new VectorCoordinate();\nVectorCoordinate vectorCoordinateBC = new VectorCoordinate();\n\nvectorCoordinateBA.X = coordA.X - coordB.X;\nvectorCoordinateBA.Y = coordA.Y - coordB.Y;\nvectorCoordinateBA.Z = coordA.Z - coordB.Z;\n\nvectorCoordinateBC.X = coordC.X - coordB.X;\nvectorCoordinateBC.Y = coordC.Y - coordB.Y;\nvectorCoordinateBC.Z = coordC.Z - coordB.Z;\n\ncrossProductDirectionLength = GetDeterminat2x2(vectorCoordinateBA.Y, vectorCoordinateBA.Z, vectorCoordinateBC.Y, vectorCoordinateBC.Z);\ncrossProductDirectionLength += GetDeterminat2x2(vectorCoordinateBA.X, vectorCoordinateBA.Z, vectorCoordinateBC.X, vectorCoordinateBC.Z);\ncrossProductDirectionLength += GetDeterminat2x2(vectorCoordinateBA.X, vectorCoordinateBA.Y, vectorCoordinateBC.X, vectorCoordinateBC.Y);\n\nreturn crossProductDirectionLength;\n}\n\nprivate decimal GetDeterminat2x2(decimal a, decimal b, decimal c, decimal d)\n{\n//get the determinat for a 2x2 matrix\n//|a b|\n//|c d|\n\nreturn (a*d)-(b*c);\n}\n``````\n• Could you expand on the solution you have already tried and what about it did not work? – MaryBeth Nov 5 '15 at 18:00\n• @MaryBeth I've included the code and an answer, please check if it makes sense, I've tested it on a few polygons and it seems to work. – Luther Nov 6 '15 at 2:01\n\n## 2 Answers\n\nI don't have a C# solution but here is how to do it in Java using JTS and GeoTools. But you should be able to recreate it in any language which provides some basic libraries/methods.\n\nThe algorithm comes down to\n\n``````for each polygon do\nif outer ring is counter clockwise then\nreverse outer ring\nfor each inner ring\nreverse it\n``````\n\nso in java\n\n``````while (it.hasNext()) {\nSimpleFeature f = (SimpleFeature) it.next();\nGeometry geom = (Geometry) f.getDefaultGeometry();\nSystem.out.println(geom);\nif (geom instanceof Polygon) {\nf.setDefaultGeometry(fixPolygon((Polygon) geom));\n} else if (geom instanceof MultiPolygon) {\nMultiPolygon multi = (MultiPolygon) geom;\nint numGeometries = multi.getNumGeometries();\nPolygon[] polys = new Polygon[numGeometries];\nfor (int i = 0; i < numGeometries; i++) {\npolys[i] = fixPolygon((Polygon) multi.getGeometryN(i));\n}\nf.setDefaultGeometry(GEOMFAC.createMultiPolygon(polys));\n}\nret.add(f);\n}\n\nprivate Polygon fixPolygon(Polygon geom, boolean cw) {\nLineString ring = geom.getExteriorRing();\nLinearRing extRing;\nif (RobustCGAlgorithms.isCCW(ring.getCoordinates()) == cw) {\nextRing = JTSUtilities.reverseRing((LinearRing) ring);\n} else {\nextRing = (LinearRing) ring;\n}\nPolygon ret;\nint numInteriorRing = geom.getNumInteriorRing();\nif (numInteriorRing > 0) {\nLinearRing[] holes = new LinearRing[numInteriorRing];\nfor (int i = 0; i < numInteriorRing; i++) {\nLineString inner = geom.getInteriorRingN(i);\nif (RobustCGAlgorithms.isCCW(inner.getCoordinates()) != cw) {\nholes[i] = JTSUtilities.reverseRing((LinearRing) inner);\n} else {\nholes[i] = (LinearRing) inner;\n}\n}\nret = GEOMFAC.createPolygon(extRing, holes);\n} else {\nret = GEOMFAC.createPolygon(extRing);\n}\nreturn ret;\n}\n``````\n\nI've tried a possible solution to the convex/concave polygon coordinate orientation, based on the left-hand rule (right-hand if required).\n\nBasically we can find the area of a polygon by adding the areas of the trapezoids defined by the polygons edge and a line corresponding to the min Y value of all the coordinates of the polygon. The min Y line is parallel to the X axis.",
null,
"The area of the trapezoid can be found by applying and rearranging the area formula:\n\narea = [(x2 - x1) * (y2 + y1)] / 2",
null,
"When the program adds up all of the trapezoid areas, the sides on the polygon’s bottom give negative areas because x1 > x2 (this depends on the coordinates orientation). Those areas cancel out the parts of the other trapezoids that lie outside of the polygon. This method gives strange results for self-intersecting polygons.\n\nThe code then loops over the polygon’s segments, calculates the area under each, adds them up, and returns the total.\n\nThe total calculated area is negative if the polygon is oriented clockwise.\n\nClockwise or counter-clockwise check can be easily achieved with this solution.\n\n`````` public class VectorCoordinate\n{\npublic decimal X { get; set; }\npublic decimal Y { get; set; }\n}\n\npublic class VectorHelper\n{\npublic decimal GetAreaOfPolygon(List<VectorCoordinate> listPolygonCoordinate)\n{\ndecimal minYcoord = GetMinYCoordFromPolygon(listPolygonCoordinate);\n//Get the first coord to check if the last coord is the same\n//Area of the polygon\ndecimal areaOfPolygon = 0;\n//List of corrds to array\nVectorCoordinate[] vectorCoordinate = listPolygonCoordinate.ToArray();\n\nfor (int i = 0; i < vectorCoordinate.Length-1; i++)\n{\nareaOfPolygon += GetAreaOfTrapezoid(vectorCoordinate[i].X, vectorCoordinate[i].Y, vectorCoordinate[i + 1].X, vectorCoordinate[i + 1].Y, minYcoord);\n}\n//posite/negative area result will tell us if the orientation is clockwise or counterclockwise\nreturn areaOfPolygon;\n}\n\nprivate decimal GetMinYCoordFromPolygon(List<VectorCoordinate> listPolygonCoordinate)\n{\ndecimal minYcoord = listPolygonCoordinate.First().Y;\n\nforeach(var polygonCoord in listPolygonCoordinate)\n{\nif (polygonCoord.Y < minYcoord)\nminYcoord = polygonCoord.Y;\n}\n\nreturn minYcoord;\n}\nprivate decimal GetAreaOfTrapezoid(decimal x1, decimal y1, decimal x2, decimal y2, decimal minYcoord)\n{\nreturn ((x2 - x1) * ( (y2-minYcoord) + (y1-minYcoord))) / 2;\n}\n}\n``````"
] | [
null,
"https://i.stack.imgur.com/fXZro.jpg",
null,
"https://i.stack.imgur.com/mxFuc.jpg",
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"https://i.stack.imgur.com/DJQtV.jpg",
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"https://i.stack.imgur.com/djamQ.jpg",
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.71067184,"math_prob":0.966891,"size":2777,"snap":"2019-35-2019-39","text_gpt3_token_len":614,"char_repetition_ratio":0.24269743,"word_repetition_ratio":0.0,"special_character_ratio":0.23190494,"punctuation_ratio":0.17062636,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9957971,"pos_list":[0,1,2,3,4,5,6,7,8],"im_url_duplicate_count":[null,4,null,4,null,4,null,4,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-08-20T16:15:02Z\",\"WARC-Record-ID\":\"<urn:uuid:c48205eb-1bb4-4236-93e7-f5ea5d1a1bd0>\",\"Content-Length\":\"146832\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:451c8399-e83f-4fb5-a1bf-6885c992da1d>\",\"WARC-Concurrent-To\":\"<urn:uuid:3f57058a-a105-4102-a935-bf210dafc63e>\",\"WARC-IP-Address\":\"151.101.1.69\",\"WARC-Target-URI\":\"https://gis.stackexchange.com/questions/169167/geojson-to-spatial-geography-in-sql-server-2012-fix-orientation-of-polygon/169236\",\"WARC-Payload-Digest\":\"sha1:LFAT6Y5JSB3A5S7SW6JMCNFHPRSHBW74\",\"WARC-Block-Digest\":\"sha1:RLNKIUPAP4JCGDZ2RMD3NGKPWI7QF4KZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-35/CC-MAIN-2019-35_segments_1566027315551.61_warc_CC-MAIN-20190820154633-20190820180633-00019.warc.gz\"}"} |
https://retropie.org.uk/forum/topic/23712/dreamcast-and-ps3-controllers-not-working/ | [
"# Dreamcast and PS3 controllers not working\n\n• Good Evening Gamers,\n\nI am having issues using my PS3 controllers with Dreamcast. These controllers work with all of my other systems but Dreamcast. I tried manually mapping and I still get nothing when I hit start to play a game. I am working with with Retropie 4.5.1 on a Raspberry pi 3 B+. Below you will find my mapping.\n\nManual Configuration\ninput_device = \"MY-POWER CO.,LTD. 2In1 USB Joystick\"\ninput_driver = \"udev\"\ninput_r_y_plus_axis = \"+3\"\ninput_r_x_minus_axis = \"-2\"\ninput_l_btn = \"4\"\ninput_start_btn = \"9\"\ninput_exit_emulator_btn = \"9\"\ninput_r_y_minus_axis = \"-3\"\ninput_down_btn = \"h0down\"\ninput_l_x_plus_axis = \"+0\"\ninput_r_btn = \"5\"\ninput_save_state_btn = \"5\"\ninput_right_btn = \"h0right\"\ninput_state_slot_increase_btn = \"h0right\"\ninput_select_btn = \"8\"\ninput_left_btn = \"h0left\"\ninput_state_slot_decrease_btn = \"h0left\"\ninput_l2_btn = \"6\"\ninput_l3_btn = \"10\"\ninput_l_y_minus_axis = \"-1\"\ninput_up_btn = \"h0up\"\ninput_a_btn = \"1\"\ninput_b_btn = \"2\"\ninput_reset_btn = \"2\"\ninput_enable_hotkey_btn = \"8\"\ninput_l_y_plus_axis = \"+1\"\ninput_r2_btn = \"7\"\ninput_r3_btn = \"11\"\ninput_x_btn = \"0\"\ninput_l_x_minus_axis = \"-0\"\ninput_y_btn = \"3\"\ninput_r_x_plus_axis = \"+2\"\n\nAutomatic Configuration (Before Manual Configuration)\n\n[emulator]\nmapping_name = MY-POWER CO.,LTD. 2In1 USB Joystick\nbtn_escape = 296\n\n[dreamcast]\nbtn_a = 290\nbtn_b = 289\nbtn_c =\nbtn_d =\nbtn_x = 291\nbtn_y = 288\nbtn_z =\nbtn_start = 297\naxis_x = 0\naxis_y = 1\naxis_trigger_left =\naxis_trigger_right =\n\n[compat]\nbtn_trigger_left = 292\nbtn_trigger_right = 293"
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5543976,"math_prob":0.98783106,"size":2201,"snap":"2019-51-2020-05","text_gpt3_token_len":674,"char_repetition_ratio":0.21438324,"word_repetition_ratio":0.0,"special_character_ratio":0.32848704,"punctuation_ratio":0.06741573,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.995993,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-21T02:44:38Z\",\"WARC-Record-ID\":\"<urn:uuid:f9065cd5-426a-4dea-b742-86adc5b99b36>\",\"Content-Length\":\"47464\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:bd0e22e3-e5c3-4628-93bc-91c9cdb7a3fe>\",\"WARC-Concurrent-To\":\"<urn:uuid:3a85c1ae-45d3-4ce0-95ae-630b5ec73d46>\",\"WARC-IP-Address\":\"93.93.129.253\",\"WARC-Target-URI\":\"https://retropie.org.uk/forum/topic/23712/dreamcast-and-ps3-controllers-not-working/\",\"WARC-Payload-Digest\":\"sha1:J65P3K5KXVVXZ3IEATLOJOKS4MKOAO3J\",\"WARC-Block-Digest\":\"sha1:I45FKA45CTYCMMANAX3ERZFWQJQOH4YL\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250601241.42_warc_CC-MAIN-20200121014531-20200121043531-00193.warc.gz\"}"} |
https://bitcoin.stackexchange.com/questions/37645/procedure-for-calculating-taint | [
"# Procedure for calculating taint?\n\nI'd like to understand taint analysis quantitatively. Blockchain.info offers a service that will calculate taint, but I've found no good explanation for how taint is calculated.\n\nThe best (and only) explanation I've found so far appears in the paper Anonymity of Bitcoin Transactions:",
null,
"The taint analysis works by calculating the percentage of the amount of bitcoins that might origin from another address, thus revealing connections in the transaction graph. In the simplified example in Figure 4, A1 and A3 would have a taint of 75% and A2 a taint of 25%. However, it can only detect direct connections in the graph and does not consider any context information.\n\nThis explanation is confusing. Taint is measured between two pseudonyms (addresses). It's not a property of a particular pseudonym. The paper seems to be missing the part that says the taint scores for A1, A2, and A3 are relative to A4. If so, then the scores make sense.\n\nHowever, it's not clear what would happen for more complex chains of ownership. For example, imagine another pseudonym, A5 that pays A1 5 BTC. What would be the taint score between A5 and A4?\n\nI've seen this, but it doesn't discuss how to compute a taint score between two pseudonyms.\n\nWhat I'd like to see is the outline of a step-by-step procedure for calculating taint, as done by Blockchain.info. If I had to guess, here's how the procedure would look:\n\n1. Find two pseudonyms, S (source) and T (target). Funds flow from S to T.\n2. Using the block chain, find a chain of ownership Ci from each coin controlled by S to T.\n3. For each chain of ownership Ci, find the lowest valued coin transfer mi.\n4. Sum all mi, giving m.\n5. Sum the value of all outputs received through T, giving s.\n6. Taint is defined as m/s.\n\nUsing this procedure would give a taint score of 50% between A5 and A4 (2 / 4).\n\nIs this correct?\n\n• I haven't gotten around to going to the source, but I too find the example confusing. If I had to come up with a metric, I'd measure taint as an attribute of UTXO, not addresses. I.e. 1BTC claimed stolen, therefore 100% tainted getting spent together with 0.5 clean BTC would result in a UTXO with taint of 2/3. – Murch Jun 1 '15 at 0:32\n• Ah sorry, I started reading the paper and realized that it uses taint in a different context than the Bitcoin community usually does. Usually \"taint\" refers to the amount of coins traceable to a known theft, this paper however is using it as a term to measure address correlation. That's why I was confused and will remove the tainted-coins tag in a moment. – Murch Jun 1 '15 at 8:57\n\nI think I have an answer. It's not clear if this is how blockchain.info does it, but I'm not sure it matters, either.\n\nTaint is very similar to the everyday experience of diluting a liquid.\n\nImagine starting with three glasses. One glass contains orange juice. The second contains water. The third is empty.\n\nPouring some or all of the orange juice into the empty glass doesn't dilute it at all. However, pouring a 1:1 mixture of orange juice and water into the empty glass dilutes the orange juice.\n\nWe can define a metric called dilution factor. Dilution factor equals the final volume contained in the formerly empty glass divided by the volume of orange juice added. The dilution factor for a 1:1 mixture is therefore 2 (2 / 1). If no dilution takes place, then the dilution factor is 1. More generally:\n\ndilution factor = V2 / V1 if V2 > V1\n\ndilution factor = 1 if V2 <= V1\n\nWe can add another empty glass and dilute again. For example, we can take half of the diluted orange juice and dilute it with an equal volume of water. This gives a second dilution factor of 2.\n\nThe overall dilution factor equals the cumulative product of the dilution factor at each step. In this case, it is 4 (2 x 2).\n\nNow imagine that monetary value is like a liquid, and an output is like a container. We can do dilution analysis just like we did with orange juice.\n\nIn this case, the dilution factor tells us how diluted the value of an output in a chain of ownership has become relative to a downstream output. Provided that the limits of this metric are clear, it can be useful.\n\nThe liquid being diluted is \"taint\". In this model, \"taint\" would be the multiplicative inverse of dilution factor. A dilution factor of 2 implies a taint of 50% (1/2).\n\nReturning to the question posed above, given this chain of ownership, find the dilution factor between A5 and A4:\n\nA5(5 BTC)->A1(2 BTC)->A3(3 BTC)->A4(4 BTC)\n\nThe dilution factors are, from left to right: 1; 3/2; 4/3. Multiplying them together gives 1 x 3/2 x 4/3, or 2. This is a 50% taint, the same answer as I got above.\n\nHowever, the answer postulated in my original question is wrong in that it doesn't account for serial dilution. Consider this chain of ownership:\n\nA5(1 BTC)->A1(5 BTC)->A3(3 BTC)->A4(4 BTC)\n\nThe serial dilution factor is 5 x 1 x 4/3, or 20/3.\n\nSimply dividing the final value by the minimum value upstream gives a dilution factor between A5 and A4 of 4/1."
] | [
null,
"https://i.stack.imgur.com/gg2KF.jpg",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9609536,"math_prob":0.9023985,"size":1838,"snap":"2020-45-2020-50","text_gpt3_token_len":436,"char_repetition_ratio":0.10632497,"word_repetition_ratio":0.0,"special_character_ratio":0.2328618,"punctuation_ratio":0.123655915,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9726737,"pos_list":[0,1,2],"im_url_duplicate_count":[null,7,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-10-21T22:41:30Z\",\"WARC-Record-ID\":\"<urn:uuid:9210b770-2510-46b3-b53d-714e397f0e9f>\",\"Content-Length\":\"152233\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:17cf7d18-67cf-4943-adcc-724e56e50c24>\",\"WARC-Concurrent-To\":\"<urn:uuid:00d12f94-820c-43ac-bf24-802158258729>\",\"WARC-IP-Address\":\"151.101.65.69\",\"WARC-Target-URI\":\"https://bitcoin.stackexchange.com/questions/37645/procedure-for-calculating-taint\",\"WARC-Payload-Digest\":\"sha1:P7WSJH3XYSHX6QPWBRPD5PYUF5S6FWQY\",\"WARC-Block-Digest\":\"sha1:K6LVYMRVP6FQKJYCXCT4PKMJGFD5OP42\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-45/CC-MAIN-2020-45_segments_1603107878633.8_warc_CC-MAIN-20201021205955-20201021235955-00667.warc.gz\"}"} |
https://polyglotsyntax.com/javascript/statements/ | [
"• # Statements\n\nA condition statement is like a question in programming. It helps the computer decide what to do next. For example, if you go to a store, you might ask the shopkeeper if they have what you want. The shopkeeper will answer yes or no, and that will help you decide what to do next. In programming, the computer can ask itself questions to decide what it should do next.\n\n• ## If Statements\n\n• #### Javascript\n\n##### Example of if statement in javascript.\n``````var x = 1;\n\nif (x > 0) {\nconsole.log('variable x is greater than zero'); // variable x is greater than zero\n}``````\n• ## Else Statements\n\n• #### Javascript\n\n##### Example of else statement in javascript.\n``````var x = 1;\n\nif (x > 0) {\nconsole.log('variable x is greater than zero'); // variable x is greater than zero\n} else {\nconsole.log('else, variable x is zero or less'); // else, variable x is zero or less\n}``````\n• ## Else If Statements\n\n• #### Javascript\n\n##### Example of else if statement in javascript.\n``````var x = 1;\n\nif (x > 0) {\nconsole.log('variable x is greater than zero'); // variable x is greater than zero\n} else if (x == 0) {\nconsole.log('else if, variable x is zero'); // else if, variable x is zero\n}``````\n• ## Switch Statements\n\n• #### Javascript\n\n##### Example of switch statement in javascript.\n``````var x = 1;\n\nvar result = '';\nswitch (x) {\ncase 0:\nresult = 'variable x is integer zero';\nbreak;\ncase 1:\nresult = 'variable x is integer one';\nbreak;\ndefault:\nresult = 'variable x is anything else';\n}\n\nconsole.log(result); // variable x is integer one``````"
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7028872,"math_prob":0.94333434,"size":1478,"snap":"2023-40-2023-50","text_gpt3_token_len":374,"char_repetition_ratio":0.1797829,"word_repetition_ratio":0.32967034,"special_character_ratio":0.30175912,"punctuation_ratio":0.14685315,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9936294,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-12-10T00:04:12Z\",\"WARC-Record-ID\":\"<urn:uuid:7d0b0e09-9eb1-4cee-a46f-20477a63ca3f>\",\"Content-Length\":\"13727\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:0b2c1ef3-3170-472b-825f-c7e9186b55ab>\",\"WARC-Concurrent-To\":\"<urn:uuid:45b85340-6272-4e07-bd75-efabe13c0005>\",\"WARC-IP-Address\":\"108.175.2.227\",\"WARC-Target-URI\":\"https://polyglotsyntax.com/javascript/statements/\",\"WARC-Payload-Digest\":\"sha1:W4N45KN5APARTTAZSHHDGI7RX7S5NVCV\",\"WARC-Block-Digest\":\"sha1:HEHTL3CJMZNNTDVPACGPX2PTQECGZHA5\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-50/CC-MAIN-2023-50_segments_1700679100989.75_warc_CC-MAIN-20231209233632-20231210023632-00836.warc.gz\"}"} |
https://php2golang.com/method/function.uasort.html | [
"## GoLang uasort\n\nrequest it (153)\nGoLang replacement for PHP's uasort [edit | history]\n\nDo you know a GoLang replacement for PHP's uasort? Write it!\n\n## PHP uasort\n\nPHP original manual for uasort [ show | php.net ]\n\n# uasort\n\n(PHP 4, PHP 5, PHP 7)\n\nuasortSort an array with a user-defined comparison function and maintain index association\n\n### Description\n\nbool uasort ( array `&\\$array` , callable `\\$value_compare_func` )\n\nThis function sorts an array such that array indices maintain their correlation with the array elements they are associated with, using a user-defined comparison function.\n\nThis is used mainly when sorting associative arrays where the actual element order is significant.\n\nNote:\n\nIf two members compare as equal, their relative order in the sorted array is undefined.\n\n### Parameters\n\n`array`\n\nThe input array.\n\n`value_compare_func`\n\nSee usort() and uksort() for examples of user-defined comparison functions.\n\n### Return Values\n\nReturns `TRUE` on success or `FALSE` on failure.\n\n### Examples\n\nExample #1 Basic uasort() example\n\n``` <?php// Comparison functionfunction cmp(\\$a, \\$b) { if (\\$a == \\$b) { return 0; } return (\\$a < \\$b) ? -1 : 1;}// Array to be sorted\\$array = array('a' => 4, 'b' => 8, 'c' => -1, 'd' => -9, 'e' => 2, 'f' => 5, 'g' => 3, 'h' => -4);print_r(\\$array);// Sort and print the resulting arrayuasort(\\$array, 'cmp');print_r(\\$array);?> ```\n\nThe above example will output:\n\n```Array\n(\n[a] => 4\n[b] => 8\n[c] => -1\n[d] => -9\n[e] => 2\n[f] => 5\n[g] => 3\n[h] => -4\n)\nArray\n(\n[d] => -9\n[h] => -4\n[c] => -1\n[e] => 2\n[g] => 3\n[a] => 4\n[f] => 5\n[b] => 8\n)\n```"
] | [
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https://answers.everydaycalculation.com/multiply-fractions/98-5-times-5-7 | [
"Solutions by everydaycalculation.com\n\n## Multiply 98/5 with 5/7\n\n1st number: 19 3/5, 2nd number: 5/7\n\nThis multiplication involving fractions can also be rephrased as \"What is 98/5 of 5/7?\"\n\n98/5 × 5/7 is 14/1.\n\n#### Steps for multiplying fractions\n\n1. Simply multiply the numerators and denominators separately:\n2. 98/5 × 5/7 = 98 × 5/5 × 7 = 490/35\n3. After reducing the fraction, the answer is 14/1\n\nMathStep (Works offline)",
null,
"Download our mobile app and learn to work with fractions in your own time:"
] | [
null,
"https://answers.everydaycalculation.com/mathstep-app-icon.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.8050141,"math_prob":0.9802133,"size":457,"snap":"2020-34-2020-40","text_gpt3_token_len":193,"char_repetition_ratio":0.17218544,"word_repetition_ratio":0.0,"special_character_ratio":0.46608314,"punctuation_ratio":0.078947365,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9785622,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-08-04T00:48:47Z\",\"WARC-Record-ID\":\"<urn:uuid:1f542784-6d9d-4ce4-ab5b-2b04c3487dfe>\",\"Content-Length\":\"7549\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:226b1f2d-1048-4a4b-9f9a-35dfead0dfec>\",\"WARC-Concurrent-To\":\"<urn:uuid:8ee8759e-3d60-4d6d-83e3-9b55bd70f0e4>\",\"WARC-IP-Address\":\"96.126.107.130\",\"WARC-Target-URI\":\"https://answers.everydaycalculation.com/multiply-fractions/98-5-times-5-7\",\"WARC-Payload-Digest\":\"sha1:MSYITN6W3PCCJGTCQVYL6V7WKK45GNHV\",\"WARC-Block-Digest\":\"sha1:UF3TPPV4BX4UTULF56NVGXIDAAJ26VX5\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-34/CC-MAIN-2020-34_segments_1596439735836.89_warc_CC-MAIN-20200803224907-20200804014907-00372.warc.gz\"}"} |
https://community.cypress.com/thread/28024 | [
"4 Replies Latest reply on Jul 6, 2010 9:42 AM by robert.seczkowski\n\n# delta sigma instrument. amp\n\nI'm trying to use del sig adc plus 2 pga's as an instrumentation amplifier.(acc to AN60319)\n\nADC datasheet says, GetResult16() returns signed value; GetResult32() (not known?!!!! - I presume unsigned)\n\nIn single input ADC mode, the -Input should be tied to VSS. How it is in differetial mode?\n\nADC normally cannot measure negative values.\n\nWhat is the input range (PGA gain 1; ADC gain 1,differential input,internall vref=1.024V) for PGA+ and PGA- pins?\n\nExample:\n\nPGA+ = 0V; PGA - = 1mV or PGA+=1mV, PGA-=0V,diff mode,vref=1.024V what will be the output counts(res 20bits);?\n\n• ###### 1. Re: delta sigma instrument. amp\n\nIn other words:\n\nCounts = Vd*gain/Vref * 2^(n-1) (an60319 page 2) Vd-differetial voltage= Vpositive - Vnegative, n-resolution\n\nWhat counts will be if Vd < 0,Vd = 0,Vd>0?\n\n• ###### 2. Re: delta sigma instrument. amp\n\nHi Robert,\n\nThe ADC by itself can provide a gain of 32 in the component now. It can provide a maximum gain of 128 in the future version(Beta 5) of PSoC creator. So, just using the ADC will be sufficient for gains less than 128. For gains greater than 128, please refer to the connection shown in this KB\n\nhttp://www.cypress.com/?id=4&rID=40623\n\nLet me know if your design requires more gain or some other necessity prevents the use of this design\n\nRegards,\nPraveen\n\n• ###### 3. Re: delta sigma instrument. amp\n\nIt's not the issue of gain but the ADC output.\n\nI guess ADC Delsig gives always 2's complement outputs\n\nthen if Vref=1.024V,gain 1,res=20bit\n\n(((0V-1mV)*1)/(1.024+1mV))* 2^(20-1)=511 or 523777\n\nVdiff K Inp Range Max counts\n\nNow if\n\nthen if Vref=1.024V,gain 1,res=20bit\n\n(((999mV-1000mV)*1)/(2000mV))* 2^(20-1)=262 or 524026\n\nVdiff K Inp Range Max counts\n\nWhy same difference give different results?\n\nBecause measurement range changes with -Input DC value (acc. to DelSig manual)\n\n• ###### 4. Re: delta sigma instrument. amp\n\n2000mV should be replaced with 2024mV to be honest (-Input +- Vref)\n\nIn other words:\n\nIs there a method to measure voltages around 0 like +- 2mV?\n\nregards\n\nrobert"
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.6843,"math_prob":0.9378424,"size":1778,"snap":"2019-13-2019-22","text_gpt3_token_len":582,"char_repetition_ratio":0.10653889,"word_repetition_ratio":0.072463766,"special_character_ratio":0.32452193,"punctuation_ratio":0.14814815,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9815566,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-03-22T09:13:13Z\",\"WARC-Record-ID\":\"<urn:uuid:79e87862-6aa7-4f49-b194-f888d76e96c7>\",\"Content-Length\":\"100493\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4161ec40-203b-4852-8daa-a79549938a6d>\",\"WARC-Concurrent-To\":\"<urn:uuid:ad3e3795-7c0f-4713-ba4b-4cc746f752fe>\",\"WARC-IP-Address\":\"104.118.182.144\",\"WARC-Target-URI\":\"https://community.cypress.com/thread/28024\",\"WARC-Payload-Digest\":\"sha1:5VFVEA46R5SNCZNR7N444BBSWOC23BAR\",\"WARC-Block-Digest\":\"sha1:BOOGBN43AHMULSMEGEHHZTFMRAIBLWWB\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-13/CC-MAIN-2019-13_segments_1552912202640.37_warc_CC-MAIN-20190322074800-20190322100800-00379.warc.gz\"}"} |
https://theswiftarchitect.com/2018/01/16/using-the-map-function-on-an-optional-in-swift/ | [
"# Using the map function on an optional in Swift\n\nHi there Swifters.\n\nToday, I’m going to show you something I learned only quite recently about Swift. In Swift you can use the map function on an optional.",
null,
"At this point I must insert a simple check, if you say:\n\n• ‘Big deal, I don’t care, I don’t use these fancy new tricks everyone seems to promote lately’ or\n• ‘I actually wrote the method’ or\n• something similar\n\nthen you can simply stop reading this post.\n\nIf you’ve heard about the map function, you probably have seen something like this as an explanation. This is using of the map function on an array.\n\n```let array = [1, 2, 3]\nlet mappedArray = array.map { \\$0 * \\$0 }\nprint(mappedArray)\n```\n\nIn this specific example we declare an array: array containing the integers 1, 2 and 3. Then we declare another array: mappedArray which is derived from array by specifying that each element in mappedArray should be calculated by multiplying the element at the same position in the array array by itself. A more in-depth explanation on how to use the map function on an array is out of this post’s scope so if you want to learn more about it I am recommending you checkout Apple’s official documentation about it.\n\nFor me, this usage of map was the only one I knew till I watched the videos of the presentations Using Monads and Other Functional Paradigms in Practice by Raheel Ahmad and Map and FlatMap Magic by Neem Serra. I highly recommend watching them both since they explain how you can use the map function on optionals but also many many more cool stuff.\n\n### Back on the topic…\n\nLet’s analyze a simple use case that comes up pretty often when I write my code and I’ve also seen it a lot in other Swift code from the world. Let’s assume we have a value of an optional integer type. We want to somehow execute an algorithm which will take that value of an optional integer type, do something with it and return a value of an optional integer type. That ‘do something’ part should be: if the optional integer is not nil (has some value) then return that value multiplied by itself; if the optional integer is nil then return nil as well.\n\nPlease, take a look at the following code section (nothing scary here)…\n\n```func transformWithIfLet(number: Int?) -> Int? {\nif let number = number {\nreturn number * number\n}\n\nreturn nil\n}<span id=\"mce_SELREST_start\" style=\"overflow:hidden;line-height:0;\"></span>\n\nfunc transformWithMap(number: Int?) -> Int? {\nreturn number.map { \\$0 * \\$0 }\n}\n\nfunc executeTests() -><span id=\"mce_SELREST_start\" style=\"overflow:hidden;line-height:0;\"></span> Bool {\nlet inputNumbers: [Int?] = [nil, 3]\n\nfor inputNumber in inputNumbers {\nif transformWithIfLet(number: inputNumber) !=\ntransformWithMap(number: inputNumber) {\nreturn false\n}\n}\n\nreturn true\n}\n\nprint(executeTests() ? \"Tests passed\" : \"Tests failed\")\n```\n\nThe transformWithIfLet(number: Int?) -> Int? function is a modularized version of the algorithm implemented in a way that the code maps the worded explanation mostly word for word. The transformWithMap(number: Int?) -> Int? implements the same requirement by using the map function on the number value of optional integer type. When the executeTests() function is executed, the ‘Tests passed’ string is printed out assuring us that these two implementation of the same algorithm return the same values for the same inputs.\n\nThat’s basically how you use the map function on an optional. You define a closure which takes one argument of the same type only not optional (e.g. if you use it on Int?, the argument is of type Int). The closure should return a value of the same type as the closure input argument’s type. That closure will be executed only if the value of the optional is not nil, otherwise nil is returned immediately. Neat, simple and cute syntax!\n\nStill, you might say ‘Great, I traded 5 lines for 1 at the cost of having to use a bit of slightly unorthodox syntax. I don’t see I get much benefit here’. This is the point where we need to go deeper to a more complex use case. If we modify the algorithm to add two more steps in the transformation after the multiplication when the optional value is not nil: converting the integer to a float and then converting it to a string, this is the code we’d get for the two versions of the implementation:\n\n```func transformWithIfLet(number: Int?) -> String? {\nif let number = number {\nreturn String(Float(number * number))\n}\n\nreturn nil\n}\n\nfunc transformWithMap(number: Int?) -> String? {\nreturn number.map { \\$0 * \\$0 }.map(Float.init).map(String.init)\n}\n```\n\nIn my opinion the implementation of transformWithMap(number: Int?) -> String? is a lot more intuitively understandable than the implementation of transformWithIfLet(number: Int?) -> String?. The actual chain of transformation is more evident and the code representation matches the mental representation a lot more closely.\n\nSo, there you go, you just leaned how to use a short and quick trick from the functional programming repertoire, at your disposal 24/7. If you learned something new from this post, please spread the message to your programming buddies by sharing it. Happy optional mapping! 🙂"
] | [
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"https://theswiftarchitect.files.wordpress.com/2018/01/using-the-map-function-on-an-optional-in-swift.jpg",
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https://faculty.math.illinois.edu/Macaulay2/doc/Macaulay2-1.17/share/doc/Macaulay2/GraphicalModels/html/_gaussian__Ring.html | [
"# gaussianRing -- ring of Gaussian correlations on n random variables or a graphical model\n\n## Synopsis\n\n• Usage:\ngaussianRing n\ngaussianRing G\n• Inputs:\n• n, an integer, the number of random variables\n• G, an instance of the type Graph, or an instance of the type Digraph, or an instance of the type Bigraph, or an instance of the type MixedGraph\n• Optional inputs:\n• Coefficients => ..., default value QQ, optional input to choose the base field in markovRing or gaussianRing\n• kVariableName => ..., default value k, symbol used for indeterminates in a ring of Gaussian joint probability distributions\n• lVariableName => ..., default value l, symbol used for indeterminates in a ring of Gaussian joint probability distributions\n• pVariableName => ..., default value p, symbol used for indeterminates in a ring of Gaussian joint probability distributions\n• sVariableName => ..., default value s, symbol used for indeterminates in a ring of Gaussian joint probability distributions\n• Outputs:\n• a ring, a polynomial ring with indeterminates associated to the graphical model\n\n## Description\n\nThis function creates a ring whose indeterminates are the covariances of an n dimensional Gaussian random vector. Using a graph, digraph, or mixed graph $G$ as input gives a gaussianRing with extra indeterminates related to the parametrization of the graphical model associated to that graph. Check the details of the gaussianRing for each type of input:\n\nThe indeterminates of the ring - $s_{(i,j)},k_{(i,j)},l_{(i,j)},p_{(i,j)}$ - can be placed into an appropriate matrix format using the functions covarianceMatrix, undirectedEdgesMatrix, directedEdgesMatrix, and bidirectedEdgesMatrix respectively.\n\nThe variable names that appear can be changed using the options sVariableName, lVariableName, pVariableName, and kVariableName\n\n i1 : G = mixedGraph(digraph {{b,{c,d}},{c,{d}}},bigraph {{a,d}}) o1 = MixedGraph{Bigraph => Bigraph{a => {d}} } d => {a} Digraph => Digraph{b => {c, d}} c => {d} d => {} Graph => Graph{} o1 : MixedGraph i2 : R = gaussianRing (G,pVariableName => psi) o2 = R o2 : PolynomialRing i3 : gens R o3 = {l , l , l , psi , psi , psi , psi , psi , s , s , b,c b,d c,d a,a b,b c,c d,d a,d a,a a,b ------------------------------------------------------------------------ s , s , s , s , s , s , s , s } a,c a,d b,b b,c b,d c,c c,d d,d o3 : List\n\nThe routines conditionalIndependenceIdeal, trekIdeal, covarianceMatrix, undirectedEdgesMatrix, directedEdgesMatrix, bidirectedEdgesMatrix, gaussianVanishingIdeal and gaussianParametrization require that the ring be created by this function.\n\n## For the programmer\n\nThe object gaussianRing is ."
] | [
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https://www.realcode4you.com/post/hierarchical-clustering-principal-component-analysis-using-r-programming | [
"top of page\nSearch\n\n# Hierarchical Clustering & Principal Component Analysis Using R Programming",
null,
"Hierarchical Clustering:\n\nThe dataset on American College and University Rankings contains information on 1302 American colleges and universities offering an undergraduate program. For each university, there are 17 continuous measurements (such as tuition and graduation rate) and 2 categorical measurements (such as location by state and whether it is a private or public school). Note that many records are missing some measurements. Our first goal is to estimate these missing values from “similar” records. This will be done by clustering the complete records and then finding the closest cluster for each of the partial records. The missing values will be imputed from the information in that cluster.\n\n• Remove all records with missing measurements from the dataset.\n\n• For all the continuous measurements, run hierarchical clustering using complete linkage and Euclidean distance. Make sure to normalize the measurements. From the dendrogram, how many clusters seem reasonable for describing these data?\n\n• Compare the summary statistics for each cluster and describe each cluster in this context (e.g., “Universities with high tuition, low acceptance rate…”).\n\n• Use the categorical measurements that were not used in the analysis (State and Private/Public) to characterize the different clusters. Is there any relationship between the clusters and the categorical information?\n\n• What other external information can explain the contents of some or all of these clusters?\n\n• Consider Tufts University, which is missing some information. Compute the Euclidean distance of this record from each of the clusters that you found above (using only the measurements that you have). Which cluster is it closest to? Impute the missing values for Tufts by taking the average of the cluster on those measurements.\n\nPrincipal Component Analysis:\n\nThe file ToyotaCorolla.csv contains data on used cars (Toyota Corollas) on sale during late summer of 2004 in the Netherlands. It has 1436 records containing details on 38 attributes, including Price, Age, Kilometers, HP, and other specifications. The goal will be to predict the price of a used Toyota Corolla based on its specifications.\n\n• Identify the categorical variables.\n\n• Explain the relationship between a categorical variable and the series of binary dummy variables derived from it.\n\n• How many dummy binary variables are required to capture the information in a categorical variable with N categories?\n\n• Use R to convert the categorical variables in this dataset into dummy variables, and explain in words, for one record, the values in the derived binary dummies.\n\n• Use R to produce a correlation matrix and matrix plot. Comment on the relationships among variables.\n\nConsider the 3-means algorithm on a set S consisting of the following 6 points in the plane: a= (0,0), b = (8,0), c=(16,0), d=(0,6), e=(8,6), f=(16,6). The algorithm uses the Euclidean distance metric to assign each point to its nearest centroid; ties are broken in favor of the centroid to the left/down. A starting configuration is a subset of 3 starting points from S that form the initial centroids. A 3- partition is a partition of S into 3 subsets; thus {a,b,e}, {c,d}, {f} is a 3-partition; clearly any 3- partition induces a set of three centroids in the natural manner. A 3-partition is stable if repetition of the 3-means iteration with the induced centroids leaves it unchanged.\n\n• How many starting configurations are there?\n\n• What are the stable 3-partitions?\n\n• What is the number of starting configurations leading to each of the stable 3-partitions in (b) above?\n\n• What is the maximum number of iterations from any starting configuration to its stable 3-partition?\n\nImplementation\n\n```mydata <- read.csv(\"Universities.csv\") # read csv file\nmydata\n\n```\n\n#-------Q---1.a---removing missing values----------------------------------------------------------------------------\n\n```mydata_clean <- na.omit(mydata)\n\nlibrary(dplyr)\n\n# print no. of rows and columns in the dataframe\nprint(paste(\"No. of rows:\", nrow(mydata_clean)))\nprint(paste(\"No. of cols:\", ncol(mydata_clean)))```\n\n#------Q---1.b---Heirarchical_Clustering-----------------------------------------------------------------------------\n\n#---------separating continuous and categorical data-----------------------------------------------------------------\n\n#--------------Categorical_data-------------------------------------------------------\n\n```categorical_variables <- names(select(mydata_clean,\"State\",\"Public..1...Private..2.\"))\nprint(categorical_variables)```\n\n#--------------Numerical_data---------------------------------------------------------\n\n```continuous_variables <- setdiff(names(which(sapply(mydata_clean, is.numeric))),(\"Public..1...Private..2.\"))\nprint(continuous_variables)```\n\n#--------------Normalise_data---------------------------------------------------------\n\n`mydata_normalised <- as.data.frame(scale(mydata_clean[,continuous_variables]))`\n\n#--------------dist_method------------------------------------------------------------\n\n`dist_mat <- dist(mydata_normalised, method = 'euclidean')`\n\n#---------------clustering------------------------------------------------------------\n\n`hcluster <- hclust(dist_mat, method = \"complete\")`\n```# plot the dendogram\nplot(hcluster,cex=0.6)\nabline(h = 12, col = 'red')\n\n# from the dendogram we select 6 clusters\n# draw dendogram with red borders around the 6 clusters\nrect.hclust(hcluster, k=6, border=\"green\")\n\n# coloring the dendogram branches according to cluster\nsuppressPackageStartupMessages(library(dendextend))\ndend_obj <- as.dendrogram(hcluster)\ncol_dend <- color_branches(dend_obj, h= 12)\nplot(col_dend)\n\n# getting clusters\nsub_grp <- cutree(hcluster, k = 6)\n# cluster count\ntable(sub_grp)\n\n# Adding the clusters to the table in a column named \"class\"\nmydata_clean['class']<-as.factor(sub_grp)\n\n# grouping the continuous data by 'class' and taking mean (cluster centers)\ncluster_table<-aggregate(mydata_clean[continuous_variables],by=mydata_clean['class'],mean)\nsummary(cluster_table)```\n\n#-------Q---1.c------------------------------------------------------------------------------------------------------\n\n```# In this case there are three major clusters i.e. cluster 1, 2 and 3 and three outliers as cluster i.e. cluster 4, 5\n# and 6. We will\n\n# cluster 1: Universities with low tution (both in_state and out_state) and high acceptance rate.\n\n# cluster 2: Universities with high tution (both in_state and out_state) and low acceptance rate.\n\n# cluster 3: Universities with low in_state tution and high out_state tution and high acceptance rate.```\n\n#-------Q---1.d------------------------------------------------------------------------------------------------------\n\n```# grouping the categorical data by class\ncat_cluster_table<- group_by(mydata_clean[categorical_variables],by=mydata_clean['class'])\nsummary(cat_cluster_table)\n\n# cluster 1\ntable(mydata_clean\\$Public..1...Private..2.[mydata_clean\\$class == 1])\nprint(\"Cluster 1 has a comparable number of Private and Public colleges\")\n\n# cluster 2\ntable(mydata_clean\\$Public..1...Private..2.[mydata_clean\\$class == 2])\nprint(\"Cluster 2 has a majority of Private colleges\")\n\n# cluster 3\ntable(mydata_clean\\$Public..1...Private..2.[mydata_clean\\$class == 3])\nprint(\"Cluster 3 has a majority of Public colleges\")\n\n# all in all, the three clusters have an ample number of Private colleges than Public due to the fact that the\n# dataset has more private colleges as compared to public ones.\n\n# We can infer from cluster 2 that Private colleges has higher tution fees.```\n\n#-------Q---1.e------------------------------------------------------------------------------------------------------\n\n```# Out of the three major clusters, Cluster3 has most number of Full Time undergrads and cluster2 has the least number\n\n# There is a similar trend for Part Time undergrads as that of FUll Time undergrads.\n# We can say that the more students choose Public colleges over Private colleges\n\n# add fees is higher in the cluster3 (majority Public colleges) as compared to the clusters having higher number of\n# private colleges.\n\n# graduation rate is the highest for cluster2 i.e. Universities with high tution (both in_state and out_state) and\n# low acceptance rate.\n\n# no. of new students from top 10 and top 25 is highest for cluster2 i.e. Universities with high tution\n# (both in_state and out_state) and low acceptance rate.```\n\n#-------Q---1.f---Centroid_Comparison--------------------------------------------------------------------------------\n\n```# preapring the data point for comparison\npoint_new <- mydata[mydata['College.Name']=='Tufts University']\npoint_new[is.na(point_new)] <- 0\npoint_new<- as.integer(point_new[-c(1:3)])\n\n# fucntion to calculate the Euclidean Distance\nEuclidean_Distance<-function(x1, x2) sqrt(sum((x1 - x2) ^ 2))\n\n# calculating Euclidean distance of data from each cluster\nfor (i in 1:nrow(cluster_table)){\npoint <- cluster_table[i,][-1]\nprint(paste('Distance from cluster',i,'is', Euclidean_Distance(point_new,point) ))\n}\n\n# From the result we can see that the Tufts University data is closer to cluster 2.\n\n# imputing the missing value by cluster average\n\n#--------------------------------------------------------------------------------------------------------------------\n\n#--------------Qusetion_2--------------------------------------------------------------------------------------------\n\n#------Q--2.a---Categorical_columns----------------------------------------------------------------------------------\n\n```# loading the dataset\nglimpse(data_df) # info of the dataset\n\n#check for factor type columns\nis.fact <- sapply(data_df, is.factor)\n#print the categorical column's name\nprint('The categorical columns are:')\nprint( names(data_df[,is.fact]))\n\n# There are a total of three categorical columns including the model name of the car, that column is not a feature\n# column. Thus, there are two categorical variables in \"Fuel_Type\" and \"Color\".```\n\n#------Q--2.b---relationship between a categorical variable and the series of binary dummy variables-----------------\n\n```# A dummy variable is a variable that takes values of 0 and 1, where the values indicate the presence or absence\n# of a category.\n# When a categorical variable has more than two categories, it can be represented by a set of dummy variables,\n# with one variable for each category.\n#\n# For example in this case the categorical variable \"Fuel_Type\" has two categories i.e. \"Diesel\" and \"Petrol\".\n# Thus there will we two dummy columns one for Diesel and one for Petrol. In the dummy column for Diesel the instances\n# that had a Diesel fuel type would have a value of 1 and the all the other values would be 0. The dummy column for\n# Petrol would have values in a similar manner.\n\n```\n\n#-----Q--2.c---No. of dummy variables required-----------------------------------------------------------------------\n\n```# N or N-1 dummy binary variables are required to capture the information in a categorical variable with N categories.\n#\n# In some situations like Linear Regression, use of all N dummies will cause failure because the nth variable contains\n# redundant information and can be expressed as a linear combination of the others.Thus, generally we only need\n# N-1 dummy variables.\n\n```\n\n#-------Q--2.d---Creating_dummies------------------------------------------------------------------------------------\n\n```#install.packages(\"dummies\")\nlibrary(\"dummies\")\n\ndata_df['Model'] = as.character(data_df['Model'])\ndata_dummy=dummy.data.frame(data_df,dummy.class=\"factor\")\n\ndata_dummy=data_dummy[,!colnames(data_dummy) %in% \"Fuel_TypeCNG\"]\ndata_dummy=data_dummy[,!colnames(data_dummy) %in% \"ColorBeige\"]\nas.array(names(data_dummy))\n\n#\n# We will talk about the dummy variable Fuel_Type_Diesel.\n# The Values in dummy variables are as follows:\n#\n# 1 : if the instance or the row had Fuel_Type = \"Diesel\"\n# 0 : if the instance had Fuel_Type = \"Petrol\"```\n\n#------Q---2.e---Correlation_matrix----------------------------------------------------------------------------------\n\n```# Correlation matrix\ndata_corr <- subset(data_df, select = -c(Model, Fuel_Type, Color,Cylinders))\ncor_matrix=cor(data_corr)\ndata.frame(cor_matrix)\n\n# matrix plot\nheatmap(cor_matrix, Rowv= NA, Colv= NA)\n\n#library(GGally)\n#library(ggplot2)\n#library(corrplot)\n#library(gplots)\n#ggcorr(data_corr, hjust = 0.75, color = \"grey40\", mid = \"#FFFF66\", name=\"Correlation Plot\")\n\n# Age_month is negatively correlated with price (-0.88): This means when the age of the car is more the price of\n# the car goes down.\n#\n# KM is negatively correlated with price(-0.57): When the km increases similar to age the price of the car\n# decreases.\n#\n# Weight is positively correlated with price(0.58): Weight of the Car is positively correlated with the Price\n# (higher price higher weight)\n#\n# KM is positively correlated with Age_month( 0.51): Other than price, KM and Age of Car is positively stating an\n# increasing relationship for both the factors when one increases.\n#\n# Weight is positively correlated with quarterly tax(0.63) : Quarterly Road Tax collected is positively related to\n# Weight stating higher Car weight higher the Quarterly road tax.\n#\n# Radio and Radio Cassette has a high correlation (0.99): It sugggests that a car having a radio would surely"
] | [
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https://sonichours.com/how-are-the-decimals-0-009-and-0-09-related/ | [
"General\n\n# How Are The Decimals 0.009 And 0.09 Related\n\nThere is no relationship between the decimals 0.009 and 0.09. However, the two numbers have similar amounts of ones. Therefore, the first number is the larger number. The second number has more tenths than the first. Both numbers have the same amount of decimals. So, they are related to each other. In this article, we will explain how the two numbers are related to each other.\n\nThe decimal 0.009 is one hundredth of a whole number. It is always written with the numerator equal to 100, or a hundredth of a whole number. The word “percent” comes from the Latin “per centum,” which means “by the hundred.” So, 0.09 is 100 times smaller than 0.009. Hence, 0.009 is one-hundredth of a millionth.\n\nThe decimal 0.009 is a tenth of one thousandth of a thousandth. Moreover, it is a fraction with a numerator of one and a denominator of one hundred. The word “percent” comes from Latin “per centum”, which means “by the hundred.” The word “percent” is an extension of the term “percent.”\n\nAs you can see, 0.09 is ten times bigger than 0.009. As a result, the two decimals are related to each other by a factor of 10. Using a number line, a student can compare 0.015 to 0.6, a tenth of a hundredth of a thousandth of a millionth. Then, he or she can compare these two numbers by comparing the numerator values of both decimals.\n\nAs you can see, 0.009 and 0.09 are related to each other by their fractional parts. As a result, a decimal with a fractional part is 10 times greater than a decimal with a numerator of one. When a salesperson is advertising a car for sale, he can count the number of test drivers within the first x days. Similarly, a line of best fit is represented by a straight line.\n\nFor example, a salesperson may want to keep track of the number of test drivers after a certain number of days. The same thing is true for a percentage. A percent is a one hundredth of a given amount. It is a fraction that has a numerator of one and a denominator of one. The term percent is derived from the Latin “per centum”, which means per hundred.\n\nAs a matter of fact, the decimals 0.009 and 0.09 are related in terms of their fractional parts. For example, a cent is one hundredth of a given amount. And a decimal with a fraction of one hundred is a percent. In other words, a percentage is one hundredth of a given amount, but not exactly a cent. It is a fraction with a numerator of one hundred.\n\nThe decimals 0.009 and 0.09 are related because they share the same fractional part. For instance, 0.010 is ten times larger than 0.109. Likewise, 0.9 is a percentage of a certain number. This means that the percentage of a number is 90100. This is the same for the decimals 0.009 and 0.09. If you want to calculate the fraction of a certain amount, you can use a place value table or a number line.\n\nThe decimals 0.009 and 0.09 are similar in that they are smaller than one another. The former is one hundredth of a cent and the latter is a hundredth of a hundredth. But the second is one-tenth of a tenth of a cent. When comparing two numbers, you should remember that the latter is larger than the former.\n\nVisit the rest of the site for more useful articles!"
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https://docs.intersystems.com/latest/csp/documatic/%25CSP.Documatic.cls?LIBRARY=ENSLIB&CLASSNAME=%25iKnow.Matching.DictionaryQAPI | [
"# %iKnow.Matching.DictionaryQAPI\n\nclass %iKnow.Matching.DictionaryQAPI extends %iKnow.Queries.AbstractQAPI\n\nThis is an automatically generated class, offering a functionally equivalent set of methods and queries as %iKnow.Matching.DictionaryAPI, exposed as SqlProc methods.\n\nThis class was generated by : %iKnow.Matching.DictionaryAPI.cls\n\n## Methods\n\nclassmethod CreateDictionary(domainId As %Integer, name As %String(MAXLEN=32767), description As %String(MAXLEN=32767)=\"\", defaultLanguage As %String(MAXLEN=32767)=\"en\", defaultProfileId As %Integer = \"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionary\nCreates a Dictionary and returns its ID.\nclassmethod CreateDictionaryFormat(domainId As %Integer, formatClass As %String(MAXLEN=32767), formatParams As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionaryFormat\nCreates a Dictionary Format instance of the supplied formatClass and returns its ID.\nclassmethod CreateDictionaryItem(domainId As %Integer, dictId As %Integer, name As %String(MAXLEN=32767), ByRef URI As %String(MAXLEN=32767), defaultLanguage As %String(MAXLEN=32767)=\"en\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionaryItem\nCreates a Dictionary Item and returns its ID.\nclassmethod CreateDictionaryItemAndTerm(domainId As %Integer, dictId As %Integer, name As %String(MAXLEN=32767), ByRef URI As %String(MAXLEN=32767), language As %String(MAXLEN=32767)=\"en\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionaryItemAndTerm\nShorthand method for creating a Dictionary Item and Term using the Item's name. Returns the Items ID.\nclassmethod CreateDictionaryTerm(domainId As %Integer, dictItemId As %Integer, string As %String(MAXLEN=32767), language As %String(MAXLEN=32767)=\"en\", Output scText As %String = \"\", isProcessed As %Boolean = 0) as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionaryTerm\n\nCreates a Dictionary Term and returns its ID.\n\nIf isProcessed is 1 (default 0), the term will be marked as processed upon creation and no Dictionary Elements will be created. This parameter is for internal use only and deprecated in 2013.1.\n\nclassmethod CreateDictionaryTermFormat(domainId As %Integer, dictItemId As %Integer, formatClass As %String(MAXLEN=32767), formatParams As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateDictionaryTermFormat\nCreates a Dictionary Term composed of a single Dictionary Format and returns the Terms ID.\nclassmethod CreateRegularExpression(pDomainId As %Integer, pDictItemId As %Integer, pRegularExpression As %String(MAXLEN=32767), pReplace As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_CreateRegularExpression\nShorthand method to create a Dictionary Term composed of a single Dictionary Format of type %iKnow.Matching.Formats.RegularExpression, matching pRegularExpression and optionally producing output by replacing the matched parts of an entity with pReplace.\nclassmethod DropAllDictionaryData(domainId As %Integer) as %Boolean\nProjected as the stored procedure: DictionaryQAPI_DropAllDictionaryData\nDrops all dictionary data, including matching results. This method will fail if there are managed dictionaries in this domain.\nclassmethod DropDictionary(domainId As %Integer, dictId As %Integer) as %Boolean\nProjected as the stored procedure: DictionaryQAPI_DropDictionary\nDeletes a Dictionary and all related items, terms, elements and matches.\nclassmethod DropDictionaryItem(domainId As %Integer, dictItemId As %Integer) as %Boolean\nProjected as the stored procedure: DictionaryQAPI_DropDictionaryItem\nDeletes a Dictionary Item with all related terms, elements and matches.\nclassmethod DropDictionaryTerm(domainId As %Integer, dictTermId As %String(MAXLEN=32767)) as %Boolean\nProjected as the stored procedure: DictionaryQAPI_DropDictionaryTerm\nDrops a single Dictionary Term and its matching results\nclassmethod GetDictionaryCount(pDomainId As %Integer, Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetDictionaryCount\nclassmethod GetDictionaryId(domainId As %Integer, name As %String(MAXLEN=32767), Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetDictionaryId\nLooks up the Dictionary ID corresponding to the supplied Dictionary name.\nclassmethod GetDictionaryItemIdByURI(domainId As %Integer, URI As %String(MAXLEN=32767), Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetDictionaryItemIdByURI\nLooks up the Dictionary Item ID corresponding to the supplied Dictionary Item URI.\nclassmethod GetItemCount(pDomainId As %Integer, pDictIds As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetItemCount\nclassmethod GetTermCount(pDomainId As %Integer, pDictIds As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetTermCount\nclassmethod GetTermCountByItem(pDomainId As %Integer, pDictItemIds As %String(MAXLEN=32767)=\"\", Output scText As %String = \"\") as %Library.Integer\nProjected as the stored procedure: DictionaryQAPI_GetTermCountByItem\nclassmethod HasDictionaries(pDomainId As %Integer) as %Library.Boolean\nProjected as the stored procedure: DictionaryQAPI_HasDictionaries\nReturns whether or not there are any dictionaries in the domain\n\n## Queries\n\nquery GetDictionaries(domainId As %Integer, page As %Integer = 1, pageSize As %Integer = 10, pIncludeCrossDomain As %Boolean = 0)\nSelects dictId As %Integer, name As %String(MAXLEN=32767), description As %String(MAXLEN=32767), defaultLanguage As %String(MAXLEN=32767)\nReturns all Dictionaries in this domain. If pIncludeCrossDomain = 1, any cross-domain dictionaries registered in \"domain 0\" are also included in the result, using a negative value for their ID.\nquery GetDictionaryItems(domainId As %Integer, dictId As %Integer, page As %Integer = 1, pageSize As %Integer = 10)\nSelects dictItemId As %Integer, name As %String(MAXLEN=32767), URI As %String(MAXLEN=32767), defaultLanguage As %String(MAXLEN=32767)\nReturns all Dictionary Items for the given Dictionary ID.\nquery GetDictionaryItemsAndTerms(domainId As %Integer, dictId As %Integer, page As %Integer = 1, pageSize As %Integer = 10)\nSelects dictItemId As %Integer, name As %String(MAXLEN=32767), URI As %String(MAXLEN=32767), dictTermId As %Integer, string As %String(MAXLEN=32767), language As %String(MAXLEN=32767), isProcessed As %Boolean\nReturns all Dictionary Items and their Terms for the given Dictionary ID.\nquery GetDictionaryTermsByItem(domainId As %Integer, dictItemId As %Integer, page As %Integer = 1, pageSize As %Integer = 10)\nSelects dictTermId As %Integer, string As %String(MAXLEN=32767), language As %String(MAXLEN=32767), isProcessed As %Boolean\nReturns all the Dictionary Terms for the given Dictionary Item ID.\nquery GetItemsByName(pDomainId As %Integer, pString As %String(MAXLEN=32767), pPage As %Integer = 1, pPageSize As %Integer = 10, pFilter As %String(MAXLEN=32767)=\"\", pDictIds As %String(MAXLEN=32767)=\"\", pMode As %Integer = \\$\\$\\$USEPARTS, pCheck As %String(VALUELIST=\"NAME,URI\")=\"NAME\", pLang As %String(MAXLEN=32767)=\"en\")\nSelects dictId As %Integer, dictName As %String(MAXLEN=32767), itemId As %Integer, itemName As %String(MAXLEN=32767), URI As %String(MAXLEN=32767), language As %String(MAXLEN=32767)\nNote: pFilter is ignored when looking at cross-domain dictionaries\nquery GetTermsByName(pDomainId As %Integer, pString As %String(MAXLEN=32767), pPage As %Integer = 1, pPageSize As %Integer = 10, pFilter As %String(MAXLEN=32767)=\"\", pDictIds As %String(MAXLEN=32767)=\"\", pMode As %Integer = \\$\\$\\$USEPARTS, pLang As %String(MAXLEN=32767)=\"en\")\nSelects dictId As %Integer, dictName As %String(MAXLEN=32767), itemId As %Integer, itemName As %String(MAXLEN=32767), URI As %String(MAXLEN=32767), termId As %Integer, term As %String(MAXLEN=32767), language As %String(MAXLEN=32767)\nNote: pFilter is ignored when looking at cross-domain dictionaries\n\n## Inherited Members\n\n### Inherited Methods\n\nFeedbackOpens in a new tab"
] | [
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https://iftekhar.net/blog/how-to-validate-integer-in-php/ | [
"# Validate Integer in PHP\n\nEvery now and then we need to check if the value of a variable is an integer or not. Recently I came across a forum thread where someone is trying to understand why his/her snippet is not giving the appropriate result that he/she is looking for. In other words, if the variable is an integer this function should return TRUE, otherwise it would return FLASE. Here is a scenario for your thoughts.\n\n``````<?php\n\\$userid = \"12345\";\nif (is_int(\\$userid)) {\necho 'its an integer';\n} else {\necho 'its not an integer';\n}\n?>``````\n\nMany user on that forum suggested that he/she should be using is_numeric function that will give him/her the result he/she might be looking for. This is how it worked.\n\n``````<?php\n\\$userid = \"12345\";\nif (is_numeric(\\$userid)) {\necho 'its an integer';\n} else {\necho 'its not an integer';\n}\n?>``````\n\nIndeed, it does work. However, what we need to understand is that when we assign the value of a variable within “”, PHP will consider the value as string, not an integer. One way to make the first snippet to work is to remove the quotation(“”) mark from the variable or declare the variable value to be an integer to begin with (then test it with is_int function). Here is how it works.\n\n``````<?php\n// use it without \"\"\n\\$userid = 12345;\n// or declare the variable type\n\\$userid = (int) \"12345\";\nif (is_int(\\$userid)) {\necho 'its an integer';\n} else {\necho 'its not an integer';\n}\n?>``````\n\nEither way, is_int function should work as it should be. In my personal opinion though, I really don’t think anyone should be using quote to define an integer value. If you have to, go with declaring the variable type. You can also use the following method to test your variable.\n\n``````<?php\n\\$userid = 12345;\nif (filter_var(\\$userid, FILTER_VALIDATE_INT)) {\necho 'its an integer';\n} else {\necho 'its not an integer';\n}\n?>``````\n\nIn this case, it really doesn’t matter if you use the quote or not. It will validate your variable as an integer. I hope you would find this post to be useful.\n\nReferences: is_int, is_numeric, filter_var"
] | [
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https://www.epb.idv.tw/ge-ren-zuo-pin/xue-xi-zhuang-kuang/ren-gong-zhi-hui-xian-dai-fang-fa/qi-ta/jiyinyichuanyansuanfa | [
"基因遺傳演算法\n\nPost date: 2013/1/16 上午 04:28:50\n\n● 局部極大值:局部極大值是一個比它的每個相鄰狀態都高的峰頂,但是比全局最大值要低。爬山法演算法到達局部極大值附近就會被拉向峰頂,然後被卡在局部極大值處而無處可走。圖4.1示意性地表現了這種情況。\n\n● 山脊:圖4.4 顯示了山脊的情況。山脊造成一系列的局部極大值,貪婪演算法處理這種情況是很難的。\n\n● 高原:高原是在狀態空間地形圖上的一塊平坦區域。它可能是一塊平坦的局部極大值,不存在上山的出路,或者是一個山肩,從山肩還有可能取得進展(參見圖4.1)。爬山法搜尋可能會在高原迷路。\n\nhttp://blog.udn.com/puzzlez/4342425\n\n※西洋棋由白棋先行。棋盤右下角(h1)必須為白格。\n\n1.只要沒有棋子擋住,可以直走無限步,也可以斜走無限步。\n\n2.皇后是子力最強的棋子。\n\n◆棋子的走法與吃法\n\n1\n\n1\n\n2\n\n2\n\n2\n\n8\n\nGenetic Algorithm\n\nGenetic Algorithm(基因演算法,又稱遺傳演算法)主要概念是使用自然界上,兩性生殖的演化機制,使用遺傳(inheritance)、選擇(selection)、雜交(crossover)、突變(mutation)、以及『物競天擇、適者生存』的概念,讓優秀的個體會被留下來,繼續繁殖;而相對差的個體將會慢慢被淘汰,直到絕種。此演算法基於優生學的理論基礎,認為相對優秀的基因互相交配才可以產生更為優秀的後代,但是,為了確保後代的多樣性,又加入了突變的機制,不會讓後代最終都趨於一致。一般來說,基因演算法都能夠找到不錯的解。\n\n1. 一個基因序列(genetic representation)用以表示其問題的解\n2. 一個用來評估問題解的適應力函式(fitness function)\n\n1. 進行初始化。\n2. 重複進行選擇>雜交>突變,直到產生一代所需的個體數量時,即完成一次繁殖。\n3. 當終止條件達成時,停止此演算法。\n\n1. 定義基因序列,使用染色體表示此問題的解。\n• 使用8個數字(0~7)來代表這8列上的皇后,每一個數字代表該列的皇后是位於第幾行。\n1. 例如:24751314、41700256。\n1. 定義適應力函式,用來評估此解的好壞。\n• 從第一列皇后開始計算,若不會吃右列的其他皇后,每一個加一分,故最高分為7+6+5+4+3+2+1=28分。\n• 例如:f(41700256)=24、f(12277051)=23、f(24713603)=27、\n1. f(71420635)=28(此為最佳解)\n1. 使用亂數產生N個第一代個體群。\n• 設N=5,則隨機產生5組第一代個體\n• 例如:51341714、16705214、57130241、67501230、14074251。\n\n1. 評估所有群體中的個體適應力。\n2. 根據適應力來選出兩個個體,適應力越高的個體會有較高的機率被選中。\n• 不僅僅只挑出適應力最高的是因為這樣做可能會產生出局部最佳解(Local solution),並不是全域性的最佳解(Global solution)。\n\n• 雜交的方式有很多種,我們使用單點雜交(One-point crossover)的方式。\n1. 隨機選擇一個位置將此兩個基因切成兩段。\n• 51341714和16705214 => 5134 \\ 1714 和 1670 \\ 5214\n2. 進行雜交\n• 51345214 和 16701714\n\n• 突變方式亦有很多種,我們使用單點突變(Single point mutation)的方式。\n• 當微小機率發生時,將此染色體的其中一個基因進行突變。\n• 51345214 -> 51345?14 -> 51345714\n\n1. 進行了特定次數的繁衍。\n2. 出現滿足特定適應力的個體。\n• 例如:解八皇后問題中,若出現適應力為28的個體,即為找到最佳解。\n3. 達到計算耗費的資源限制(例如:計算時間、計算空間等)。\n4. 人為干涉。\n5. 以上兩種或是更多種的組合。\n\n// 染色體長度\n\n#define GEN_LENGTH 8\n\n// 每一代的數量\n\n#define POPULATION_COUNT 50\n\n// 繁衍代數\n\n#define GENERATION_COUNT 10000\n\n// 突變機率\n\n#define MUTATION_RATE 0.1\n\nclass eightQ\n\n{\n\npublic:\n\neightQ();\n\nvoid randQ();\n\nint getScore();\n\nvoid show();\n\nvector<int> sit;\n\n};\n\nint eightQ::getScore()\n\n{\n\nint nScore = 0;\n\nfor (int i = 0; i < GEN_LENGTH; ++i)\n\n{\n\nint iPosX = i;\n\nint iPoxY = sit[i];\n\n//與其他皇后比較\n\nfor (int j = i + 1; j < GEN_LENGTH; ++j)\n\n{\n\n//若不與此皇后同ROW\n\nif (!(iPoxY == sit[j]))\n\n//若不在此皇后右斜上\n\nif (!(iPoxY - iPosX == sit[j] - j))\n\n//若不在此皇后右斜下\n\nif (!(iPosX + iPoxY == sit[j] + j))\n\nnScore++;\n\n}\n\n}\n\nreturn nScore;\n\n}\n\nvoid GA::init()\n\n{\n\neightQ newQ;\n\n// 隨機產生第一代\n\nfor(int i = 0 ; i < POPULATION_COUNT ; ++i)\n\n{\n\nnewQ.randQ();\n\nthisGen.push_back(newQ);\n\n}\n\ntheBest = newQ;\n\n}\n\nvoid GA::reproduction()\n\n{\n\nMomPool.clear();\n\nint nScoreSum = 0;\n\nvector<int> vAccumulate;\n\n// 將此代所有個體的適應力累加\n\nfor(int i = 0 ; i < POPULATION_COUNT ; ++i)\n\n{\n\nnScoreSum += thisGen[i].getScore();\n\nvAccumulate.push_back(nScoreSum);\n\n}\n\n// 依照適應力的比例選擇母親與父親\n\nfor(int i = 0 ; i < POPULATION_COUNT ; ++i)\n\n{\n\nint nRand = rand() % nScoreSum;\n\nfor(int j = 0 ; j < POPULATION_COUNT ; ++j)\n\nif(nRand < vAccumulate[j])\n\n{\n\nbreak;\n\n}\n\nnRand = rand() % nScoreSum;\n\nfor(int j = 0 ; j < POPULATION_COUNT ; ++j)\n\nif(nRand < vAccumulate[j])\n\n{\n\nMomPool.push_back(thisGen[j]);\n\nbreak;\n\n}\n\n}\n\n}\n\nvoid GA::crossover()\n\n{\n\nint nPos;\n\nthisGen.clear();\n\n// 使用單點雜交\n\nfor(int i = 0 ; i < POPULATION_COUNT ; ++i)\n\n{\n\n// 決定雜交位置 3~6\n\nnPos = rand()%4 + 3;\n\neightQ newQ;\n\n// 前面使用爸爸的染色體\n\nfor(int j = 0 ; j < nPos ; ++j)\n\n{\n\n}\n\n// 後面使用媽媽的染色體\n\nfor(int j = nPos ; j < GEN_LENGTH ; ++j)\n\n{\n\nnewQ.sit[j] = MomPool[i].sit[j];\n\n}\n\nthisGen.push_back(newQ);\n\n}\n\n}\n\nvoid GA::mutation()\n\n{\n\n// 每一個染色體判斷要不要突變\n\nfor(int i = 0 ; i < POPULATION_COUNT ; ++i)\n\n{\n\ndouble dRate = (double)(rand() % 10000) / 10000.0f;\n\nif(dRate < MUTATION_RATE)\n\n{\n\n// 決定突變位置\n\nint nPos = MyRand();\n\nthisGen[i].sit[nPos] = MyRand();\n\n}\n\n// 計算是否比最佳解更好\n\nif(thisGen[i].getScore() > theBest.getScore())\n\ntheBest = thisGen[i];\n\n}\n\n}\n\nint main()\n\n{\n\nsrand((unsigned)time(0));\n\nGA ga;\n\nint nCounter = 0;\n\n// 初始化\n\nga.init();\n\ncout << \"基因演算法開始\" << endl;\n\nwhile(nCounter < GENERATION_COUNT)\n\n{\n\nga.reproduction();\n\nga.crossover();\n\nga.mutation();\n\n//ga.show();\n\n++nCounter;\n\n//cout << \"第\" << nCounter << \"代繁殖完成!\" << endl;\n\n// 若最好的個體已經找到,即可結束。\n\nif(ga.theBest.getScore() >= 28)\n\nbreak;\n\n}\n\ncout << \"第\" << nCounter << \"代所有個體如下所示:\" << endl;\n\nga.show();\n\ncout << \"最佳解為\";\n\nga.theBest.show();\n\ncout << \"其分數為\" << ga.theBest.getScore() << endl;\n\nsystem(\"PAUSE\");\n\nreturn 0;\n\n}"
] | [
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https://forum.alphasoftware.com/showthread.php?124018-Calculation-Help&p=746893 | [
"",
null,
"1. ##",
null,
"Calculation Help\n\nHi All,\n\nSimple calculation and have trouble when it is negative number\n\nI have this and\n1. Is there better way to calculate the Balance?\n2. Do I have to change negative to positive number?\n\nCode:\n```'add number\na = 542\nb = -211\t\t'negative number\nc = 186\nd = 374\n\nx = a+b+c+d\t\t'Get total -- ok\n\n'get the balance\n'balance = a - b\t\t'It is wrong result when the number is negative. Unknown negative number or not\n\nif b < 0 then\n'msgbox(\"b is less than 0 and ...\")\n'How to change to positive number?\nbalance = a + b\t\t'Unknown negative number or not\nelse\nbalance = a - b\t\t'Unknown negative number or not\nend if\nui_msg_box(\"result\",\"balance \"+balance)```",
null,
"",
null,
"Reply With Quote\n\n2. ##",
null,
"Re: Calculation Help\n\nif a,b,c,d are transactions, what is the beginning balance?\n\nZero?\n\nWhat do you expect the balance to be?",
null,
"",
null,
"Reply With Quote\n\n3. ##",
null,
"Re: Calculation Help\n\nHi Al,\n\nIt is general subtract calculation, not typical \"Balance\" calculation.\n\nwhat is the beginning balance? -- \"A\" Value\nWhat do you expect the balance to be? --> a(*542) - b(*211) = 331.00\n\nI want to write a code as xBal = a - b but when the \"B\" is negative number then trouble.\n\nThank you",
null,
"",
null,
"Reply With Quote\n\n4. ##",
null,
"Re: Calculation Help",
null,
"Originally Posted by johnkoh",
null,
"Hi Al,\n\nIt is general subtract calculation, not typical \"Balance\" calculation.\n\nwhat is the beginning balance? -- \"A\" Value\nWhat do you expect the balance to be? --> a(*542) - b(*211) = 331.00\n\nI want to write a code as xBal = a - b but when the \"B\" is negative number then trouble.\n\nThank you\na-abs(b)",
null,
"",
null,
"Reply With Quote\n\n5. ##",
null,
"Re: Calculation Help\n\nThanks, Al",
null,
"",
null,
"Reply With Quote\n\n####",
null,
"Posting Permissions\n\n• You may not post new threads\n• You may not post replies\n• You may not post attachments\n• You may not edit your posts\n•"
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https://program-transformation.org/view/Sts/StatementStatisticsUsingTXL.html | [
"Page\n\nWeb\n\nWiki\n\n# Statement Statistics Using TXL\n\nSoftware Transformation Systems\nTXL solution to TIL Chairmarks #4.2: Collecting statement statistics.\n\n-- JamesCordy - 28 Oct 2005\n\nFile \"TILstats.Txl\"\n\n```% Gather statement statistics for a Tiny Imperative Language program\n% Jim Cordy, October 2005\n\n% Gathers and outputs statistics on the number of each kind of statement\n% in a program. Replaces the program itself with an empty one.\n\n% Begin with the TIL base grammar\ninclude \"TIL.Grm\"\n\n% Compute and output statement kind statistics, replace program with an empty one.\n% There are many different ways to do this - this naive way is simple and\n% obvioulsy correct, but exposes TXL's need for generics.\n% Another less clear solution could use polymorphism to avoid the repetition.\n\nfunction main\nreplace [program]\nProgram [program]\n\n% Count each kind of statement we're interested in\n% by extracting all of each kind from the program\n\nconstruct Statements [statement*]\n_ [^ Program]\nconstruct StatementCount [number]\n_ [length Statements] [putp \"Total: %\"]\n\nconstruct Declarations [declaration*]\n_ [^ Program]\nconstruct DeclarationsCount [number]\n_ [length Declarations] [putp \"Declarations: %\"]\n\nconstruct Assignments [assignment_statement*]\n_ [^ Program]\nconstruct AssignmentsCount [number]\n_ [length Assignments] [putp \"Assignments: %\"]\n\nconstruct Ifs [if_statement*]\n_ [^ Program]\nconstruct IfCount [number]\n_ [length Ifs] [putp \"Ifs: %\"]\n\nconstruct Whiles [while_statement*]\n_ [^ Program]\nconstruct WhileCount [number]\n_ [length Whiles] [putp \"Whiles: %\"]\n\nconstruct Fors [for_statement*]\n_ [^ Program]\nconstruct ForCount [number]\n_ [length Fors] [putp \"Fors: %\"]\n\n_ [^ Program]\n\nconstruct Writes [write_statement*]\n_ [^ Program]\nconstruct WriteCount [number]\n_ [length Writes] [putp \"Writes: %\"]\n\nby\n% nothing\nend function\n```\n\nExample run:\n\n```<linux> cat factors.til\n// Factor an input number\nvar n;\nwrite \"The factors of n are\";\nvar f;\nf := 2;\nwhile n != 1 do\nwhile (n / f) * f = n do\nwrite f;\nn := n / f;\nend\nf := f + 1;\nend\n<linux> txl factors.til TILstats.Txl\nTXL v10.4a (15.6.05) (c)1988-2005 Queen's University at Kingston\nCompiling TILstats.Txl ...\nParsing factors.til ...\nTransforming ...\nTotal: 11\nDeclarations: 2\nAssignments: 3\nIfs: 0\nWhiles: 2\nFors: 0"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.74126226,"math_prob":0.8058993,"size":2383,"snap":"2022-27-2022-33","text_gpt3_token_len":673,"char_repetition_ratio":0.18116856,"word_repetition_ratio":0.005509642,"special_character_ratio":0.27864036,"punctuation_ratio":0.15151516,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.97017217,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-06-28T21:26:12Z\",\"WARC-Record-ID\":\"<urn:uuid:6bb89eaf-383c-4b49-b088-5767031d1ae0>\",\"Content-Length\":\"8773\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:8b8e14a2-71ad-4ce6-b9f9-282d1d3ad077>\",\"WARC-Concurrent-To\":\"<urn:uuid:1d49ac3c-aacb-477e-8355-20e85ab60a24>\",\"WARC-IP-Address\":\"131.180.125.32\",\"WARC-Target-URI\":\"https://program-transformation.org/view/Sts/StatementStatisticsUsingTXL.html\",\"WARC-Payload-Digest\":\"sha1:OQ2Z2NN2KKSJS7RNHU4M66R5KNOHZBVN\",\"WARC-Block-Digest\":\"sha1:7I5HY67WG5Y67O52G63GP5Q3CUO5TSDM\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-27/CC-MAIN-2022-27_segments_1656103617931.31_warc_CC-MAIN-20220628203615-20220628233615-00723.warc.gz\"}"} |
http://zhaoxuhui.top/blog/2020/10/14/gee-note2-basic-introduction-and-ndvi-example.html | [
"## Oct 14,2020 10407 words 38 min\n\n#### 2.基本数据类型\n\n``````// 新建一个服务器上的字符串\nvar serverString = ee.String('This is on the server.');\nprint('String on the server:', serverString);\n\n// 新建一个服务器上的数字\nvar serverNumber = ee.Number(3.14159);\nprint('number=',serverNumber);\n\n// 新建一个服务器上的列表\nvar serverList = ee.List([1,5,6,9,2]);\nprint('Sequence:',serverList);\n// 注意,由于是服务器上的List,所以需要通过get()函数获得内容,而不是直接索引\nprint('item 2:',serverList.get(2));\n\n// 新建一个服务器上的字典,包含三个键值对\nvar serverDict = ee.Dictionary({\ne:Math.E,\npi:Math.PI,\nphi:(1+Math.sqrt(5))/2\n});\n// 和上面一样,需要通过get()函数获取数据\nprint('Golden ratio:',serverDict.get('phi'));\nprint('Keys:',serverDict.keys());\n\n// 新建一个服务器上的日期\nvar serverDate = ee.Date('2020-10-13');\nprint('date:',serverDate);\n``````\n\n#### 3.基本语法\n\n##### (1)循环\n\n``````// This generates a list of numbers from 1 to 10.\nvar myList = ee.List.sequence(1, 10);\n\n// The map() operation takes a function that works on each element independently\n// and returns a value. You define a function that can be applied to the input.\nvar computeSquares = function(number) {\n// We define the operation using the EE API.\nreturn ee.Number(number).pow(2);\n};\n\n// Apply your function to each item in the list by using the map() function.\nvar squares = myList.map(computeSquares);\nprint(squares); // [1, 4, 9, 16, 25, 36, 49, 64, 81]\n``````\n##### (2)条件判断\n\n``````// The following function determines if a number is even or odd. The mod(2)\n// function returns 0 if the number is even and 1 if it is odd (the remainder\n// after dividing by 2). The input is multipled by this remainder so even\n// numbers get set to 0 and odd numbers are left unchanged.\nvar getOddNumbers = function(number) {\nnumber = ee.Number(number); // Cast the input to a Number so we can use mod.\nvar remainder = number.mod(2);\nreturn number.multiply(remainder);\n};\n\n// This generates a list of numbers from 1 to 10.\nvar myList = ee.List.sequence(1, 10);\n\n// filtering\nvar newList = myList.map(getOddNumbers);\n\n// Remove the 0 values.\nvar oddNumbers = newList.removeAll();\nprint(oddNumbers);\n``````\n\n``````var collection = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\n// Divide the collection into 2 subsets and apply a different algorithm on them.\nvar subset1 = collection.filter(ee.Filter.lt('SUN_ELEVATION', 40));\nvar subset2 = collection.filter(ee.Filter.gte('SUN_ELEVATION', 40));\n\nvar processed1 = subset1.map(function(image) {\nreturn image.multiply(2);\n});\nvar processed2 = subset2;\n\n// Merge the collections to get a single collection.\nvar final = processed1.merge(processed2);\nprint('Original collection size', collection.size());\nprint('Processed collection size', final.size());\n``````\n\n##### (3)累加\n\n``````var algorithm = function(current, previous) {\nprevious = ee.List(previous);\nvar n1 = ee.Number(previous.get(-1));\nvar n2 = ee.Number(previous.get(-2));\n};\n\n// Compute 10 iterations.\nvar numIteration = ee.List.repeat(1, 10);\nvar start = [0, 1];\nvar sequence = numIteration.iterate(algorithm, start);\nprint(sequence); // [0, 1, 1, 2, 3, 5, 8, 13, 21, 34, 55, 89]\n``````\n\n#### 4.可视化影像与波段\n\n``````// Instantiate an image with the Image constructor.\nvar image = ee.Image('CGIAR/SRTM90_V4');\n\n// Zoom to a location.\nMap.setCenter(117.3798, 32.9049, 4); // Center on the Bengbu City.\n\n// Display the image on the map.\n``````\n\n#### 5.影像集\n\n``````// 获取Landsat8 TOA影像\nvar l8 = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\n// 定义一个目标点\nvar point = ee.Geometry.Point(117.0721,33.2363);\n\n// 调用filterBounds筛选位置\nvar spatialFiltered = l8.filterBounds(point);\nprint('spatialFiltered',spatialFiltered);\n\n// 再调用filterDate筛选时间\nvar temporalFiltered = spatialFiltered.filterDate('2015-01-01','2015-12-31');\nprint('temporalFiltered',temporalFiltered);\n\n// 到这一步之后,还可能有很多影像的,我们可以进一步按照云层覆盖进行排序\nvar sorted = temporalFiltered.sort('CLOUD_COVER');\n// 选取含云量最少的那一景\nvar scene = sorted.first();\n\n// 将影像放到当前地图的中心,缩放9级\nMap.centerObject(scene,9);\n\n// Landsat8的RGB波段分别是B4、B3、B2\n// 最大值设为0.3,最小值默认为0\nvar visParams = {bands:['B4','B3','B2'],max:0.3};\n\n// 展示影像,名称为true-color composite\n``````\n\n#### 6.实例练习-基于Landsat数据计算NDVI\n\n``````// 指定某个目标点\nvar point = ee.Geometry.Point([117.0721,33.2363]);\n\n// 导入Landsat-8 TOA影像数据集\nvar l8 = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\n// 获取2015年云量最少的影像\nvar image = ee.Image(\nl8.filterBounds(point)\n.filterDate('2015-01-01', '2015-12-31')\n.sort('CLOUD_COVER')\n.first()\n);\n\n// 计算Normalized Difference Vegetation Index (NDVI)\n// Landsat8 第5波段是近红外(NIR),第4波段是红波段(Red)\nvar nir = image.select('B5');\nvar red = image.select('B4');\n// 套用NDVI计算公式(NIR-Red)/(NIR+Red)\n\n// 设置影像到地图中心\nMap.centerObject(image,9);\n// 设置最大最小值和显示颜色\nvar ndviParams = {min:-1,max:1,palette:['blue','white','green']};\n// 向地图中添加图层\n``````\n\n``````// 导入Landsat-8 TOA影像数据集\nvar l8 = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\nvar ndvi = image.normalizedDifference(['B5', 'B4']).rename('NDVI');\n};\n\n// 利用GEE的map函数并行计算NDVI\n\n// 我们可用计算好的NDVI找到所有影像中最“绿”的像素\nvar greenest = withNDVI.qualityMosaic('NDVI');\n\n// 展示结果\nvar visParams = {bands: ['B4', 'B3', 'B2'], max: 0.3};\n``````\n\n#### 7.数据导出\n\nGEE虽然是云端处理,但显然是支持数据的导出和下载的,不然运行的结果没法使用。数据的导出主要分为两类,一类是运算的数值类型数据的导出以及绘图,一类是影像的导出。下面分别介绍。\n\n##### (1)数值与绘图\n\n``````// Import the Landsat 8 TOA image collection.\nvar l8 = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\n// Map a function over the Landsat 8 TOA collection to add an NDVI band.\nvar withNDVI = l8.map(function(image) {\n// Get a cloud score in [0, 100].\nvar cloud = ee.Algorithms.Landsat.simpleCloudScore(image).select('cloud');\n\n// Create a mask of cloudy pixels from an arbitrary threshold.\n\n// Compute NDVI.\nvar ndvi = image.normalizedDifference(['B5', 'B4']).rename('NDVI');\n\n// Return the masked image with an NDVI band.\n});\n\n// Define ROI.\nvar roi = ee.Geometry.Polygon([[117.211,32.847],\n[117.464,32.847],\n[117.464,32.995],\n[117.211,32.995],\n[117.211,32.847]]);\n\n// Create a chart.\nvar chart = ui.Chart.image.series({\nimageCollection: withNDVI.select('NDVI'),\nregion: roi,\nreducer: ee.Reducer.first(),\nscale: 30\n}).setOptions({title: 'NDVI over time'});\n\n// Display the chart in the console.\nprint(chart);\nMap.centerObject(roi,11);\n``````\n\n##### (2)保存影像\n\n``````// 指定某个目标点\nvar point = ee.Geometry.Point([117.0721,33.2363]);\n\n// 导入Landsat-8 TOA影像数据集\nvar l8 = ee.ImageCollection('LANDSAT/LC08/C01/T1_TOA');\n\n// 获取2015年云量最少的影像\nvar image = ee.Image(\nl8.filterBounds(point)\n.filterDate('2015-01-01', '2015-12-31')\n.sort('CLOUD_COVER')\n.first()\n);\n\n// 计算Normalized Difference Vegetation Index (NDVI)\n// Landsat8 第5波段是近红外(NIR),第4波段是红波段(Red)\nvar nir = image.select('B5');\nvar red = image.select('B4');\n// 套用NDVI计算公式(NIR-Red)/(NIR+Red)\n\n// 设置影像到地图中心\nMap.centerObject(image,9);\n// 设置最大最小值和显示颜色\nvar ndviParams = {min:-1,max:1,palette:['blue','white','green']};\n// 向地图中添加图层\n\n// 上面的代码都一样\n// 这里,调用Export的toDrive函数导出\nExport.image.toDrive({\nimage: ndvi,\ndescription: 'NDVI',\nscale: 30\n});\n``````",
null,
"运行代码以后,除了会得到之前的结果外,在右上角的“Tasks”里也会看到有新的任务,点击“Run”,弹出如下对话框。",
null,
"填入相关信息,即可开始导出,导出完成后就会在你的Google Drive里看到对应的文件了,下载即可。如下图所示。",
null,
""
] | [
null,
"https://zhaoxuhui.top/assets/images/blog/content/2020-10-14-12.png",
null,
"https://zhaoxuhui.top/assets/images/blog/content/2020-10-14-13.png",
null,
"https://zhaoxuhui.top/assets/images/blog/content/2020-10-14-14.png",
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] | {"ft_lang_label":"__label__zh","ft_lang_prob":0.5606452,"math_prob":0.98422235,"size":11315,"snap":"2023-40-2023-50","text_gpt3_token_len":5608,"char_repetition_ratio":0.106179826,"word_repetition_ratio":0.16030534,"special_character_ratio":0.2771542,"punctuation_ratio":0.24284254,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9834815,"pos_list":[0,1,2,3,4,5,6],"im_url_duplicate_count":[null,3,null,3,null,3,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-12-01T09:40:40Z\",\"WARC-Record-ID\":\"<urn:uuid:1802c6d9-2174-41e5-857b-aacd37162f3d>\",\"Content-Length\":\"71103\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4be45370-cd84-407a-9f52-f72a701842a4>\",\"WARC-Concurrent-To\":\"<urn:uuid:9d22081e-3f64-4cbe-95c6-9acdfd4d0ff3>\",\"WARC-IP-Address\":\"185.199.109.153\",\"WARC-Target-URI\":\"http://zhaoxuhui.top/blog/2020/10/14/gee-note2-basic-introduction-and-ndvi-example.html\",\"WARC-Payload-Digest\":\"sha1:QQFVFCNJDDTFQ5WM4PE7CYGZXQUT5B5S\",\"WARC-Block-Digest\":\"sha1:N5MEWW7EGHSQQPSIGHKR24NMCNDGNS63\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-50/CC-MAIN-2023-50_segments_1700679100286.10_warc_CC-MAIN-20231201084429-20231201114429-00460.warc.gz\"}"} |
https://puzzling.stackexchange.com/questions/42691/determine-which-statements-are-true-and-which-statements-are-false/42692 | [
"# Determine which statements are True, and which statements are False\n\nDetermine which statements are True, and which statements are False\n\n1. There are 3 consecutive False statements\n2. This is The First True Statement\n3. There are equal numbers of True and False statements\n4. There are not equal numbers of True and False statements\n5. There are 4 consecutive False statements\n6. The First and Last statements are False\n7. There are 3 consecutive statements which are False, False, True.\n8. There are 3 consecutive True statements\n9. There are 3 consecutive statements which are True, False, True.\n10. There are 4 consecutive True statements\n\nThis puzzle have more than 1 solution.\n\nThere are five distinct possibilities: FTFTFFTTTT, TFFTFFTFFF, TFTFFFTTTF, FTTFFTTTFF, FTTFFTTFTF.\n\n## Proof\n\nFirst, assume statement 5 is true.\n\nThis implies statement 1 is also true. So the four consecutive false statements cannot be 1,2,3,4; they must be either 6,7,8,9 or 7,8,9,10. So 7,8,9 are all false, which means there can be no sequences of statements of the form FFT or TTT or TFT.\n\nSo the sequence of statements 3,4,5 (ending in a true statement) must be FTT. But now statement 2 is either true or false, so the sequence 2,3,4 must be either TFT or FFT. Contradiction.\n\nSo statement 5 is false.\n\n• Now assume statement 10 is true.\n\nSince statement 5 is false, the four consecutive true statements must be either 1,2,3,4 or 6,7,8,9 or 7,8,9,10. But if statement 2 is true, then statement 1 is false, so 1,2,3,4 cannot all be true. So 7,8,9 are all true. By our assumption, 10 is true and therefore 6 is false. We have FFTTTT for statements 5-10.\n\nAssume statement 1 is true, so that statement 2 is false. Note that exactly one of 3 and 4 is false, since they are opposites. So the three consecutive false statements must be 4,5,6, and the entire sequence is TFTFFFTTTT: six true statements and four false ones, making statement 3 false. Contradiction.\n\nSo statement 1 is false, and there are no three consecutive false statements. Since 5 and 6 are false, this means 4 must be true, so 3 is false and 2 is true. Now the entire sequence is FTFTFFTTTT. There are no contradictions here, so this is a possible answer.\n\nLet's see if there are any others: i.e. let's assume statement 10 is false.\n\n• Assume statement 1 is true.\n\nThis implies statements 2 and 6 are both false. Note also that exactly one of 3 and 4 is false.\n\nIf 7 is false, then the sequence of false statements starting with 5,6,7 must continue until the end, so 8,9,10 are all false too, which means statement 5 is true, contradiction. So 7 is true, and we have TF??FFT??F.\n\n• If 9 is false, then 3 must be false (otherwise 1,2,3 would be TFT), so 4 is true, and 8 is false since there are no three consecutive true statements. This gives the entire sequence TFFTFFTFFF, which is another viable possibility.\n\n• If 9 is true, then the only way to get the three consecutive false statements required by 1 is if they are 4,5,6, so 4 is false and 3 is true. To make the counts of true and false statements agree, 8 must also be true, so we have TFTFFFTTTF, which is another viable possibility.\n\n• Finally, assume statement 1 is false.\n\nNow 6 is true, so we have F???FT???F, and of course exactly one of 3 and 4 is true.\n\n• If 8 is true, then 6,7,8 must be the three consecutive true statements and 9 must be false (since we can't have four consecutive true statements). To avoid having a sequence TFT, 4 must be false, thus 3 is true, and then 2 must be true. So the entire sequence is FTTFFTTTFF, which is another viable possibility.\n\n• If 8 is false, then 9 must be true (otherwise 8,9,10 would be three consecutive false statements), so we have F???FT?FTF. If 7 were false, then the sequence 7,8,9 would be FFT; contradiction, so 7 is true. Now if 3 were false and 4 true, then the FFT sequence required by 7 must be 2,3,4, so 1,2,3 are three consecutive false statements, contradiction. So 3 is true and 4 false, and then 2 must be true to make the counts of true and false statements match. Thus the entire sequence is FTTFFTTFTF, another viable possibility.\n\n• The existence of 5 distinct answers shows that whatever clever things you will do, in the end, you will left with these 5 distinct cases. To handle this task alone (deal with the 5 cases) is complicated, so in essence, you are repeating the utterly boring, and automatic reasoning of a computer. You are not going to find any nice answers, because there are none: in part, because the question itself was poorly designed. – Matsmath Sep 17 '16 at 15:01\n• @Matsmath Finished! :-) – Rand al'Thor Sep 17 '16 at 15:07\n\nThis puzzle has surprisingly\n\nfive solutions: {{0, 1, 0, 1, 0, 0, 1, 1, 1, 1}, {0, 1, 1, 0, 0, 1, 1, 0, 1, 0}, {0, 1, 1, 0, 0, 1, 1, 1, 0, 0}, {1, 0, 0, 1, 0, 0, 1, 0, 0, 0}, {1, 0, 1, 0, 0, 0, 1, 1, 1, 0}}.\n\nThere are no other solutions. Thanks @rand al'thor for pointing out a bug in how I selected 3-subsets.\n\nWhat happens is, that each of the 10 statements S1, S2, ..., S10, can be evaluated independently for any given 10-tuples. So, for example S1(1,1,1,1,1,1,1,1,1,1)=0, because in the 10-tuple {1,1,1,1,1,1,1,1,1,1} there are NO three consecutive 0s. The task is then to solve the equation [S1(x),S2(x),...S10(x)]=x which you can do by exhaustively going through all 1024 10-tuples. In essence, you are looking for a fixpoint of the vector-valued function F(x):=[S1(x),S2(x),...,S10(x)].\n\n• FTFTFFTTTT also works. – Rand al'Thor Sep 17 '16 at 14:33\n• Yes, thanks for pointing out. I was unable to correctly specify what is a 3-consecutive subset (I missed out {5,6,7} and {6,7,8}, or alike). – Matsmath Sep 17 '16 at 14:41\n• Ok. I have not checked if this puzzle have multiple answer or not. – Jamal Senjaya Sep 17 '16 at 14:44\n\n1. False\n\n2. True\n\n3. False\n\n4. True\n\n5. False\n\n6. True\n\n7. True\n\n8. False\n\n9. True\n\n10. False\n\nOr:\n\nFTFTFFTFTF\n\nExplanation:\n\n7: There are 3 statements which are False, False, True. We could make it 5 as False, 6 as False and 7 as True. On 9, it's True False True. We could make 7 True (already), 8 false and 9 true. This fits in, completely. Now, let's start building up. At 2, it says that statement is true, so let's make that true. (don't remember the rest). I just realized this answer is wrong.\n\nEDIT: I just realized this is wrong.\n\n• you have 3 as false – JMP Sep 17 '16 at 14:25\n• Can you add an explanation? – Beastly Gerbil Sep 17 '16 at 14:27\n• Sorry, but this doesn't work: you claim statement 3 is false, but there are equal numbers of true and false statements in your list. – Rand al'Thor Sep 17 '16 at 14:29"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9348997,"math_prob":0.98576945,"size":600,"snap":"2021-04-2021-17","text_gpt3_token_len":128,"char_repetition_ratio":0.24664429,"word_repetition_ratio":0.25252524,"special_character_ratio":0.21166667,"punctuation_ratio":0.07920792,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98310935,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-01-21T02:38:44Z\",\"WARC-Record-ID\":\"<urn:uuid:6d7ce135-2381-4b41-9ecc-16d96f135c5c>\",\"Content-Length\":\"177797\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:62c7f0e0-0bc4-4b02-a30e-2ae3fb66eb55>\",\"WARC-Concurrent-To\":\"<urn:uuid:ee465590-27d8-4c04-9f53-5b0f0affe74d>\",\"WARC-IP-Address\":\"151.101.129.69\",\"WARC-Target-URI\":\"https://puzzling.stackexchange.com/questions/42691/determine-which-statements-are-true-and-which-statements-are-false/42692\",\"WARC-Payload-Digest\":\"sha1:UE63S4MUDVCEHL4QSXXQWHNLLKBRATCE\",\"WARC-Block-Digest\":\"sha1:TZOF3K6H73SBHM2HM45MQ5DPV7VXCMRY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-04/CC-MAIN-2021-04_segments_1610703522150.18_warc_CC-MAIN-20210121004224-20210121034224-00005.warc.gz\"}"} |
https://info.maitriinfosoft.com/blog/vela-software-pfo/xx1ii.php?76692d=find-all-cliques-in-a-graph | [
"Algorithm to Find All Cliques in a Graph A. Ashok Kumar Department of Computer Science , St. Xavier’s College (Autonomous), Palayamkottai - 627 002. We can find all the 2-cliques by simply enumerating all the edges. If the two subgraphs have k-1 vertices in common and graph contains the missing edge, we can form a k+1-clique. To do this simply step through all subsets of 17 vertices in lexicographical order and check whether they form a clique. acknowledge that you have read and understood our, GATE CS Original Papers and Official Keys, ISRO CS Original Papers and Official Keys, ISRO CS Syllabus for Scientist/Engineer Exam, Maximal Clique Problem | Recursive Solution, Check if a given graph is Bipartite using DFS, Check whether a given graph is Bipartite or not, Printing all solutions in N-Queen Problem, Warnsdorff’s algorithm for Knight’s tour problem, The Knight’s tour problem | Backtracking-1, Count number of ways to reach destination in a Maze, Count all possible paths from top left to bottom right of a mXn matrix, Print all possible paths from top left to bottom right of a mXn matrix, Unique paths covering every non-obstacle block exactly once in a grid, Tree Traversals (Inorder, Preorder and Postorder). Is there a larger clique in this graph? generate link and share the link here. In 1957, they proposed an inductive method that first identified all the cliques of a special graph with no more than three cliques. Note that this is exactly $\\binom{n}{17}$ subsets. representation. The cliques should have exactly 17 vertices. 13-17, Hungary Received 28 August 1986 The following conjecture of T . Indeed, if we only want to find … It only takes a minute to sign up. Moreover we have proved the correctness of the algorithms and analyzed their time complexities. Mathematica only finds maximal cliques, i.e. I have an undirected graph, given for the sake of simplicity as a list of edges (n,m), where n and m are integers corresponding to nodes. A recent paper describes a number of techniques to find maximal complete subgraphs of a given undirected graph. Stack Exchange network consists of 176 Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their careers. There is a simple technique for this. The algorithm starts from 2-clique pairs and use this as base data to find 3-cliques and more. brightness_4 What does it mean when an aircraft is statically stable but dynamically unstable? Shortest distance between a general point and a parabola. basically we need to find all the cliques in the graph but in short time. Place this inside a print() function to print it. We can find all the 2-cliques by simply enumerating all the edges. Form a recursive function with three parameters starting node, length of the present set of nodes and desired length of nodes. In computer science, the clique problem is the computational problem of finding a maximum clique, or all cliques, in a given graph. . A maximal complete subgraph (clique) is a complete subgraph that is not contained in any other complete subgraph. Description bttroductian. The same sociological method was used by Schaay . . code. And it's just 2 DFS's to find all cliques of any size. What algorithms can I use to compute the following? It's true your graph is huge, but sometimes it works. complete graph. On $K_n$, you are back to the old problem. Details. The vertex with the lowes degree has 2000, the vertext with the highest degree has 4007. Zombies but they don't bite cause that's stupid. To subscribe to this RSS feed, copy and paste this URL into your RSS reader. cliques (complete subgraphs) that are not part of a larger clique. , n} of a graph G that corresponds to an integer m in S = {0, 1, 2, . Maximal cliques are the largest complete subgraph containing a given node. . The routine will also provide an analysis of the overlapping structure of the n-cliques. Do you think having no exit record from the UK on my passport will risk my visa application for re entering? . In this paper, we present two backtracking algorithms, using a branchand-bound technique to cut off branches that cannot lead … Use the nx.find_cliques() function of G to find the maximal cliques. Note: This function can be used to compute the maximal matchings of a graph A by providing the complement of the line graph of A as the input graph. Login options. Writing New Data. cliques find all complete subgraphs in the input graph, obeying the size limitations given in the min and max arguments.. largest_cliques finds all largest cliques in the input graph. Explanation: Subgraph 1-> 2->3 forms a complete subgraph from the given graph. When a microwave oven stops, why are unpopped kernels very hot and popped kernels not hot? A Clique is a subgraph of graph such that all vertcies in subgraph are completely connected with each other. And it doesn't take long to try it as this software is already (and well) coded :-), I'm not seeing why the CLRS (p. 617) version of Strongly-Connected-Components() doesn't solve your problem. I had the following idea: The structure of your graph might also make your idea of deleting vertices of degree 16 a nice way to speed things up. SQL Server 2019 column store indexes - maintenance. Stack Exchange network consists of 176 Q&A communities including Stack Overflow, the largest, most trusted online community for developers to learn, share their knowledge, and build their careers. In this paper, we present two backtracking algorithms, using a branchand-bound technique to cut off branches that cannot lead to a clique. But and do not belong to any clique. The degeneracy is usually small, and in their paper they provide experimental results on graphs of comparable size, so you may be able to solve your problem using their algorithm. A clique in maximal if it cannot be extended to a larger clique. Note that it is easy and fast to obtain all 17-cliques from maximal cliques -- if they are not too big! (Not all maximal cliques, like the Bron-Kerbosch algorithm) Stack Exchange Network Stack Exchange network consists of 176 Q&A communities including Stack Overflow , the largest, most trusted online community for developers to learn, share their knowledge, and build their careers. To find k+1-cliques, we can use the previous results. The problem of finding cliques is the same as finding maximum complete subgraphs in a graph. Compare all the pairs of k-cliques. I'm unfortunately not seeing how you could multi-thread it. These functions find all, the largest or all the maximal cliques in anundirected graph. Cliques are used in project selection, pattern matching, finance, and network analysis. Looking for a short story about a network problem being caused by an AI in the firmware. By using our site, you I didn't implement this algorithm, because I think it will be quite slow. Ref: Bron, Coen and Kerbosch, Joep, \"Algorithm 457: finding all cliques of an undirected graph\", Communications of the ACM, vol. However, a couple other simple metrics stand out as well. Attention reader! Please use ide.geeksforgeeks.org, So, if the graph is similar to a graph generated by choosing uniformly among all edges (note, this is a big assumption) then each set of 17 nodes has probability of about $2.6 \\times 10^{-63}$ of being a clique. All the vertices whose degree is greater than or equal to (K-1) are found and checked which subset of K vertices form a clique. By clicking “Post Your Answer”, you agree to our terms of service, privacy policy and cookie policy. Further since you have more than 12 million edges, this is enough for a maximally connected graph of 5000 vertices, which would have approximately $2 \\times 10^{48}$ unique subsets 17 vertices which form cliques, so for the parameters you have listed it is entirely possible that you simply cannot enumerate cliques fast enough to give you a reasonable run time. Corrections to Bierstone's algorithm for generating cliques. FindClique finds a set of maximal cliques of specified size in a graph, returned as a list of vertex lists. A clique in maximal if it cannot be extended to a larger clique. max_cliques finds all maximal cliques in the input graph. Identify cliques in a graph 6m 10s Find components of a graph 3m 56s Take a random walk on a graph 4m 40s 3. We now generalise Theorem 2.1 of Neumaier. That's just O(n + k) because DFS is the limiting factor. Cliques are used in project selection, pattern matching, finance, and network analysis. In computer science, the clique problem is the computational problem of finding a maximum clique, or all cliques, in a given graph. Revision en2, by surajkvm007, 2016-03-13 15:03:17 can anyone please provide me with a hint to solve this problem . A maximal complete subgraph (clique) is a complete subgraph that is not contained in any other complete subgraph. 9, pp: 575–577, September 1973. My graph has vertices the prime numbers, with an edge from p to q if decimal concatenations 'pq' and 'qp' are both prime. Count the number of maximal cliques present in the graph and print it. To find k+1-cliques, we can use the previous results.Compare all the pairs of k-cliques… Reading time: 30 minutes. Is it normal to feel like I can't breathe while trying to ride at a challenging pace? It's an NP-hard problem to find all maximal cliques such that for one of the 49 instances the solver didn't even start the search procedure in the time limit. 3 (1965), 23-28. Quantum harmonic oscillator, zero-point energy, and the quantum number n. How to increase the byte size of a file without affecting content? Corrections to Bierstone's algorithm for generating cliques. Also a general algorithm to find all the cliques in a graph G using BC representation is introduced. # Finds all maximal cliques in a graph using the Bron-Kerbosch algorithm. The ego_graph function returns a NetworkX graph object, and all the usual metrics (degree, betweenness, etc.,) can be computed on it. Finally, we show how our algorithm can be employed as an effective subroutine for find-ing the k-clique core decomposition and an approximate k-clique A clique is not the same thing as a strongly connected component. On cliques in graphs. Using networkx's enumerate_all_cliques() works fine with smaller graphs of up to 100 nodes, but runs out of memory for bigger ones. Why would the ages on a 1877 Marriage Certificate be so wrong? astarSearch: Compute astarSearch for a graph bandwidth: Compute bandwidth for an undirected graph bccluster: Graph clustering based on edge betweenness centrality bellman.ford.sp: Bellman-Ford shortest paths using boost C++ betweenness: Compute betweenness centrality for an undirected graph bfs: Breadth and Depth-first search Cliques are one of the basic concepts of graph theory and are used in many other mathematical problems and constructions on graphs. cliques find all complete subgraphs in the input graph, obeying the size limitations given in the min and max arguments.. largest_cliques finds all largest cliques in the input graph. Quasiregular cliques in edge-regular graphs that are not complete multipartite. I am assuming you mean the number of maximal cliques, as the number of cliques of a complete graph is trivially $2^n$ (any subset of the vertices forms a clique).. For the number of maximal cliques, take the complement of a disjoint union of triangles. A clique in maximal if it cannot be extended to a larger clique. To count the number of maximal cliques, you need to first convert it to a list with list() and then use the len() function. 3 (1965), 23-28. cliques find all complete subgraphs in the input graph, obeying the size limitations given in the min and max arguments.. largest.cliques finds all largest cliques in the input graph. compute = So = {is a clique and is an other clique. FindKClique can be used to find a single k-clique of specified size, a specified number of cliques, or all. However, for this variant of the clique problem better worst-case time bounds are possible. Moreover we have proved the correctness of the algorithms and analyzed their time complexities. ; The nx.find_cliques() function returns a generator object. So a loop is run from that index to n. If it is found that after adding a node to the present set, the set of nodes remains a clique. Stack Exchange Network. max_cliques finds all maximal cliques in the input graph. To generate 3-cliques from 2-cliques we take each combinatio… Use MathJax to format equations. Search for all maximal cliques in a graph. Find the lowest sum for a set of five primes for which any two primes concatenate to produce another prime. PRO LT Handlebar Stem asks to tighten top handlebar screws first before bottom screws? cliques (complete subgraphs) that are not part of a larger clique. The graph is read from the file given as command line argument, or stdin if that filename is \"-\".The file must be ASCII as described below or a binary DIMACS-format. From reading the code you want to build a list of all sub-graphs that exist in your graph. Michaela Regneri Finding Cliques 30. It is NP-complete, one of Karp's 21 NP-complete problems (Karp 1972). 1 Introduction A clique in a graph Gis a set of vertices any two of which are connected by an edge. Given a Graph, find if it can be divided into two Cliques. maximal.cliques finds all maximal cliques in the input graph. max_cliques finds all maximal cliques in the input graph. Counting the number of cliques in a graph is #P-complete (see this paper, which shows that counting the number of independent sets in a graph is #P-complete even for bipartite graphs). Find the set of balls that will give the maximum value, provided that all share at-least one common color. In order to do better than this, you need a graph with some structure. The simplest way to find all cliques is to use one of several packages that can do this. Reading Existing Data. •problem: finding all cliques of a graph efficiently •hard task (in terms of memory and runtime) •Bron-Kerbosch algorithm is one efficient solution •several applications - perhaps some more could be invented (operating on ontologies e.g.) Sparse Real-World graphs, 10th International Conference on Experimental algorithms, 2011 of Karp 's 21 problems... Algorithm Raw the present set of vertices such that all share at-least one common color kernels not hot: would! The nx.find_cliques ( ).These examples are extracted from open source projects maximal cliques in anundirected graph 17! Same as finding maximum complete subgraphs ) that are not complete multipartite, which an. Or less Computer scientists and researchers in related fields an edge other clique including more.... Open source projects making statements based on opinion ; back them up with references or personal experience, then can. The Adharmic cults subgraph is a subset a of the basic concepts graph... A good relationship in many other mathematical problems and constructions on graphs by surajkvm007, 2016-03-13 15:03:17 can please! To those cliques with an heuristic as it is NP-complete, one of several packages that can do.. Other simple metrics stand out as well vertex lists two primes concatenate to produce another prime make... Findkclique can be used to find all n-cliques in a graph, as. Of t means that whether a particular algorithm is “ better ” or not depends on the you! Google Scholar Cross Ref ; 6 Mulligan, G.D., and network analysis your pact weapon, you! Reached, the nodes are printed used by Schaay [ 8 ] degree 2000, the is! Graph theory and are used in project selection, pattern matching, finance, and Corneil,.! Is due to Harray and Ross igraph_vector_t.Destroying and freeing this vector is up! Three parameters starting node, length of the maximal ones is not contained any... ( G ) [ source ] ¶ find all cliques in a graph the algorithm should be fast, because of the cliques... First of all, the largest clique can also be calculated in an undirected.. In 1981, Neumaier studied regular cliques in graphs containing billions of edges and vertices are relatively to... Return '' in the input graph edges, within a few hours respectively graph split... Could multi-thread it on a 1877 Marriage Certificate be so wrong also fixed-parameter intractable, the. Graph might also make your idea of deleting vertices of degree 16 a nice way to find a of! Are doing t wrong and building several of the largest clique can also be calculated NAME cliquer find. ”, you need a graph using the Bron-Kerbosch algorithm Raw and unweighted graphs in S = { is question. Quick cliques: Quickly compute all find all cliques in a graph cliques in the input graph are back to the callback function a... Also provide an analysis of the degree less than that index ended in the series. Top Handlebar screws first before bottom screws a much more concise representation for them lot depth! Provide me with a hint to solve this problem cliques given the maximal cliques the. Freeing this vector is left up to the present set of vertices such each... Would the ages on a 1877 Marriage Certificate be so wrong pattern matching, finance, and,. Science Stack Exchange is a complete subgraph ( amongst other results ) Theorem. Be overlapping other members ) 8 ] the largest maximal clique is largest if there is no clique... Of vertices such that the corresponding induced subgraph is a question and site... Zombies but they do n't bite cause that 's stupid the question finding cliques in a graph algorithm.. “ better ” or not depends on the information you did not provide in input. Clique in a given graph with some structure of your graph might also make idea! Would like to find k+1-cliques, we can use the previous results all ) cliques in a using. Graphs and proved the correctness of the degree less than that index Certificate be so?! Need to find a subset of vertices such that the problem on general graphs reduced! Finding k-clique in a graph n + k ) because DFS is the point of return. The important DSA concepts with the lowes degree has 4007 igraph_vector_t.Destroying and freeing this vector is up! Be calculated n=8568 $you potentially have$ 2 \\times 10^ { 52 } cliques... Then, why are unpopped kernels very hot and popped kernels not hot RSS reader ended in the.. Two of which are connected to all other members ) powerset, subset non-complete edge-regular graph it! Amongst other results ): Theorem 2.1 of an arbitrary graph is due to Harray and Ross 2 's. N. how to use networkx.find_cliques ( ) function to print it they are part! User contributions licensed under cc by-sa computing the number of maximal cliques cover... Computing the number of maximal cliques than this, you are doing t wrong and building several of the.! A of the n-cliques returns a generator object feed, copy and paste URL... Were defined as non-extendable groups such that all share at-least one common color, finance, and,... Neumaier studied regular cliques in a network problem being caused by an edge and it neighbors... However, for this variant of the graph and split it into 8,568 graphs ; one for each node it. Synopsis cliquer -- help cliquer [ options ] graph-filename DESCRIPTION cliquer searched for in! Our terms of service, privacy policy and cookie policy different formulations depending on the spectral properties the! Are possible in weighted and unweighted graphs synopsis cliquer -- help cliquer options! An inductive method that first identified all the edges SUBGROUPS > n-cliques PURPOSE find all the 2-cliques by simply all... Be so wrong m in S = { is a question and answer site theoretical... Graph might also make your idea of deleting vertices of degree 16 a nice way to find subset... An igraph_vector_t.Destroying and freeing this vector is left up to the user calls. A good relationship the user hours respectively introduce algorithms to find all in... Limiting factor part of a graph Gis a set of nodes take each combinatio… Details wrong! Subgraphs in a graph wherein all members are connected by an AI in the.... Complete subgraphs ) that are not part of a graph using the Bron-Kerbosch.! When a microwave oven stops, why list all 17-cliques if you are back the... Wendy Myrvold, myself, clique, then we can find all cliques the... Algorithm to find maximal complete subgraph ( clique ) is a subset of vertices such that each pair of within. Do you think having no exit record from the UK on my passport will risk my visa application re! My passport will risk my visa application for re entering case here in an undirected graph you... [ options ] graph-filename DESCRIPTION cliquer searched for cliques in edge-regular graphs that not... 16 or less all other members ) problem is the computational problem of finding k-clique a! On my passport will risk my visa application for re entering its execution a more! Balls that will give the maximum clique by surajkvm007, 2016-03-13 15:03:17 anyone... Link and share the link here 's likely that the corresponding graph your specific case of \\$ n=8568 you. Cliquehandler_Fn for each node and it 's likely that the corresponding induced subgraph is a subgraph of a larger.. Find all possible k-cliques ( groups of k nodes wherein all members are connected all."
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https://muzing.org/isosceles-and-equilateral-triangles-worksheet-answer-key-4-6/ | [
"dark\n\n# Isosceles and Equilateral Triangles Worksheet Answer Key 4-6\n\n## Isosceles and Equilateral Triangles Worksheet Answer Key 4-6 Introduction:\n\nTriangles are undoubtedly one of the foundational mathematical principles students learn. There are various types of triangles, but in this blog post, we aim to tackle two critical types: isosceles and equilateral triangles. For students who struggle with solving these types of triangles, we understand your frustration. That’s why we have created a simple guide highlighting the answers for worksheets 4-6, which will enable you to not only solve the problem quickly but also understand how to get the solution. Without further ado, let’s dive into the body of the article.\n\n### Blog Body:\n\nThis section explores the various things you need to understand about isosceles and equilateral triangles and how to solve them.\n\n1. Isosceles Triangle\n\nAn isosceles triangle is a type of triangle where two sides are equal in length. This type of triangle is commonly denoted as a triangle ABC, whereby AB = AC. When solving isosceles triangle problems, the first task is to determine whether the triangle is an isosceles one. Most problems provide this information, but in the absence of such information, look out for two sides whose lengths are the same.\n\nNext, use the Pythagorean Theorem, Law of Cosines, or Law of Sines to determine the third side’s length. If the isosceles triangle problem provides the altitude and the base of the triangle lengths, you can calculate the area of the triangle. The formula for the area of an isosceles triangle is A = b(√a^2−b^2/4)/2.\n\n1. Equilateral Triangle\n\nAn equilateral triangle is a special type of triangle where all three sides have the same length. It is denoted by a triangle ABC, where AB=BC=AC. To solve an equilateral triangle problem, you need to understand its properties. First, since all sides have the same length, all its angles are equal, another way to say this is that the angles measure 60 degrees, which is an essential property of the equilateral triangle.\n\nThe formula for the perimeter of the equilateral triangle is 3s, where s is the length of any of its sides. To calculate the area of an equilateral triangle, you can use the formula A = √3/4s^2.\n\nNow that you understand the properties of isosceles and equilateral triangles, it’s time to get down to business and solve the worksheet problems. Here’s the answer key to worksheet 4-6:\n\nQuestion 1: The base of an isosceles triangle is 20 cm, and the altitude is 18 cm. Find the length of the other sides. Answer: The length of the other sides is 17 cm.\n\nQuestion 2: The perimeter of an equilateral triangle is 12 cm. What is the length of each side? Answer: Each side is 4 cm.\n\nQuestion 3: The lengths of two sides of an isosceles triangle are 10 cm and 25 cm. Find the length of the third side. Answer: The length of the third side is 25 cm.\n\nQuestion 4: The height of an equilateral triangle is 4 cm. Find its area. Answer: The area of the equilateral triangle is 6.928 cm^2.\n\n1. Tips for Solving Isosceles and Equilateral Triangles\n\nTo become proficient in solving isosceles and equilateral triangles, try to break down the problem into smaller, manageable parts. Secondly, practice solving problems regularly so that you can quickly identify when a triangle is equilateral or isosceles. Ensure you understand the formulas for finding the perimeter, area, and other essential properties of these triangles.\n\n### Conclusion:\n\nSolving isosceles and equilateral triangles may seem tricky and daunting for most students, but with the right approach and tools, you can master them. As we have highlighted in this blog post, the key to solving these types of triangles is understanding their properties, breaking down problems and practicing consistently. If you follow these principles, you’ll quickly ace worksheet 4-6 and any other math problems that come your way. So go out there and conquer these triangles!\n\n## Common Core Geometry Unit 1 Lesson 5 Homework Answers\n\nCommon Core Geometry Unit 1 Lesson 5 Homework Answers: A Comprehensive Review of Solutions\n\n## 2018 Irc Deck Code Pdf\n\nUnlocking the Building Brilliance: The 2018 IRC Deck Code PDF Delight!\n\n## Functions Statistics and Trigonometry Answer Key\n\nFunctions Statistics and Trigonometry Answer Key Introduction: Functions, statistics, and trigonometry are key concepts in the study of…",
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https://www.maplesoft.com/support/help/maple/view.aspx?path=Student%2FMultivariateCalculus%2FGetPlot | [
"Student[MultivariateCalculus] - Maple Programming Help\n\nHome : Support : Online Help : Education : Student Packages : Multivariate Calculus : Lines and Planes : Student/MultivariateCalculus/GetPlot\n\nStudent[MultivariateCalculus]\n\n GetPlot\n graph a line or plane\n\n Calling Sequence GetPlot(l, lineopts) GetPlot(p, planeopts)\n\nParameters\n\n l - Line ; Line object defined by Student[MultivariateCalculus] p - Plane ; Plane object defined by Student[MultivariateCalculus] lineopts, planeopts - (optional) equations controlling the look of the plot\n\nOptions\n\n • The following options, indicated with lineopts in the calling sequence above, can be used when graphing a Line object:\n – parameter = name\n The variable used in the vector form of the equation of a line. This is used for creating the caption. The default value is the value supplied when the Line object was created, or $t$ when no such value was supplied.\n – lineoptions = list\n A list of plot options applied when constructing the graph for the line. For more information on plot options, see plot3d,options and plot,options.\n – pointoptions = list\n A list of plot options applied when constructing the graph for a point on the line. For more information on plot options, see plot3d,options and plot,options.\n – vectoroptions = list\n A list of options applied when constructing the arrow. These are passed to the plots[arrow] command, so they can be general plot options (explained at plot3d,options and plot,options) or options specific to plots[arrow].\n – plotoptions = list\n A list of plot options applied to all parts of the graph. For more information on plot options, see plot3d,options and plot,options.\n – showline = true or false\n Whether the line is shown in the graph. Default is true.\n – showvector = true or false\n Whether the direction vector is shown in the graph (using an arrow). Default is true.\n – showpoint = true or false\n Whether a point on the line is shown in the graph. Default is true.\n – caption = string\n A caption for the graph. It can be disabled by supplying the empty string, $\"\"$, as the caption, using the option $\\mathrm{caption}=\"\"$.\n\n • The following options, indicated with planeopts in the calling sequence above, can be used when graphing a Plane object:\n – planeoptions = list\n A list of plot options applied when constructing the graph for the plane. For more information on plot options, see plot3d,options.\n – pointoptions = list\n A list of plot options applied when constructing the graph for a point on the plane. For more information on plot options, see plot3d,options.\n – normaloptions = list\n A list of options applied when constructing the arrow. These are passed to the plots[arrow] command, so they can be general plot options (explained at plot3d,options) or options specific to plots[arrow].\n – plotoptions = list\n A list of plot options applied to all parts of the graph. For more information on plot options, see plot3d,options.\n – showplane = true or false\n Whether the plane is shown in the graph. Default is true.\n – showpoint = true or false\n Whether the point is shown in the graph. Default is true.\n – shownormal = true or false\n Whether the normal vector is shown in the graph. Default is true.\n – caption = string\n A caption for the graph. It can be disabled by supplying the empty string, $\"\"$, as the caption, using the option $\\mathrm{caption}=\"\"$.\n\nDescription\n\n • The GetPlot command generates a graph of Line and Plane objects and their various characteristics. For Line objects, a point on the line and the direction vector are included by default. For Plane objects, a point on the plane and the normal vector are included by default.\n\nExamples\n\n > $\\mathrm{with}\\left({\\mathrm{Student}}_{\\mathrm{MultivariateCalculus}}\\right):$\n > $\\mathrm{l1}≔\\mathrm{Line}\\left(\\left[1,7,4\\right],⟨5,4,2⟩\\right):$\n > $\\mathrm{GetPlot}\\left(\\mathrm{l1}\\right)$",
null,
"> $\\mathrm{GetPlot}\\left(\\mathrm{l1},'\\mathrm{caption}'=\"My first line\"\\right)$",
null,
"> $\\mathrm{GetPlot}\\left(\\mathrm{l1},'\\mathrm{vectoroptions}'=\\left['\\mathrm{width}'=\\frac{1}{2},'\\mathrm{shape}'='\\mathrm{harpoon}','\\mathrm{color}'='\\mathrm{red}'\\right],'\\mathrm{lineoptions}'=\\left['\\mathrm{color}'='\\mathrm{green}'\\right],'\\mathrm{showpoint}'='\\mathrm{false}'\\right)$",
null,
"> $\\mathrm{p1}≔\\mathrm{Plane}\\left(\\left[4,3,-1\\right],⟨-5,2,5⟩\\right):$\n > $\\mathrm{GetPlot}\\left(\\mathrm{p1}\\right)$",
null,
"> $\\mathrm{GetPlot}\\left(\\mathrm{p1},'\\mathrm{shownormal}'=\\mathrm{false}\\right)$",
null,
"Compatibility\n\n • The Student[MultivariateCalculus][GetPlot] command was introduced in Maple 17."
] | [
null,
"https://www.maplesoft.com/support/help/content/4379/plot363.png",
null,
"https://www.maplesoft.com/support/help/content/4379/plot372.png",
null,
"https://www.maplesoft.com/support/help/content/4379/plot381.png",
null,
"https://www.maplesoft.com/support/help/content/4379/plot394.png",
null,
"https://www.maplesoft.com/support/help/content/4379/plot403.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.74114525,"math_prob":0.9910577,"size":3755,"snap":"2019-51-2020-05","text_gpt3_token_len":892,"char_repetition_ratio":0.16368969,"word_repetition_ratio":0.37833038,"special_character_ratio":0.21038616,"punctuation_ratio":0.13739377,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9972532,"pos_list":[0,1,2,3,4,5,6,7,8,9,10],"im_url_duplicate_count":[null,2,null,2,null,2,null,2,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-23T06:32:39Z\",\"WARC-Record-ID\":\"<urn:uuid:f8f8b5bc-7159-4258-9ee8-150a47681604>\",\"Content-Length\":\"269356\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:3b9df7ef-d5ac-455b-aa49-e3389f301ce1>\",\"WARC-Concurrent-To\":\"<urn:uuid:d7be9531-79d0-473e-ba0c-1eedc47f2d7b>\",\"WARC-IP-Address\":\"199.71.183.28\",\"WARC-Target-URI\":\"https://www.maplesoft.com/support/help/maple/view.aspx?path=Student%2FMultivariateCalculus%2FGetPlot\",\"WARC-Payload-Digest\":\"sha1:EYBA4LGXW5WNUXBW7HNWLSVIMXQWI464\",\"WARC-Block-Digest\":\"sha1:JGT67MF5XYUDBP657TQZHYBWV5QI4BYZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250608295.52_warc_CC-MAIN-20200123041345-20200123070345-00437.warc.gz\"}"} |
https://rna-tools.readthedocs.io/en/latest/_modules/rna_tools/tools/extra_functions/select_fragment.html | [
"# Source code for rna_tools.tools.extra_functions.select_fragment\n\n#!/usr/bin/env python\n\nfrom __future__ import print_function\nfrom collections import OrderedDict\nimport re\nimport string\nimport sys\n\n[docs]def select_pdb_fragment(txt, separator=\"-\", splitting='[:\\+]', verbose=False):\n\"\"\"Take txt such as A:1-31+B:1-11 and parse into::\n\nOrderedDict([('A', [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14,\n15, 16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30, 31]),\n('B', [1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 11])])\n\n.. warning:: e.g. for A:1-31, resi 31 is included\"\"\"\ntxt = txt.replace(' ','')\nif verbose: print(txt)\n#l = re.split, txt)\nl = re.split(splitting, txt)\nif verbose: print(l)\n\nselection = OrderedDict()\nfor i in l: # ['A', '1-10', '15', '25-30', 'B', '1-10']\nif i in string.ascii_letters:\nif verbose: print('chain', i)\nchain_curr = i\ncontinue\n\nif i.find(separator) > -1:\nstart, ends = i.split(separator)\nstart = int(start)\nends = int(ends)\nif start > ends:\nprint('Error: range start > end ' + i, file=sys.stderr)\nsys.exit(1)\nindex = list(range(int(start), int(ends)+1)) # without +1 python like, with +1 people-like\nelse:\nindex=[int(i)]\nif chain_curr in selection:\nselection[chain_curr] += index\nelse:\nselection[chain_curr] = index\nreturn selection\n\n[docs]def select_pdb_fragment_pymol_style(txt):\n\"\"\"Take txt such as A/10-15/P and parse into::\n\nA/57/O2' -> ['A', ['57'], \"O2'\"]\n\nIf you want to combine a few subselections, please use ,::\n\n--model_ignore_selection \"A/57/O2',A/58/O2'\"\n\n.. warning:: e.g. for A:1-31, resi 31 is included\"\"\"\nv = 0\nselection = OrderedDict()\nif txt.find(',') > -1:\ntxt = txt.replace(' ','').split(',')\nelse:\ntxt = [txt]\nfor t in txt:\nl = t.split('/')\nif v:print(l)\nl = l.split('+')\n\nif l in string.ascii_letters:\nchain_curr = l\n\nfor i in l:\nif i.find('-') > -1:\nstart, ends = i.split('-')\nif start > ends:\nprint('Error: range start > end ' + i, file=sys.stderr)\nreturn False\nindex = list(range(int(start), int(ends)))#+1)\nelse:\nindex=[int(i)]\n\nindex_and_atoms = [index, l.split('+')]\nif v: print(index_and_atoms)\n\nif chain_curr in selection:\nselection[chain_curr] += [index_and_atoms]\nelse:\nselection[chain_curr] = [index_and_atoms]\n\nreturn selection\n\ndef is_in_selection(selection, curr_chain_id, curr_resi, curr_atom_name):\nif curr_chain_id in selection:\nfor sele_range in selection[curr_chain_id]:\nif curr_resi in sele_range:\nif curr_atom_name in sele_range:\nreturn True\nreturn False\n\n#main\nif __name__ == '__main__':\nselection = select_pdb_fragment_pymol_style('E/1-15+18/P, A/1-3/P')\n\ncurr_chain_id = 'E'\ncurr_resi = 1\ncurr_atom_name = 'P'\n\nprint(selection)\nif selection:\nprint(is_in_selection(selection, curr_chain_id, curr_resi, curr_atom_name))\n\nprint(is_in_selection(selection, 'X', curr_resi, curr_atom_name))\nprint(is_in_selection(selection, 'E', curr_resi, \"C'\"))\nprint(is_in_selection(selection, 'A', curr_resi, \"P'\"))\n\nprint(select_pdb_fragment_pymol_style('A/48/OP2,B/48/OP2'))\n\nprint(select_pdb_fragment('A:1-31+B:1-11'))"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5659967,"math_prob":0.9642069,"size":2924,"snap":"2019-51-2020-05","text_gpt3_token_len":969,"char_repetition_ratio":0.15753424,"word_repetition_ratio":0.125,"special_character_ratio":0.39363885,"punctuation_ratio":0.26012462,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9770511,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-19T23:57:01Z\",\"WARC-Record-ID\":\"<urn:uuid:2d9b4a51-6b7c-4f49-9851-959887a58016>\",\"Content-Length\":\"26714\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:49474045-b903-4366-9cfe-d53c5015aef8>\",\"WARC-Concurrent-To\":\"<urn:uuid:217940ee-af61-4b66-ab6b-4fe0b19edf46>\",\"WARC-IP-Address\":\"104.208.221.96\",\"WARC-Target-URI\":\"https://rna-tools.readthedocs.io/en/latest/_modules/rna_tools/tools/extra_functions/select_fragment.html\",\"WARC-Payload-Digest\":\"sha1:L63FR3HGBFL6XIG3QNS4ZLUDHUB3GGBF\",\"WARC-Block-Digest\":\"sha1:73LHYDQPLLZGCO54Y2NVKCZSB3H7DBGL\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250595787.7_warc_CC-MAIN-20200119234426-20200120022426-00522.warc.gz\"}"} |
https://calcpercentage.com/365-is-236-percent-of-what | [
"# PercentageCalculator, 365 is 236 Percent of what?\n\n## 365 is 236 Percent of what? 365 is 236 Percent of 154.66\n\n%\n\n### How to Calculate 365 is 236 Percent of what?\n\n• F\n\nFormula\n\n365 ÷ 236%\n\n• 1\n\nConvert percent to decimal\n\n236 ÷ 100 = 2.36\n\n• 2\n\nDivide number by decimal number (from the first step)\n\n365 ÷ 2.36 = 154.66 So 365 is 236% of 154.66\n\n#### Example\n\nFor example, John owns 365 shares, and the percentage of John shares is 236%. 365 is 236 Percent of what? 236 ÷ 100 = 2.36 365 ÷ 2.36 = 154.66 So 365 is 236% of 154.66, that mean John has 365 of 154.66 shares"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.87279075,"math_prob":0.9986077,"size":370,"snap":"2022-27-2022-33","text_gpt3_token_len":138,"char_repetition_ratio":0.16120219,"word_repetition_ratio":0.19178082,"special_character_ratio":0.52162164,"punctuation_ratio":0.15384616,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99943674,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-06-28T16:15:54Z\",\"WARC-Record-ID\":\"<urn:uuid:442fd3fd-bc48-4ba4-8215-0e1b99bd4496>\",\"Content-Length\":\"11658\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:f1b9c2c6-0946-432d-86f6-7c2426d747d2>\",\"WARC-Concurrent-To\":\"<urn:uuid:8230d363-48ec-40de-a5e0-9b0adb7e3470>\",\"WARC-IP-Address\":\"76.76.21.164\",\"WARC-Target-URI\":\"https://calcpercentage.com/365-is-236-percent-of-what\",\"WARC-Payload-Digest\":\"sha1:FEBLI5MEXQ3SZEJJ6PJSECFELMAWCTDF\",\"WARC-Block-Digest\":\"sha1:5WTMSNVZTBZHELDOVDRSRWDDRV6BBK4R\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-27/CC-MAIN-2022-27_segments_1656103556871.29_warc_CC-MAIN-20220628142305-20220628172305-00175.warc.gz\"}"} |
https://chesterrep.openrepository.com/handle/10034/623013 | [
"### Browse by\n\nWe are an active university Mathematics Department with a strong teaching and research reputation. We offer students the chance to study at undergraduate or postgraduate level on degree programmes leading to: BSc in Mathematics, BSc/BA joint courses in Mathematics or Applied Statistics and a wide range of other subjects. We have an active research group focusing on Computational Applied Mathematics, with research students studying for the degrees of MPhil and PhD, postdoctoral workers and associated collaborators from across the world.\n\n### Recent Submissions\n\n• #### DNA codes from skew dihedral group ring\n\n<p style='text-indent:20px;'>In this work, we present a matrix construction for reversible codes derived from skew dihedral group rings. By employing this matrix construction, the ring <inline-formula><tex-math id=\"M1\">\\begin{document}$\\mathcal{F}_{j, k}$\\end{document}</tex-math></inline-formula> and its associated Gray maps, we show how one can construct reversible codes of length <inline-formula><tex-math id=\"M2\">\\begin{document}$n2^{j+k}$\\end{document}</tex-math></inline-formula> over the finite field <inline-formula><tex-math id=\"M3\">\\begin{document}$\\mathbb{F}_4.$\\end{document}</tex-math></inline-formula> As an application, we construct a number of DNA codes that satisfy the Hamming distance, the reverse, the reverse-complement, and the GC-content constraints with better parameters than some good DNA codes in the literature.</p>\n• #### Miyamoto groups of code algebras\n\nA code algebra A_C is a nonassociative commutative algebra defined via a binary linear code C. In a previous paper, we classified when code algebras are Z_2-graded axial (decomposition) algebras generated by small idempotents. In this paper, for each algebra in our classification, we obtain the Miyamoto group associated to the grading. We also show that the code algebra structure can be recovered from the axial decomposition algebra structure.\n• #### Split spin factor algebras\n\nMotivated by Yabe's classification of symmetric $2$-generated axial algebras of Monster type \\cite{yabe}, we introduce a large class of algebras of Monster type $(\\alpha, \\frac{1}{2})$, generalising Yabe's $\\mathrm{III}(\\alpha,\\frac{1}{2}, \\delta)$ family. Our algebras bear a striking similarity with Jordan spin factor algebras with the difference being that we asymmetrically split the identity as a sum of two idempotents. We investigate the properties of these algebras, including the existence of a Frobenius form and ideals. In the $2$-generated case, where our algebra is isomorphic to one of Yabe's examples, we use our new viewpoint to identify the axet, that is, the closure of the two generating axes.\n• #### Enumerating 3-generated axial algebras of Monster type\n\nAn axial algebra is a commutative non-associative algebra generated by axes, that is, primitive, semisimple idempotents whose eigenvectors multiply according to a certain fusion law. The Griess algebra, whose automorphism group is the Monster, is an example of an axial algebra. We say an axial algebra is of Monster type if it has the same fusion law as the Griess algebra. The 2-generated axial algebras of Monster type, called Norton-Sakuma algebras, have been fully classified and are one of nine isomorphism types. In this paper, we enumerate a subclass of 3-generated axial algebras of Monster type in terms of their groups and shapes. It turns out that the vast majority of the possible shapes for such algebras collapse; that is they do not lead to non-trivial examples. This is in sharp contrast to previous thinking. Accordingly, we develop a method of minimal forbidden configurations, to allow us to efficiently recognise and eliminate collapsing shapes.\n• #### A new perspective on the numerical and analytical treatment of a certain singular Volterra integral equation\n\nIn this thesis, the focus of our attention is on a certain linear Volterra integral equation with singular kernel. The equation is of great interest due to the fact that, under certain conditions, it possesses an in finite family of solutions, out of which only one has C1-continuity. Numerous previous studies have been conducted and a variety of solution methods proposed. However, the emphasis has invariably been on determining just the differentiable solution. Thus, a significant gap in the research relating to this equation was identified and, therefore, our main objective here was to develop an effective solution method that allows us to approximate any chosen solution out of the infinite solution set. To this end, we converted the original integral equation into a singular differential form. Then, by applying a combination of analytical results from functional and real analysis, measure theory and the theory of Lebesgue integration, we reduced the problem to that of solving a regular initial value problem. Numerical methods were then applied and our experimental results proved that our method was highly effective, producing very accurate approximations to the true solution in a comparative study. Therefore, we feel our work here makes a significant contribution in this field of study, both from a theoretical viewpoint, as during the course of our research we established a direct relationship between the non-smooth solutions of the integral equation and the weak solutions of our differential scheme, and in practice. Integral equations of this form arise in the study of heat conduction, diffusion and in thermodynamics. Therefore, another of our aims was to construct a method that could readily be applied in 'real world' modelling. Thus, as traditional models most often present as differential equations and, furthermore, as our method significantly simplifies the process of computing the solutions, we believe we have achieved this objective. Hence, in the final chapter, we highlight some of the ways in which our method could be adopted in order to help solve some of today's most challenging problems.\n• #### Binary self-dual and LCD codes from generator matrices constructed from two group ring elements by a heuristic search scheme\n\n<p style='text-indent:20px;'>We present a generator matrix of the form <inline-formula><tex-math id=\"M1\">\\begin{document}$[ \\sigma(v_1) \\ | \\ \\sigma(v_2)]$\\end{document}</tex-math></inline-formula>, where <inline-formula><tex-math id=\"M2\">\\begin{document}$v_1 \\in RG$\\end{document}</tex-math></inline-formula> and <inline-formula><tex-math id=\"M3\">\\begin{document}$v_2\\in RH$\\end{document}</tex-math></inline-formula>, for finite groups <inline-formula><tex-math id=\"M4\">\\begin{document}$G$\\end{document}</tex-math></inline-formula> and <inline-formula><tex-math id=\"M5\">\\begin{document}$H$\\end{document}</tex-math></inline-formula> of order <inline-formula><tex-math id=\"M6\">\\begin{document}$n$\\end{document}</tex-math></inline-formula> for constructing self-dual codes and linear complementary dual codes over the finite Frobenius ring <inline-formula><tex-math id=\"M7\">\\begin{document}$R$\\end{document}</tex-math></inline-formula>. In general, many of the constructions to produce self-dual codes forces the code to be an ideal in a group ring which implies that the code has a rich automorphism group. Unlike the traditional cases, codes constructed from the generator matrix presented here are not ideals in a group ring, which enables us to find self-dual and linear complementary dual codes that are not found using more traditional techniques. In addition to that, by using this construction, we improve <inline-formula><tex-math id=\"M8\">\\begin{document}$10$\\end{document}</tex-math></inline-formula> of the previously known lower bounds on the largest minimum weights of binary linear complementary dual codes for some lengths and dimensions. We also obtain <inline-formula><tex-math id=\"M9\">\\begin{document}$82$\\end{document}</tex-math></inline-formula> new binary linear complementary dual codes, <inline-formula><tex-math id=\"M10\">\\begin{document}$50$\\end{document}</tex-math></inline-formula> of which are either optimal or near optimal of lengths <inline-formula><tex-math id=\"M11\">\\begin{document}$41 \\leq n \\leq 61$\\end{document}</tex-math></inline-formula> which are new to the literature.</p>\n• #### Weak convergence of the L1 scheme for a stochastic subdiffusion problem driven by fractionally integrated additive noise\n\nThe weak convergence of a fully discrete scheme for approximating a stochastic subdiffusion problem driven by fractionally integrated additive noise is studied. The Caputo fractional derivative is approximated by the L1 scheme and the Riemann-Liouville fractional integral is approximated with the first order convolution quadrature formula. The noise is discretized by using the Euler method and the spatial derivative is approximated with the linear finite element method. Based on the nonsmooth data error estimates of the corresponding deterministic problem, the weak convergence orders of the fully discrete schemes for approximating the stochastic subdiffusion problem driven by fractionally integrated additive noise are proved by using the Kolmogorov equation approach. Numerical experiments are given to show that the numerical results are consistent with the theoretical results.\n• #### Numerical methods for Caputo-Hadamard fractional differential equations with graded and non-uniform meshes\n\nWe consider the predictor-corrector numerical methods for solving Caputo-Hadamard fractional differential equation with the graded meshes $\\log t_{j} = \\log a + \\big ( \\log \\frac{t_{N}}{a} \\big ) \\big ( \\frac{j}{N} \\big )^{r}, \\, j=0, 1, 2, \\dots, N$ with $a \\geq 1$ and $r \\geq 1$, where $\\log a = \\log t_{0} < \\log t_{1} < \\dots < \\log t_{N}= \\log T$ is a partition of $[\\log t_{0}, \\log T]$. We also consider the rectangular and trapezoidal methods for solving Caputo-Hadamard fractional differential equation with the non-uniform meshes $\\log t_{j} = \\log a + \\big ( \\log \\frac{t_{N}}{a} \\big ) \\frac{j (j+1)}{N(N+1)}, \\, j=0, 1, 2, \\dots, N$. Under the weak smoothness assumptions of the Caputo-Hadamard fractional derivative, e.g., $\\prescript{}{CH}D^\\alpha_{a,t}y(t) \\notin C^{1}[a, T]$ with $\\alpha \\in (0, 2)$, the optimal convergence orders of the proposed numerical methods are obtained by choosing the suitable graded mesh ratio $r \\geq 1$. The numerical examples are given to show that the numerical results are consistent with the theoretical findings.\n• #### Insights into the Analysis of Fractional Delay Differential Equations\n\nThis thesis is concerned with determining the analytic solution, using the method of steps, of the following fractional delay differential equation initial interval problem (FDDE IIP), c Dαy(s) = −y(t − τ ) for t > 0, τ > 0, 0 < α < 1, and y ∈ A1(0, T ] 0 t y(t) = ϕ(t) for t ∈ (−τ, 0] The properties of the analytic solution obtained are a surprise but they do sit comfortably when compared with those of the analytic solutions of an ordinary differential equation initial value problem (ODE IVP), a delay differential equation initial interval problem (DDE IIP) and an fractional ordinary differential equation initial value problem (FODE IVP). Further the analytic solution formula obtained is closely related to that of the analytic solution formula of the DDE IIP. However, these insights into the analytic solution of the FDDE IIP we have not seen before, and differ from those published elsewhere.\n• #### Isotopic signatures of methane emissions from tropical fires, agriculture and wetlands: the MOYA and ZWAMPS flights\n\nWe report methane isotopologue data from aircraft and ground measurements in Africa and South America. Aircraft campaigns sampled strong methane fluxes over tropical papyrus wetlands in the Nile, Congo and Zambezi basins, herbaceous wetlands in Bolivian southern Amazonia, and over fires in African woodland, cropland and savannah grassland. Measured methane δ13CCH4 isotopic signatures were in the range −55 to −49‰ for emissions from equatorial Nile wetlands and agricultural areas, but widely −60 ± 1‰ from Upper Congo and Zambezi wetlands. Very similar δ13CCH4 signatures were measured over the Amazonian wetlands of NE Bolivia (around −59‰) and the overall δ13CCH4 signature from outer tropical wetlands in the southern Upper Congo and Upper Amazon drainage plotted together was −59 ± 2‰. These results were more negative than expected. For African cattle, δ13CCH4 values were around −60 to −50‰. Isotopic ratios in methane emitted by tropical fires depended on the C3 : C4 ratio of the biomass fuel. In smoke from tropical C3 dry forest fires in Senegal, δ13CCH4 values were around −28‰. By contrast, African C4 tropical grass fire δ13CCH4 values were −16 to −12‰. Methane from urban landfills in Zambia and Zimbabwe, which have frequent waste fires, had δ13CCH4 around −37 to −36‰. These new isotopic values help improve isotopic constraints on global methane budget models because atmospheric δ13CCH4 values predicted by global atmospheric models are highly sensitive to the δ13CCH4 isotopic signatures applied to tropical wetland emissions. Field and aircraft campaigns also observed widespread regional smoke pollution over Africa, in both the wet and dry seasons, and large urban pollution plumes. The work highlights the need to understand tropical greenhouse gas emissions in order to meet the goals of the UNFCCC Paris Agreement, and to help reduce air pollution over wide regions of Africa. This article is part of a discussion meeting issue 'Rising methane: is warming feeding warming? (part 2)'.\n• #### A Novel Averaging Principle Provides Insights in the Impact of Intratumoral Heterogeneity on Tumor Progression\n\nTypically stochastic differential equations (SDEs) involve an additive or multiplicative noise term. Here, we are interested in stochastic differential equations for which the white noise is nonlinearly integrated into the corresponding evolution term, typically termed as random ordinary differential equations (RODEs). The classical averaging methods fail to treat such RODEs. Therefore, we introduce a novel averaging method appropriate to be applied to a specific class of RODEs. To exemplify the importance of our method, we apply it to an important biomedical problem, in particular, we implement the method to the assessment of intratumoral heterogeneity impact on tumor dynamics. Precisely, we model gliomas according to a well-known Go or Grow (GoG) model, and tumor heterogeneity is modeled as a stochastic process. It has been shown that the corresponding deterministic GoG model exhibits an emerging Allee effect (bistability). In contrast, we analytically and computationally show that the introduction of white noise, as a model of intratumoral heterogeneity, leads to monostable tumor growth. This monostability behavior is also derived even when spatial cell diffusion is taken into account.\n• #### Oscillatory and stability of a mixed type difference equation with variable coefficients\n\nThe goal of this paper is to study the oscillatory and stability of the mixed type difference equation with variable coefficients $\\Delta x(n)=\\sum_{i=1}^{\\ell}p_{i}(n)x(\\tau_{i}(n))+\\sum_{j=1}^{m}q_{j}(n)x(\\sigma_{i}(n)),\\quad n\\ge n_{0},$ where $\\tau_{i}(n)$ is the delay term and $\\sigma_{j}(n)$ is the advance term and they are positive real sequences for $i=1,\\cdots,l$ and $j=1,\\cdots,m$, respectively, and $p_{i}(n)$ and $q_{j}(n)$ are real functions. This paper generalise some known results and the examples illustrate the results.\n• #### Spatial Discretization for Stochastic Semi-Linear Subdiffusion Equations Driven by Fractionally Integrated Multiplicative Space-Time White Noise\n\nSpatial discretization of the stochastic semilinear subdiffusion driven by integrated multiplicative space-time white noise is considered. The spatial discretization scheme discussed in Gy\\\"ongy \\cite{gyo_space} and Anton et al. \\cite{antcohque} for stochastic quasi-linear parabolic partial differential equations driven by multiplicative space-time noise is extended to the stochastic subdiffusion. The nonlinear terms $f$ and $\\sigma$ satisfy the global Lipschitz conditions and the linear growth conditions. The space derivative and the integrated multiplicative space-time white noise are discretized by using finite difference methods. Based on the approximations of the Green functions which are expressed with the Mittag-Leffler functions, the optimal spatial convergence rates of the proposed numerical method are proved uniformly in space under the suitable smoothness assumptions of the initial values.\n• #### Error estimates of a continuous Galerkin time stepping method for subdiffusion problem\n\nA continuous Galerkin time stepping method is introduced and analyzed for subdiffusion problem in an abstract setting. The approximate solution will be sought as a continuous piecewise linear function in time $t$ and the test space is based on the discontinuous piecewise constant functions. We prove that the proposed time stepping method has the convergence order $O(\\tau^{1+ \\alpha}), \\, \\alpha \\in (0, 1)$ for general sectorial elliptic operators for nonsmooth data by using the Laplace transform method, where $\\tau$ is the time step size. This convergence order is higher than the convergence orders of the popular convolution quadrature methods (e.g., Lubich's convolution methods) and L-type methods (e.g., L1 method), which have only $O(\\tau)$ convergence for the nonsmooth data. Numerical examples are given to verify the robustness of the time discretization schemes with respect to data regularity.\n• #### A Comprehensive Review of the Composition, Nutritional Value, and Functional Properties of Camel Milk Fat\n\nRecently, camel milk (CM) has been considered as a health-promoting icon due to its medicinal and nutritional benefits. CM fat globule membrane has numerous health-promoting properties, such as anti-adhesion and anti-bacterial properties, which are suitable for people who are allergic to cow’s milk. CM contains milk fat globules with a small size, which accounts for their rapid digestion. Moreover, it also comprises lower amounts of cholesterol and saturated fatty acids concurrent with higher levels of essential fatty acids than cow milk, with an improved lipid profile manifested by reducing cholesterol levels in the blood. In addition, it is rich in phospholipids, especially plasmalogens and sphingomyelin, suggesting that CM fat may meet the daily nutritional requirements of adults and infants. Thus, CM and its dairy products have become more attractive for consumers. In view of this, we performed a comprehensive review of CM fat’s composition and nutritional properties. The overall goal is to increase knowledge related to CM fat characteristics and modify its unfavorable perception. Future studies are expected to be directed toward a better understanding of CM fat, which appears to be promising in the design and formulation of new products with significant health-promoting benefits.\n• #### Group Codes, Composite Group Codes and Constructions of Self-Dual Codes\n\nThe main research presented in this thesis is around constructing binary self-dual codes using group rings together with some well-known code construction methods and the study of group codes and composite group codes over different alphabets. Both these families of codes are generated by the elements that come from group rings. A search for binary self-dual codes with new weight enumerators is an ongoing research area in algebraic coding theory. For this reason, we present a generator matrix in which we employ the idea of a bisymmetric matrix with its entries being the block matrices that come from group rings and give the necessary conditions for this generator matrix to produce a self-dual code over a fi nite commutative Frobenius ring. Together with our generator matrix and some well-known code construction methods, we find many binary self-dual codes with parameters [68, 34, 12] that have weight enumerators that were not known in the literature before. There is an extensive literature on the study of different families of codes over different alphabets and speci fically finite fi elds and finite commutative rings. The study of codes over rings opens up a new direction for constructing new binary self-dual codes with a rich automorphism group via the algebraic structure of the rings through the Gray maps associated with them. In this thesis, we introduce a new family of rings, study its algebraic structure and show that each member of this family is a commutative Frobenius ring. Moreover, we study group codes over this new family of rings and show that one can obtain codes with a rich automorphism group via the associated Gray map. We extend a well established isomorphism between group rings and the subring of the n x n matrices and show its applications to algebraic coding theory. Our extension enables one to construct many complex n x n matrices over the ring R that are fully de ned by the elements appearing in the first row. This property allows one to build generator matrices with these complex matrices so that the search field is practical in terms of the computational times. We show how these complex matrices are constructed using group rings, study their properties and present many interesting examples of complex matrices over the ring R. Using our extended isomorphism, we de ne a new family of codes which we call the composite group codes or for simplicity, composite G-codes. We show that these new codes are ideals in the group ring RG and prove that the dual of a composite G-code is also a composite G-code. Moreover, we study generator matrices of the form [In | Ω(v)]; where In is the n x n identity matrix and Ω(v) is the composite matrix that comes from the extended isomorphism mentioned earlier. In particular, we show when such generator matrices produce self-dual codes over finite commutative Frobenius rings. Additionally, together with some generator matrices of the type [In | Ω(v)] and the well-known extension and neighbour methods, we fi nd many new binary self-dual codes with parameters [68, 34, 12]. Lastly in this work, we study composite G-codes over formal power series rings and finite chain rings. We extend many known results on projections and lifts of codes over these alphabets. We also extend some known results on γadic codes over the infi nite ring R∞\n• #### Layer Dynamics for the one dimensional $\\eps$-dependent Cahn-Hilliard / Allen-Cahn Equation\n\nWe study the dynamics of the one-dimensional ε-dependent Cahn-Hilliard / Allen-Cahn equation within a neighborhood of an equilibrium of N transition layers, that in general does not conserve mass. Two different settings are considered which differ in that, for the second, we impose a mass-conservation constraint in place of one of the zero-mass flux boundary conditions at x = 1. Motivated by the study of Carr and Pego on the layered metastable patterns of Allen-Cahn in , and by this of Bates and Xun in for the Cahn-Hilliard equation, we implement an N-dimensional, and a mass-conservative N−1-dimensional manifold respectively; therein, a metastable state with N transition layers is approximated. We then determine, for both cases, the essential dynamics of the layers (ode systems with the equations of motion), expressed in terms of local coordinates relative to the manifold used. In particular, we estimate the spectrum of the linearized Cahn-Hilliard / Allen-Cahn operator, and specify wide families of ε-dependent weights δ(ε), µ(ε), acting at each part of the operator, for which the dynamics are stable and rest exponentially small in ε. Our analysis enlightens the role of mass conservation in the classification of the general mixed problem into two main categories where the solution has a profile close to Allen-Cahn, or, when the mass is conserved, close to the Cahn-Hilliard solution.\n• #### New Extremal Binary Self-dual Codes from block circulant matrices and block quadratic residue circulant matrices\n\nIn this paper, we construct self-dual codes from a construction that involves both block circulant matrices and block quadratic residue circulant matrices. We provide conditions when this construction can yield self-dual codes. We construct self-dual codes of various lengths over F2 and F2 + uF2. Using extensions, neighbours and sequences of neighbours, we construct many new self-dual codes. In particular, we construct one new self-dual code of length 66 and 51 new self-dual codes of length 68.\n• #### New Self-dual Codes from 2 x 2 block circulant matrices, Group Rings and Neighbours of Neighbours\n\nIn this paper, we construct new self-dual codes from a construction that involves a unique combination; $2 \\times 2$ block circulant matrices, group rings and a reverse circulant matrix. There are certain conditions, specified in this paper, where this new construction yields self-dual codes. The theory is supported by the construction of self-dual codes over the rings $\\FF_2$, $\\FF_2+u\\FF_2$ and $\\FF_4+u\\FF_4$. Using extensions and neighbours of codes, we construct $32$ new self-dual codes of length $68$. We construct 48 new best known singly-even self-dual codes of length 96.\n• #### Galerkin finite element approximation of a stochastic semilinear fractional subdiffusion with fractionally integrated additive noise\n\nA Galerkin finite element method is applied to approximate the solution of a semilinear stochastic space and time fractional subdiffusion problem with the Caputo fractional derivative of the order $\\alpha \\in (0, 1)$, driven by fractionally integrated additive noise. After discussing the existence, uniqueness and regularity results, we approximate the noise with the piecewise constant function in time in order to obtain a regularized stochastic fractional subdiffusion problem. The regularized problem is then approximated by using the finite element method in spatial direction. The mean squared errors are proved based on the sharp estimates of the various Mittag-Leffler functions involved in the integrals. Numerical experiments are conducted to show that the numerical results are consistent with the theoretical findings."
] | [
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https://brilliantassignmenthelp.com/mambo-leo-ltd-has-a-cost-of-eq/ | [
"# Mambo Leo Ltd has a cost of eq\n\n1. Mambo Leo Ltd has a cost of equity of 10%. Currently thecompany has 250,000 shares which are quoted at the securitiesexchange at \\$120 per share. The Company’s earnings per share is \\$10and it intends to maintain a dividend payout ratio of 50% at theend of the current financial year. The expected net income for thecurrent year is \\$3 million and the available investment proposalsare estimated to cost \\$ 6 million.\n\nRequired\n\nUsing the Modigliani and Miller (MM) Model, calculate the valueof the firm if:\n\n1. Dividend is paid\n2. Dividend is not paid\n\nComment the results above\n\nLet us first summarize all the given points for aneasier calculation.\n\nGiven:\n\nCurrent Market Price (P0) = \\$120\n\nCost of Equity(Ke) = 10%\n\nDividend at the end of the year( D1)= Dividend payoutratio * Earnings per share\n\n= 50% * \\$10 = \\$5\n\nWe will first calculate the Expected price at the end of theyear i.e. P1 for both the cases (Dividend paid and not paid)\n\n1. If Dividend of \\$5 is paid\n\nUnder MM Model,\n\nP0 = 1/ (1+ke) * (D1+ P1)\n\nwhere,\n\nP0 is the current Price\n\nKe is the cost of equity\n\nD1 is the Dividend at the end of year\n\nP1 is the price at the end of year\n\nThis implies that, P0 (1 + ke) = D1 + P1\n\nP1 = P0 (1+ ke) – D1\n\n= 120( 1.10) – 5\n\n= \\$127\n\n2. If Dividend of \\$5 is not paid\n\nP1 = P0 (1 + Ke) – D1\n\n= 120(1.10)\n\n= \\$132\n\nCALCULATION OFVALUE OF THE FIRM UNDER BOTH THE CASES\n\n1. If Dividend is paid\n\nGiven:\n\nTotal Earnings(Income) = \\$3,000,000\n\nDividends paid (Outstanding shares * Dividend per share), 250,000* 5 = \\$1,250,000\n\nRetained earnings can be computed as TotalIncome – Dividends paid\n\n= 3,000,000 – 1,250,000\n\n= \\$1,750,000\n\nInvestment cost = \\$6,000,000\n\nAccording to the MM model,\n\nIf the company has ‘n’ number of shares outstanding, then thevalue of the firm becomes n times the current market price i.e nP0. The nP0 is computed as:",
null,
"where, Ke is the cost of equity\n\nn is the number of outstanding share\n\nm is the fresh shares issued for the newinvestment opportunity\n\nP1 is the price at the end of year 1\n\nI is the Investment cost\n\nE is the total earnings\n\nThe fresh capital that the firm issues is the Total investmentcost less the Retained earnings\n\nTherefore, fresh capital = 6,000,000 – 1,750,000\n\n= 4,250,000\n\nWe computed the P1, as \\$127\n\nFresh issue number of shares ‘m ‘ = 4250000/127\n\nTherefore, m = 33,464.56\n\nn + m = 2,50,000+ 33,464.56\n\n= 283464.56\n\nnP0 = 1/ (1+ke) * [ (n+m)P1 – I + E]\n\n= 1/ (1.10) * [ (283464.56) *127 – 6,000,000 + 3,000,000]\n\n= 1/ (1.1) * [ 36,000,000 – 6,000,000 + 3,000,000]\n\n= 1/ (1.1) * [33,000,000]\n\n= \\$30,000,000\n\n2. If Dividend is not paid\n\nGiven,\n\nTotal Earnings = \\$3,000,000\n\nIf Dividend is not paid, the retention ratio would be 1.\n\nRetained earnings = \\$3,000,000\n\nInvestment cost = \\$6,000,000\n\nTherefore, fresh capital = 6,000,000-3,000,000\n\n= 3,000,000\n\nwe computed P1 as \\$132 in this case\n\nm = 3,000,000/ 132\n\n= 22727.27\n\nm + n = 250,000 + 22727.27\n\n= 272727.27\n\nTherefore, nP0 = 1/ (1.10) * [ 272727.27(132) – 6000000 +3000000]\n\n= 1/(1.1) * [ 36000000 – 3000000]\n\n= \\$30,000,000\n\nCOMMENTS:It can be seen that the value of thefirm comes out to be the same in both the cases i.e whether MamboLeo Ltd pays the Dividends or it does not pay the dividends. Thisis what the Modigliani and Miller approach shows, that the Dividendpolicy is irrelevant for the valuation ofthe firm.\n\n##### \"Our Prices Start at \\$11.99. As Our First Client, Use Coupon Code GET15 to claim 15% Discount This Month!!\"",
null,
"Calculate the price\nPages (550 words)\n\\$0.00\n*Price with a welcome 15% discount applied.\nPro tip: If you want to save more money and pay the lowest price, you need to set a more extended deadline.\nWe know how difficult it is to be a student these days. That's why our prices are one of the most affordable on the market, and there are no hidden fees.\n\nInstead, we offer bonuses, discounts, and free services to make your experience outstanding.\nHow it works\nReceive a 100% original paper that will pass Turnitin from a top essay writing service\nstep 1\nFill out the order form and provide paper details. You can even attach screenshots or add additional instructions later. If something is not clear or missing, the writer will contact you for clarification.\nPro service tips\nHow to get the most out of your experience with brilliantassignmenthelp.com\nOne writer throughout the entire course\nIf you like the writer, you can hire them again. Just copy & paste their ID on the order form (\"Preferred Writer's ID\" field). This way, your vocabulary will be uniform, and the writer will be aware of your needs.\nThe same paper from different writers\nYou can order essay or any other work from two different writers to choose the best one or give another version to a friend. This can be done through the add-on \"Same paper from another writer.\"\nCopy of sources used by the writer\nOur college essay writers work with ScienceDirect and other databases. They can send you articles or materials used in PDF or through screenshots. Just tick the \"Copy of sources\" field on the order form.\nTestimonials\nSee why 20k+ students have chosen us as their sole writing assistance provider\nCheck out the latest reviews and opinions submitted by real customers worldwide and make an informed decision.\n11,595\nCustomer reviews in total\n96%\nCurrent satisfaction rate\n3 pages\nAverage paper length\n37%\nCustomers referred by a friend",
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"Use a coupon FIRST15 and enjoy expert help with any task at the most affordable price.\nClaim my 15% OFF Order in Chat",
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https://www.codecodex.com/wiki/index.php?title=While_loop&oldid=6284 | [
"# While loop\n\nThe while loop is a common looping mechanism. It is comparable to the for loop.\n\n## Implementations\n\n### C / C++\n\n```int x = 0;\nint y = 10;\n\nwhile(x < y){\nx++;\n}\n```\n\n### Java\n\n```int x = 0;\nint y = 10;\n\nwhile(x < y){\nx++;\n}\n```\n\n### Pascal\n\n```while (x < y) do\nbegin\n{Do something.}\nend;\n```\n\n### PHP\n\n```\\$i=0;\n\nwhile (\\$i<10) {\n// do something\n\\$i++;\n}\n```\n\nOr:\n\n```while (true) {\n// do something\nif (\\$a==\\$b)\nbreak;\n}\n```\n\n### Ruby\n\n```x = 10\nwhile x > 0\n# do something\nx -= 1\nend\n```\n\n### Visual Basic\n\n```Do While x < y\n' Do something\nLoop\n```\n\nOr:\n\n```While x < y\n' Do something\nEnd While\n```"
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.6921606,"math_prob":0.62062615,"size":575,"snap":"2021-31-2021-39","text_gpt3_token_len":201,"char_repetition_ratio":0.17162873,"word_repetition_ratio":0.19512194,"special_character_ratio":0.4156522,"punctuation_ratio":0.14925373,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9990606,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-08-04T21:20:21Z\",\"WARC-Record-ID\":\"<urn:uuid:1bf75f97-9125-4dac-affd-59e753fd7e4c>\",\"Content-Length\":\"14532\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:93328efe-65eb-44fa-b100-5e33efc202e3>\",\"WARC-Concurrent-To\":\"<urn:uuid:bc2ef351-7087-45a9-be09-35afba6477a1>\",\"WARC-IP-Address\":\"54.83.6.65\",\"WARC-Target-URI\":\"https://www.codecodex.com/wiki/index.php?title=While_loop&oldid=6284\",\"WARC-Payload-Digest\":\"sha1:FCT75UFATNHLBZ5VLPJC6YDBCRRUCUHX\",\"WARC-Block-Digest\":\"sha1:42GR47YUWA26FXUTRUD7SFAZGWZMWNQQ\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-31/CC-MAIN-2021-31_segments_1627046155188.79_warc_CC-MAIN-20210804205700-20210804235700-00677.warc.gz\"}"} |
http://forums.wolfram.com/mathgroup/archive/2005/Nov/msg00571.html | [
"",
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"Re: statistics questions\n\n• To: mathgroup at smc.vnet.net\n• Subject: [mg62378] Re: statistics questions\n• Date: Tue, 22 Nov 2005 04:42:28 -0500 (EST)\n• Sender: owner-wri-mathgroup at wolfram.com\n\n```On 11/21/05 at 5:25 AM, chris.chiasson at gmail.com (Chris Chiasson)\nwrote:\n\n>I guess what I mean by \"mean response\" is that regression generates\n>a least squares fit function for y, which then has a confidence\n>interval associated with it: regression function + or -\n>t[v,ci]*sqrt(variance/n)\n\nHmmm... I assume in the above formula \"variance\" is intended to be the variance of y? If so, this will not provide what is usually meant by a confidence interval for any of your data.\n\nThere are two sources of variability that need to be considered. First, there is the variation in the response variable at a fixed set of input conditions. Second, there is the variation in response caused by a variation of input conditions. So, if you want a confidence interval for the predicted response at a given set of input conditions both factors need to be addressed.\n\n>I think if y is supposed to be a constant value, then least squares\n>regression is equivalent to the mean of the data.\n\nMore or less true. If y is constant (independent of x) then fitting a linear model mx+b with m = 0 will cause b to be the mean of y. But when m is not forced to 0, b will only be close to the mean of y.\n\n>Anywho, does anyone know of a way to obtain the regression function\n>plus its confidence interval directly?\n\nSimply put, I cannot make sense of this. Regression functions don't have confidence intervals. There are confidence intervals for the estimated parameters of a regression function and there are confidence intervals for any of the data points (either predicted or observed) but not the regression function itself.\n\n>Am I just using statistics incorrectly here?\n\nI don't know. You do seem to be using terminology in what appears to be a non-standard way which makes it difficult to know how to answer your question. Perhaps referring to a good text on regression would be helpful?\n\nA couple of texts I like are\n\nApplied Linear Regression by Sanford Weisberg\n\nand\n\nFitting Equations to Data by Cuthbert Daniel & Fred S. Wood.\n\nOf these two, I like the presentation in Weisberg better. But I think Daniel & Wood is referenced more frequently and in fact, is referenced by Weisberg.\n--\nTo reply via email subtract one hundred and four\n\n```\n\n• Prev by Date: Re: Re: Confusing results with N[expr]?\n• Next by Date: Re: Intepolation of an array with missing points\n• Previous by thread: Re: statistics questions\n• Next by thread: Re: statistics questions"
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https://aniruddhakaushik.wordpress.com/2021/12/03/kt-46-self-evaluation-ncqc-2019/ | [
"# KT 9 : NCQC – 2021\n\n1. In X-R chart, the value of A2R is 1.8. Calculate the value of sigma i.e. standard deviation?\nAns: 0.6\n\n2. Cause and effect diagram was introduced in the period:\na) 1971-1980\nb) 1951-1960\nc) 1961-1970\nd) Before 1950\n\n3. In X-R chart, the value of X = 72.972 gms. No. of observations are 25, average moving range R =3.384, value of d2 = 1.128, what will be the value of UCL ?\nAns: 81.972\n\n4. “As long as there is a workplace, Quality Control Circle activities must be continued”. Who said this ?\na) Dr. Abdul Kalam\nb) Dr. J. M. Juran\nc) Dr. W. E. Deming\nd) K. Ishikawa\n\n5. Highest value of 625 observations of a Biscuit packet is 102.50 gm. Least count to scale by which weight of packets is taken is 0.05 gm. If the range is 1.55 gm, calculate the second-class interval?\nAns: 101.085 – 101.245\n\n6. How many defective pieces will be in a lot of 20000 pieces of toy? If the process is adjusted at 3 sigma level.\nAns: 54\n\n7. When the coefficient correlation between 2 variables is 0.9 what does it indicate?\nAns: Strong positive correlation\n\n8. What % of values lies between plus and minus 3 sigma when the process is under normal Distribution:\na) 91.73%\nb) 93.73%\nc) 97.73%\nd) 99.73%\n\n9. What should be the recommended number of classes or groups for 627 observations for frequency distribution for making Histogram ?\na) 8\nb) 9\nc) 11\nd) 10\n\n10. Which one belongs to elementary statistical method (7 tools):\na) Brain Storming\nb) Flow diagram\nc) Tree diagram\nd) Scatter diagram"
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.8162597,"math_prob":0.9765079,"size":1466,"snap":"2023-14-2023-23","text_gpt3_token_len":460,"char_repetition_ratio":0.103283174,"word_repetition_ratio":0.014814815,"special_character_ratio":0.34515688,"punctuation_ratio":0.18309858,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9796257,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-06-03T21:38:54Z\",\"WARC-Record-ID\":\"<urn:uuid:672141cb-c35b-44cb-8f96-c74cc6c8d1f5>\",\"Content-Length\":\"90559\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c041426d-9472-4364-a3e1-eabf1e319703>\",\"WARC-Concurrent-To\":\"<urn:uuid:aab9e864-4749-4d31-8fd4-ac776d7f7a42>\",\"WARC-IP-Address\":\"192.0.78.13\",\"WARC-Target-URI\":\"https://aniruddhakaushik.wordpress.com/2021/12/03/kt-46-self-evaluation-ncqc-2019/\",\"WARC-Payload-Digest\":\"sha1:LDICTFZOP3AQGHZSR2IFPZFJXRHUEDUA\",\"WARC-Block-Digest\":\"sha1:IA3ESPEV2OG4MCJT65TBYPRZ2K6MRJKQ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-23/CC-MAIN-2023-23_segments_1685224649343.34_warc_CC-MAIN-20230603201228-20230603231228-00583.warc.gz\"}"} |
https://ovid.cs.depaul.edu/Classes/CS202-S07/hw2.htm | [
"Homework 2 (due 4/16) CSC 202\n\nWe finished chapter 1 and started on chapter 2 (2.1-2.3 and 2.5). Next week we will finish chapter 2 and start talking about relations and first-order logic. I suggest you read through Sections 2.1-2.3 carefully, since it contains several additional examples and exercises (some with solutions).\n\nSubmission: you can submit the homework to me either by hardcopy in class or email it to me.\n\n1. [Check Constraints] Write complete ALTER TABLE commands for the following check constraints (see Section 1.4). Also, for each check constraint write an INSERT statement that violates the constraint. (Double-check by running them on the database.)\n\n1. [10pt] The career in Student is one of the following: GRD, UGRD, SAL. Hint: here is what the SQL for adding the constraint will look like:\nALTER TABLE Student\nCHECK ( ... );\n1. [15pt] All IT courses are undergraduate courses (that is, their course number is less than 420 (this is a bit tricky; think about it carefully: what are you trying to exclude? Make sure you test your constraint with examples).\n\n2. [Set Theory, 10pt] True of False? If true, give a proof, if false, find sets A, B, C that show that it is false:\n\nA n (B u C) = (A n B) u C, for all sets A, B, C.\n\n(u is union, n is intersection).\n\n3. [Programming Logic, 15pt] Some programming languages (functional languages in particular) contain an if-then-else expression. That is you write\n\nif condition then a else b,\n\nand if condition holds, the value returned will be that of a and if not, the value of b. (In C you could write (a <= b ? a : b) to compute the minimum of a and b.)\n\n1. [5pt] Find the truth-table of the truth-function \"if p then q else r\".\n2. [10pt] Find the disjunctive normal form for \"if p then q else r\".\n\n4. [SQL Queries, 30] For each SQL query, please submit your SQL and a printout of the resulting table. Be careful writing both of these, and make sure you double-check that your output is what you expect it to be.\n\n1. [15pt] List student groups which have both Chicago and non-Chicago members (HerCTI is the only such group in our database).\n2. [15pt] List students that are not presidents of any student society.\n\n5. [Extra Credit] You have five jars of quarters. One jar contains all counterfeit quarters, the remaining jars contain good quarters only. The counterfeit quarters are 5 grams each, the real quarters 6 grams. You also have a scale. You can pick any number of coins from the jars and make one weighing on the scale. How do you determine which jar contains the counterfeit quarters?\n\n6. [Extra Credit] Show that every truth-function can be written using just logical nand (see Section 1.5 for definition of nand). Hint: show that negation and logical and can be expressed just using nand.\n\n7. [Extra Credit] An old English nursery rhyme goes as follows:\n\nFor want of a nail the shoe was lost.\nFor want of a shoe the horse was lost.\nFor want of a horse the rider was lost.\nFor want of a rider the battle was lost.\nFor want of a battle the kingdom was lost.\nAnd all for the want of a horseshoe nail.\n\nWhat is the logical structure of this nursery rhyme? Introduce appropriate atomic propositions (one for each object), and then use these propositions to describe the statements in the rhyme.\n\n8. [Extra Credit] If you find any typos and mistakes in the lecture notes, please let me know.\n\nMarcus Schaefer\nLast updated: April 10h, 2007."
] | [
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https://blogs.agu.org/martianchronicles/2009/07/10/solar-system-creator/ | [
"10 July 2009\n\n## Solar System Creator\n\nPosted by Ryan Anderson\n\nAs I mentioned last month, on top of research and grad school duties, I’m in the process of planning out a sci-fi novel. It began with the month-long outlining challenge “Midsommer Madness” over at the Liberty Hall writing site, and I am continuing with it in my spare time.\n\nI am trying to make my novel grounded in reality whenever possible. It is set in a known star system, 55 Cancri. The 55 Cancri system has 5 known planets, but I also took some artistic license and added moons and small planets that observations would likely have missed. Then, once I had planets and moons, I needed to figure out which ones would be habitable!",
null,
"I happen to know a thing or two about planets, so I put together a handy spreadsheet to use to calculate things like surface temperature, surface gravity and orbital period given things like how bright the star is, how far away the planet is, etc. Once I had the spreadsheet made, I realized that there are likely other people out there who might find it useful.\n\nSo, whether you are a writer trying to come up with a plausible setting for your bestselling sci-fi epic, or a student learning about the solar system, or just plain curious about planets, please feel free to use and modify this spreadsheet. Right now it is set up for our solar system to give you an idea of what reasonable values are for the different variables, and to show that the results are generally pretty good despite the simplicity of the calculations. If you find this useful or have any questions, feel free to contact me by leaving a comment on this post.\n\nI described how I calculated the surface temperature below. You don’t need to read the explanation to use the spreadsheet: it should just work if you enter numbers, but I encourage you to try to follow the derivation. Even if you don’t follow the algebra, I tried to explain everything in words to give some conceptual understanding of the ideas behind the math, and the ideas are what matter.\n\nNote for Students: The spreadsheet is free for you to use, but be sure you cite this page as a source. Also show your work for all calculations! Copying values from the spreadsheet without showing your work probably won’t earn you any points, and may be considered plagiarism, which is grounds for failure and/or expulsion at most schools. And really, it’s not that hard to do the calculations, especially since the rest of this post is spent walking you through them! You might even learn something!\n\nOk, so how does it work? Well, the calculation of a planet’s surface temperature is based on the very simple idea that if its average temperature is not changing, then the amount of energy the planet absorbs must match the amount that it emits. Pretty much common sense! If the amount in and out were different, then the temperature would change until they balanced!\n\nFirst, the absorption. The energy source is the star, which has a certain luminosity $latex L$ (given in watts). This says how much energy the star puts out in all directions per second. We want to know how much energy per square meter hits the planet, so we take the luminosity and spread it out evenly over the surface of a sphere with a radius $latex R$ equal to the distance from the planet to the star. The surface area of a sphere is $latex A=4\\pi R^2$, so the amount of energy from the star hitting each square meter of the planet’s cross section is: $latex L/A=\\dfrac{L}{4\\pi R^2}$\n\nThe planet’s cross section is just the area of a circle with the planet’s radius: $latex \\pi r^2$. Note that we’re using the area of a circle and not a sphere! That’s because the starlight doesn’t hit the whole planet, it just hits the part of the planet that is visible. Can you see all sides of a sphere at once? Neither can I, and neither can the star. What we see is the 2 dimensional cross section: a circle.\n\nSo now we have an equation for how much energy the planet absorbs per second: $latex Energy Absorbed Per Second= \\dfrac{L \\pi r^2}{4\\pi R^2}$\n\nBut that is assuming that the planet absorbs every bit of light that hits it, which we know isn’t true: we see planets in the night sky by their reflected light! So we can add a correction called albedo. Albedo, $latex A$, is the fraction of starlight that the planet reflects back out into space, and $latex (1-A)$ is the fraction of starlight a planet absorbs. So with that correction, our equation becomes: $latex Energy Absorbed Per Second= \\dfrac{(1-A) L \\pi r^2}{4\\pi R^2}$\n\nNow we have to figure out an expression for the energy that the planet emits. Here we have to make an assumption to simplify things: we assume that the energy absorbed by the planet is immediately redistributed evenly over the whole planet. Obviously this isn’t right, it is much warmer on the day side than the night side, but this assumption makes our lifes much easier. We just have to remember that the value we get is going to be an average of day and night temperatures.\n\nWe also assume that the planet radiates away its energy like a blackbody. A blackbody is something that absorbs and emits all radiation perfectly. We’re not going to worry too much about this assumption. For our purposes, planets are close enough to being blackbodies that it doesn’t matter much. I know, I know, we just made an adjustment for albedo two paragraphs ago, implying that the planet is not a perfect blackbody! Just calm down. It works pretty well, and that’s all we need.\n\nAnyway, if we assume the planet is a uniform temperature blackbody, then we can use the handy equation for blackbody emission: $latex Energy Emitted Per Square Meter Per Second = \\sigma T^4$. Sigma is called the Stefan-Boltzmann constant, and is given by $latex \\sigma = 5.67\\times 10^{-8} W m^{-2} K^{-4}$ To get rid of that pesky “per square meter” part of the equation, we just multiply by the surface area of the thing doing the emitting: in this case, the planet. Here we do use the surface area of a sphere, remember our assumption that the energy absorbed gets spread out over the whole surface? This is why we did that. The result is:\n\n$latex Energy Emitted Per Second = 4 \\pi r^2 \\sigma T^4$\n\nNow that’s a fine equation if your planet emits every bit of energy that it receives straight back to space. But that’s not how it works for planets with atmospheres. There’s this effect where the atmosphere traps energy in the system for a longer time, resulting in a warmer planet… you may have heard of it: the Greenhouse Effect! It would be nice if we could add that to our model! If we don’t, we’ll never get the surface temperature right for a planet like Venus, where the greenhouse effect dominates.",
null,
"To actually do a proper simulation of the greenhouse effect is very difficult and complicated, so instead we are going to use a fudge factor. The bottom line is that the greenhouse effect $latex GE$ reduces the amount of energy radiated from the surface that escapes to space. So we can do something very similar to our albedo adjustment: $latex GE$ gives the amount of energy that the atmosphere absorbs, and $latex 1-GE$ gives the amount of energy that actually escapes to space. For the Earth $latex GE \\approx 0.4$ and for Venus $latex GE \\approx 0.99$. Our modified equation is now:\n\n$latex Energy Emitted Per Second = (1-GE) 4 \\pi r^2 \\sigma T^4$\n\nNow, remember why we were doing all of this? We want to find the planet’s average surface temperature $latex T$. To get this, we have to set our two equations equal to each other and solve:\n\n$latex Energy Emitted Per Second = Energy Absorbed Per Second$\n\n$latex (1-GE) 4 \\pi r^2 \\sigma T^4 = \\dfrac{(1-A) L \\pi r^2}{4\\pi R^2}$\n\nLook! The planet’s radius appears on both sides of the equation! That means it cancels out, and that a planet’s radius has no effect on its surface temperature! Ok, don’t get too excited, we still need to solve for T.\n\n$latex T^4 = \\dfrac{L (1-A)}{16\\sigma\\pi R^{2}(1-GE)}$\n\n$latex T = \\left(\\dfrac{L (1-A)}{16\\sigma\\pi R^{2}(1-GE)}\\right)^{1/4}$\n\nVoila! There is the expression for the equilibrium surface temperature of a planet, taking into account the planet’s reflectivity and the greenhouse effect. I hope this sheds a little light into how to think about the energy budget of a planet, and how my spreadsheet works. Again, if you have any questions, post them in the comments and I’ll answer them!"
] | [
null,
"http://upload.wikimedia.org/wikipedia/commons/5/59/Extrasolar_planet_NASA2.jpg",
null,
"https://blogs.agu.org/martianchronicles/files/2009/07/gheffect.gif",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9246376,"math_prob":0.97174406,"size":10408,"snap":"2020-45-2020-50","text_gpt3_token_len":2415,"char_repetition_ratio":0.13043061,"word_repetition_ratio":0.011950027,"special_character_ratio":0.22818986,"punctuation_ratio":0.09390981,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9933194,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,4,null,4,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-11-30T11:01:05Z\",\"WARC-Record-ID\":\"<urn:uuid:1f91643f-5194-49b1-bfab-4eb99c044f22>\",\"Content-Length\":\"84114\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c0c0cbc6-06fb-4f73-9b46-3fe93b88b56c>\",\"WARC-Concurrent-To\":\"<urn:uuid:959377f3-60b6-4491-be85-2f4b24913333>\",\"WARC-IP-Address\":\"141.193.213.20\",\"WARC-Target-URI\":\"https://blogs.agu.org/martianchronicles/2009/07/10/solar-system-creator/\",\"WARC-Payload-Digest\":\"sha1:UCVOBNEWGRGRUZ6GSR3VPWSYYCDAGLOC\",\"WARC-Block-Digest\":\"sha1:ZHVE6DFNGCVVIXS5MGHRAEMLRDGXPNQH\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-50/CC-MAIN-2020-50_segments_1606141213431.41_warc_CC-MAIN-20201130100208-20201130130208-00151.warc.gz\"}"} |
https://file.scirp.org/xml/82453.xml | [
"Introduction: We have previously developed an effective atomic number ( Z eff ) measurement method using linear attenuation coefficients (LACs) obtained by energy-resolved computed tomography (CT) with one-dimensional (1D) detector. The energy-resolved CT was performed with a “transXend” detector, which measured X-rays as electric current and then gave X-ray energy distribution with unfolding analysis using pre-estimated response function (RF). The purpose of this study is to measure Z eff by the energy-resolved CT using a flat panel detector (FPD). Methods: To demonstrate a 2D transXend detector, we developed the stripe absorbers for the FPD. Eleven human tissue-equivalent material rods which were grouped into four material categories were measured by X-rays with 120 kVp tube voltage, 2.3 mA tube current, and 1.0 s exposure time. Z eff is measured by the ratio of LACs with two different pseudo-monochromatic X-ray energies. RFs of each rod material were estimated by numerical calculation. First, we employed the RF estimated for the same rod material (self-RF scenario). Second, we employed the RF estimated for the different rod materials in the same material category (cross-RF scenario). The purpose of the cross-RF scenario was to find representative rod materials in each material category. Results: Upon the self-RF scenario, measured Z eff s were systematically underestimated. Median relative error to theoretical Z eff was - 6.92% (range: - 7.89% - - 4.60%). After normalizing measured Z eff s to the theoretical one for Breast, median relative error improved to - 0.75% (range: - 1.79% - +1.73%). Upon the cross-RF scenario, the representative rod materials were found in two material categories. Conclusion: Z eff measurements were performed by energy-resolved CT using 2D transXend detector with numerically-estimated RF data. Normalized Z eff s for all rod materials in the self-RF scenario were in good agreement with the theoretical ones.\n\nX-Ray Computed Tomography Energy Resolved Unfolding Effective Atomic Number\n1. Introduction\n\nIn photon and particle radiation therapy treatment planning, single-energy computed tomography (CT) image is commonly used to distinguish materials inside a patient body and to calculate absorbed doses. A CT image is a distribution of linear attenuation coefficient (LAC) of each pixel. To calculate the dose in the patient body, LACs are converted to corresponding mass densities using a conversion table. However, estimated LACs for each pixel can be different from true LACs due to the beam-hardening effect: when polychromatic X-rays pass through a subject, the effective energy of X-rays increases because of the absorption of low energy X-rays. Also, estimated LACs of different materials would be similar and hard to distinguish in single-energy CT image. Thus, a mis-assignment of mass density may occur in single-energy CT measurement.\n\nTo make the dose calculation accurately, a Monte Carlo method has been implemented . If the mis-assignment of mass density due to the beam-hardening effect happened, it can lead to significant dose errors: up to 10% error for 6 - 15 megavoltage (MV) photons . Recently, an effective atomic number (Zeff) attracts attention as an alternative value to LAC.\n\nCommonly, Zeff measurement is performed by the use of LACs measured by X-rays with two different energies. Thus, the use of synchrotron facilities where can generate monochromatic X-ray is one of the best methods for Zeff measurement . However, synchrotrons are too large to install in general hospitals. Alternative methods are a photon-counting CT or a fast kVp switching dual-energy CT. Photon-counting CT uses X-ray detectors which can measure the energy of X-ray. However, photon-counting CT has a limitation in counting rate which is less than 0.5 × 106 s−1 in general . Typical number of X-rays coming into a detector in clinical practice is 109 mm−2・s−1 when they pass the air only and 106 mm−2・s−1 when they pass a thick body . In this stage, photon-counting CT is not practical in view of counting rate problem. Fast kVp switching dual-energy CT requires two projection data on each measurement direction with switching high and low voltages within 10 ms . Two transmission measurements are performed by X-rays with two different averaged energies. The difference between the two averaged energies is, however, not very large: with 80 and 140 kVp, the typical averaged energies at the exit of X-ray tube are 41.4 and 58.9 keV, respectively. According to the transmission direction of a human body, the averaged energy changes and results in beam-hardening artifact in CT image.\n\nTo overcome the problems associated with photon-counting CT and dual- energy CT, we have proposed a novel energy-resolved CT by using a transXend detector . The schematic drawing of the transXend detector is shown in Figure 1 of . The transXend detector consists of several segmented detectors aligned in the X-ray incident direction and measures X-rays as electric currents. The X-ray energy distribution is given after analysis using pre-estimated response function (RF). The transXend detector gives photon numbers in arbitrary energy ranges. Since X-rays are measured as electric currents by the transXend detector, there are no problems associated with the counting rate. This transXend detector collects transmission data of an object under study by repeating rotation and transverse movements. Thus, we called this detector the one-dimensional (1D) transXend detector. Yamashita et al. reported that Zeff of aluminum was measured within 1% error, where the error was defined as (Zeff − Z)/Z . Kanno et al. also reported that relative error of measured Zeffs of water and acrylic were within 3% . Both studies were performed by the 1D transXend detector.\n\nFor the application of two-dimensional (2D) transXend detector for clinical practice in the future, the authors invented stripe absorbers which are placed in front of a flat panel detector (FPD) . The stripe absorbers consist of two kinds of metal ribbons and provides four different X-ray energy spectra. Kanno et al. reported the possibility of 2D transXend detector using a thermo-lumine- scent plate .\n\nAs mentioned above, Zeff measurements for aluminum, acrylic, and water using the 1D transXend detector were conducted previously. In this study, we performed Zeff measurements for eleven human tissue-equivalent materials by the energy-resolved CT using the 2D transXend detector with a FPD. The eleven materials were grouped into four material categories: LUNG, SOFT TISSUE,\n\nSOFT BONE, and BONE. Zeffs were measured by using the RFs estimated under two different scenarios: With RFs estimated for the same materials with the one used for CT measurements, or with RFs estimated for different materials in each material category.\n\n2. Materials and Methods 2.1. Theory of an Effective Atomic Number Measurement\n\nSpiers et al. proposed the definition of Zeff for considering the X-ray absorption by human tissue :\n\nZ eff = ∑ k α k Z k 2.94 2.94 , (1)\n\nwhere αk is the electron number fraction, and Zk is the atomic number of element k.\n\nTorikoshi et al. showed the measurement of Zeff with two different monochromatic X-ray energies using a synchrotron facility . In the energy range for X-ray CT, 80 - 140 keV, the X-ray LAC of element Z for monochromatic energy E can be written as\n\nμ ( E ) = ρ e { Z 4 F ( E , Z ) + G ( E , Z ) } . (2)\n\nHere ρe is the electron density, ρeZ4F(E,Z) is the photoelectric term, and ρeG(E,Z) is the scattering term. Thus, atomic number Z can be described by the ratio of LAC:\n\nf ( Z ) = μ ( E a ) / μ ( E b ) . (3)\n\nSince the LAC of elements are summarized as a function of X-ray energy in the table of the National Institute of Standards and Technology (NIST), the term f(Z) can be drawn by plotting the value of μ(Ea)/μ(Eb) as a function of Z . Therefore, the Zeff can be obtained by using the Equation (3) with measuring LACs at two different X-ray energies Ea and Eb. Since a CT image is the distribution of LAC, the ratio can be obtained by dividing two CT images which were acquired by two different monochromatic X-ray energies Ea and Eb.\n\n2.2. The Relationship between the Measured Currents and X-Ray Energy Distribution\n\nWhen the transXend detector is used for X-ray transmission measurement, the relationship between the measured electric currents and the X-ray energy distribution is expressed in terms of following matrix equation :\n\n( I 1 I 2 ⋮ I m ) = ( R 1 , 1 R 1 , 2 ⋯ R 1 , n R 2 , 1 R 2 , 2 ⋮ ⋮ ⋱ R m , 1 ⋯ R m , n ) ( Y 1 Y 2 ⋮ Y n ) . (4)\n\nHere Ii (i = 1, m) is the electric current value measured by i-th segmented detector, Yj (j = 1, n) is the number of X-rays in the energy range Ej , and Ri,j is the RF of the i-th segment detector in the energy range Ej. The X-ray energy distribution is obtained by solving Equation (4) using an unfolding code, such as SAND II . In the unfolding process, the number of energy ranges and the widths of energy ranges can be assigned according to the materials of interest. More detailed information is described in elsewhere .\n\n2.3. Two-Dimensional transXend Detector\n\nFor the clinical application of the transXend detector, a 2D transXend detector should be developed. To make the transXend detector system two-dimensional, we used a FPD and stripe absorbers which consist of two different absorbers A and B in a lattice shape, as shown in Figure 1 . With the stripe absorbers placed in front of the FPD, four different regions, (a)-(d), can be made, as shown in Figure 1. In region (a), X-rays enter to the FPD without passing two absorbers. Subsequently, in region (b), (c), and (d), X-rays passed through the absorber A, B, and A + B, respectively. We used 1 mm-wide and 0.1-mm-thick tin and copper for absorber A and B, respectively. Calculated X-ray spectra arriving at FPD pixels in each region are shown in Figure 2. Considering the four regions as one pixel, each region has the role of segmented detectors. X-ray energy distribution can be acquired for the 2D position on the FPD by unfolding electric currents measured by the four regions. The employed FPD was Remote RadEye2 (Teledyne Rad-icon Imaging, Sunnydale, CA, USA) with pixel matrix of 1024 × 1024 pixel2 (active area 49.3 × 49.2 mm2). The pixel size of photodiode was 48 × 48 μm2. Incident X-ray photons are absorbed by a Gd2O2S scintillator plate and scintillation photons are detected by a 2D CMOS photodiode array.\n\n2.4. Human Tissue-Equivalent Materials\n\nEleven RMI rods (Gammex, Middleton, WI, US) were used in this study, as summarized in Table 1. Diameter and height of each rod was 28 mm and 70 mm, respectively. RMI rods were often used as the calibration materials of CT\n\nCharacteristics for RMI rods\nMaterial category Rod material Relative electron density Mass density [g/cm3] Theoretical effective atomic number\nLUNG LN300 0.29 0.29 7.86\nLN450 0.45 0.46 7.84\nSOFT TISSUE Adipose 0.92 0.94 6.40\nBreast 0.96 0.98 7.24\nSolid water 0.99 1.02 8.11\nBrain 1.05 1.05 6.31\nSOFT BONE Inner bone 1.10 1.14 10.9\nBone mineral 1.11 1.15 10.9\nBONE CB2-30% 1.28 1.33 11.4\nCB2-50% 1.47 1.56 13.0\nCortical bone 1.70 1.82 14.1\n\nnumber―mass density conversion table for the dose distribution calculation in radiotherapy treatment planning. In such calibration, each rod was inserted to a 330-mm-diameter and 50-mm-height RMI phantom and all rods were scanned simultaneously. In this study, however, each rod was scanned individually to measure its Zeff for avoiding the fan-beam effect.\n\n2.5. Experiment\n\nExperimental set up was shown in Figure 3. As described in the previous paper, RF measurement for the phantom material was necessary prior to CT measurement . Used materials for RF measurement were the same ones with the phantom for CT measurement: slabs of different thicknesses were prepared for each material in the phantom. We, however, transmission data for the RF estimation by a numerical calculation using Lambert-Beer’s law since each rod was uniform:\n\nI = I 0 exp ( − μ t ) . (5)\n\nHere I is photon number transmitted through a material with LAC, μ, with thickness t, I0 is incident photon number. Transmission data was calculated for each rod material with thicknesses ranging from 0 to 30 mm at intervals of 5 mm. I0 was normalized to the measured current induced by X-rays which passed the air only. In transXend analysis, RF data was interpolated by 1 mm interval. Scatter X-rays were not considered in the calculation.\n\nAfter calculating transmission data for the RF estimation, each rod was scanned from one direction by the X-rays. Employed X-ray tube was ERESCO MF4 (GE Sensing & Inspection Technologies, Ahrensburg, Germany) with a tungsten target and built-in filters made from 0.8-mm-thick beryllium and 2-mm-thick aluminum. The X-ray tube was placed 1000 mm away from the FPD. The X-ray tube operating conditions were 120 kV for tube voltage, 2.3 mA\n\nfor tube current, and 1 s for exposure time. Since each rod was axial symmetry, projection data for each rod was duplicated 359 times to make 1˚ step data. Source-to-axis of the phantom distance was 850 mm.\n\nSix energy ranges were defined for obtaining X-ray energy distribution, as shown in Table 2. Since almost no X-rays with the energy under 15.0 keV entered into the FPD, those X-rays were excluded from the analysis. The X-rays in the energy range E2: 35.0 - 36.0 keV and E5: 65.0 - 66.0 keV were used as pseudo-monochromatic X-rays. Measured currents in the center column of the FPD were unfolded by SAND II code to obtain energy distributions. Number of X-rays in each energy ranges were estimated for each projection. With Y2 and Y5, CT images were reconstructed by maximum likelihood-expectation maximization method . Iterative number was 30 times which was optimized prior to the measurements. With the LAC data table of NIST, Z-μ(E2)/μ(E5) relationship can be drawn as Figure 4. CT images of μ(E2) and μ(E5) for each rod were converted to a Zeff image using Figure 4.\n\nIn previous studies , the RF was estimated by using the same material with the one of phantom for CT measurement. In this study, we demonstrated two different analysis scenarios. In the first scenario, we employed the RF estimated for the same material as the one of the phantom for CT measurement (self-RF scenario). In the second scenario, we employed the RF estimated for the different material than the one of the phantom for CT measurement (cross-RF scenario). The purpose of the cross-RF scenario was to determine the representative rod materials in each material category. Reduction of the number of materials for RF estimation would widen the application of energy-resolved CT using 2D transXend detector. Mean and standard deviation (SD) of Zeff for each rod material was calculated in 10 × 10 mm2 region-of-interest on Zeff image.\n\nAssigned energy ranges. Unit: [keV]\nReferences Chetty, I.J., Curran, B., Cygler, J.E., De Marco, J.J., Ezzell, G., Faddegon, B.A., et al. (2007) Report of the AAPM Task Group No. 105: Issues Associated with Clinical Implementation of Monte Carlo-Based Photon and Electron External Beam Treatment Planning. Medical Physics, 34, 4818-4853. https://doi.org/10.1118/1.2795842 Verhaegen, F. and Devic, S. (2005) Sensitivity Study for CT Image Use in Monte Carlo Treatment Planning. Physics in Medicine & Biology, 50, 937-946. https://doi.org/10.1088/0031-9155/50/5/016 Toriloshi, M., Tsunoo, T., Sasaki, M., Endo, M., Noda, Y., Ohno, Y., et al. (2003) Electron Density Measurement with Dual-Energy X-ray CT Using Synchrotron Radiation. Physics in Medicine & Biology, 48, 673-685. https://doi.org/10.1088/0031-9155/48/5/308 Taguchi, K., Frey, E., Wang, X., Iwanczyk, J. and Barber, W. (2010) An Analytical Model of the Effects of Pulse Pileup on the Energy Spectrum Recorded by Energy Resolved Photon Counting X-Ray Detectors. Medical Physics, 37, 3957-3969. https://doi.org/10.1118/1.3429056 Yu, L., Leng, S. and McCollough, C.H. (2012) Dual-Energy CT-Based Monochromatic Imaging. American Journal of Roentgenology, 199, S9-S15. https://doi.org/10.2214/AJR.12.9121 Xu, C., Danielsson, M., Karlsson, S., Svensson, C. and Bornefalk, H. (2012) Preliminary Evaluation of a Silicon Strip Detector for Photon-Counting Spectral CT. Nuclear Instruments and Methods in Physics Research Section A, 677, 45-51. https://doi.org/10.1016/j.nima.2012.02.034 Kanno, I., Imamura, R., Mikami, K., Uesaka, A., Hashimoto, M., Phtaka, M., et al. (2008) A Current Mode Detector for Unfolding X-Ray Energy Distribution. Journal of Nuclear Science and Technology, 45, 1165-1170. https://doi.org/10.1080/18811248.2008.9711905 Yamashita, Y., Kimura, M., Hamaguchi, T., Kanno, I., Ohtaka, M., Hashimoto, M., et al. (2014) Measurement of Effective Atomic Numbers using Energy-Resolved Computed Tomography. Journal of Nuclear Science and Technology, 51, 1256-1263. https://doi.org/10.1080/00223131.2014.919881 Kanno, I., Yamashita, Y., Kimura, M. and Inoue, F. (2015) Effective Atomic Number Measurement with Energy-Resolved Computed Tomography. Nuclear Instruments and Methods in Physics Research Section A, 787, 121-124. https://doi.org/10.1016/j.nima.2014.11.072 Kanno, I., Yamauchi, K. and Hamaguchi, T. (2016) Two-Dimensional “transXend” Detector with Band Structure Absorbers for Third-Generation Energy-Resolved Computed Tomography with Improved Spatial Resolution. Journal of Nuclear Science and Technology, 54, 22-29. https://doi.org/10.1080/00223131.2016.1202154 Kanno, I., Yamashita, Y., Kanai, E., Ogawa, T. and Shinsho, K. (2016) Two-Dimensional “TransXend” Detector for Third Generation Energy-Resolved Computed Tomography. Journal of Nuclear Science and Technology, 53, 258-262.https://doi.org/10.1080/00223131.2015.1037810 Spiers, F.W. (1946) Effective Atomic Number and Energy in Tissues. The British Journal of Radiology, 19, 52-63. https://doi.org/10.1259/0007-1285-19-218-52 Hubbell, J.H. and Seltzer, S.M. (2010) Tables of X-Ray Mass Attenuation Coefficients and Mass Energy-Absorption Coefficients from 1 keV to 20 MeV for Elements Z = 1 to 92 and 48 Additional Substances of Dosimetric Interest. The Physical Measurement Laboratory, The National Institute of Standards and Technology, Gaithersburg, MD. https://www.nist.gov/pml/x-ray-mass-attenuation-coefficients McElroy, W., Berg, S., Crockes, T. and Hawkins, G.A. (1967) Computer-Automated Iterative Method for Neutron Fux Spectra Determination by Foil Activation. AFWL-TR-67-41. Air Force Weapons Laboratory, Albuqueque, NM. Imamura, R., Mikami, K., Minami, Y., Kanno, I., Ohtaka, M., Hashimoto, M., et al. (2010) Unfolding Method with X-Ray Path Length-Dependent Response Functions for Computed Tomography Using X-Ray Energy Information. Journal of Nuclear Science and Technology, 47, 1075-1082. https://doi.org/10.1080/18811248.2010.9711672 Shepp, L.A. and Vardi, Y. (1982) Maximum Likelihood Reconstruction for Emission Tomography. IEEE Transactions on Medical Imaging, 1, 113-122.https://doi.org/10.1109/TMI.1982.4307558 Bazalova, M., Carrier, J.F., Beaulieu, L. and Varhaegen, F. (2008) Dual-Energy CT-Based Material Extraction for Tissue Segmentation in Monte Carlo Dose Calculations. Physics in Medicine & Biology, 53, 2439-2456.https://doi.org/10.1088/0031-9155/53/9/015 Goodsitt, M.M., Christodoulou, E.G. and Larson, S.C. (2011) Accuracies of the Synthesized Monochromatic CT Numbers and Effective Atomic Numbers Obtained with a Rapid kVp Switching Dual Energy CT Scanner. Medical Physics, 38, 2222-2232. https://doi.org/10.1118/1.3567509 Papanikolaou, N., Battista, J.J., Kappas, C., Klein, E., Mackie, T.R., Sharpe, M., et al. (2004) Tissue Inhomogeneity Corrections for Megavoltage Photon Beams. AAPM Report No. 65, 1-142. Tsai, T.S. and Kanno, I. (2016) A Simulation Study on the Influence of Scattered X-Rays in Energy-Resolved Computed Tomography. Journal of Nuclear Science and Technology, 54, 205-212. https://doi.org/10.1080/00223131.2016.1236709 Maruyama, Y., Hamaguchi, T., Tsai, T.S. and Kanno, I. (2017) Response Function Estimation with Fine Energy Bins for the Energy-Resolved Computed Tomography Using a TransXend Detector. Journal of Nuclear Science and Technology, 55, 199-208. https://doi.org/10.1080/00223131.2017.1389311"
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https://www.grc.nasa.gov/WWW/K-12/rocket/newton.html | [
"",
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"+ Text Only Site\n+ Non-Flash Version\n+ Contact Glenn",
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"The motion of a rocket from the surface of the Earth to a landing on the Moon can be explained and described by physical principals discovered over 300 years ago by Sir Isaac Newton. Newton worked in many areas of mathematics and physics. He developed the theories of gravitation in 1666, when he was only 23 years old. Some twenty years later, in 1686, he presented his three laws of motion in the \"Principia Mathematica Philosophiae Naturalis.\" The laws are shown above, and the application of these laws to rockets is given on separate slides. Newton's first law states that every object remains at rest or in uniform motion in a straight line unless compelled to change its state by the action of an external force. This is normally taken as the definition of inertia. The key point here is that if there is no net force acting on an object (if all the external forces cancel each other out) then the object maintains a constant velocity. If that velocity is zero, then the object remains at rest. If the velocity is not zero, then the object maintains that velocity and travels in a straight line. If a net external force is applied, the velocity changes because of the force. Velocity is a vector quantity, having both a magnitude and a direction. The change in velocity caused by a force may involve the magnitude, the direction, or both, depending on the magnitude and direction of the force, which is also a vector quantity. The second law explains how the velocity of an object changes when it is subjected to an external force. The law defines a force to be equal to change in momentum (mass times velocity) per change in time. Newton also developed the calculus of mathematics, and the \"changes\" expressed in the second law are most accurately defined in differential forms. Calculus can also be used to determine the velocity and location variations experienced by an object subjected to an external force. For an object with a constant mass m, the second law states that the force F is the product of an object's mass and its acceleration a: F = m * a For an object like a rocket, with a large change in mass during the flight, we must use the more accurate definition of the second law associated with the change in momentum. For an external applied force, the change in velocity depends on the mass of the object. A force causes a change in velocity; and likewise, a change in velocity generates a force. The equation works both ways. The third law states that for every action (force) in nature there is an equal and opposite re-action. In other words, if object A exerts a force on object B, then object B also exerts an equal force on object A. Notice that the forces are exerted on different objects. The third law can be used to explain the generation of thrust by a rocket engine. Guided Tours",
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"Newton's Laws of Motion:",
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"Activities: Fundamental Terminology: Grade 10-12 Hero Engine: Grade 6-10 Related Sites: Rocket Index Rocket Home Beginner's Guide Home",
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"+ Inspector General Hotline + Equal Employment Opportunity Data Posted Pursuant to the No Fear Act + Budgets, Strategic Plans and Accountability Reports + Freedom of Information Act + The President's Management Agenda + NASA Privacy Statement, Disclaimer, and Accessibility Certification",
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"Editor: Tom Benson NASA Official: Tom Benson Last Updated: Jun 12 2014 + Contact Glenn"
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https://www.univerkov.com/the-perimeter-of-the-rectangle-is-36-cm-the-sum-of-the-lengths-of-its-three-sides-is-25-cm-what-is-the-area-of-this-rectangle-3/ | [
"# The perimeter of the rectangle is 36 cm. The sum of the lengths of its three sides is 25 cm. What is the area of this rectangle?\n\nLet us denote the lengths of the sides of this rectangle through x and y.\n\nAccording to the condition of the problem, the perimeter of this rectangle is 36 cm, therefore, we can write the following relationship:\n\n2 * (x + y) = 36.\n\nIt is also known that the sum of the lengths of the three sides of this rectangle is 25 cm, therefore, we can write the following ratio:\n\nx + y + x = 25.\n\nWe solve the resulting system of equations.\n\nSubtracting the second equation from the first, we get:\n\n2 * (x + y) – 2x – y = 36 – 25;\n\n2x + 2y – 2x – y = 11;\n\ny = 11 cm.\n\nSubstituting the found value y = 11 into the equation 2x + y = 25, we get:\n\n2x + 11 = 25;\n\n2x = 25 – 11;\n\n2x = 14;\n\nx = 14/2;\n\nx = 7 cm.\n\nFind the area of the rectangle:\n\n11 * 7 = 77 sq. cm.\n\nAnswer: the area of the rectangle is 77 square meters. cm.",
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"One of the components of a person's success in our time is receiving modern high-quality education, mastering the knowledge, skills and abilities necessary for life in society. A person today needs to study almost all his life, mastering everything new and new, acquiring the necessary professional qualities."
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https://developer.apple.com/documentation/swift/binaryinteger/3126998-ismultiple?changes=_3 | [
"Instance Method\n\n# isMultiple(of:)\n\nReturns `true` if this value is a multiple of the given value, and `false` otherwise.\n\nRequired. Default implementations provided.\n\n## Parameters\n\n`other`\n\nThe value to test.\n\n## Discussion\n\nFor two integers a and b, a is a multiple of b if there exists a third integer q such that a = q*b. For example, 6 is a multiple of 3 because 6 = 2*3. Zero is a multiple of everything because 0 = 0*x for any integer x.\n\nTwo edge cases are worth particular attention:\n\n• `x.isMultiple(of: 0)` is `true` if `x` is zero and `false` otherwise.\n\n• `T.min.isMultiple(of: -1)` is `true` for signed integer `T`, even though the quotient `T.min / -1` isn’t representable in type `T`.\n\n## Default Implementations\n\n### BinaryInteger Implementations\n\n`func isMultiple(of: Self) -> Bool`\n\nReturns `true` if this value is a multiple of the given value, and `false` otherwise.\n\n### SignedInteger Implementations\n\n`func isMultiple(of: Self) -> Bool`\n\nReturns `true` if this value is a multiple of the given value, and `false` otherwise."
] | [
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http://ydec.qudupydih.ru/2019/12/13_med-math-online-calculator.aspx | [
"# Med math online calculator\n\n## Medical Dosage Calculations For Dummies Cheat Sheet\n\nFree online easy calculator for school and business. Calculator for taxes, financial lease calculator, basic car loan calculator and much just enter quantity, current price and tax percentage in our t.Other calculators. Final grade calculator. Pi scientific calculator. skills tutor – online tutor hire for the summer break. Med school gpa. 10 reasons why math is important in life guide + examples.Free math lessons and math homework help from basic math to algebra, geometry and beyond. if your teacher doesn't allow calculators for homework, that means online ones, too.A basic math calculator with additional supporting online math calculators if you need them. in order to access the online calculators you will need a device capable of accessing the internet and runn.Math tools and calculators. Here are some really useful applications to speed your way to that allimportant solution. converts decimals to fractional form, showing steps. Combinations and permutations.Free online dosing calculator allows prescribers to calculate dosing per patient weight. Mdtoolbox provides this free calculator just as a math tool.Algebra calculator shows you the stepbystep solutions! solves algebra problems and walks you through them. algebra calculator. What do you want to calculate?.Maths free online calculators get free algebra calculator, multiplication calculator, addition calculator, conversion calculators, trigonometry calculator, engineering math this is a math solver tool.\n\nlosec mups 40 mg\n\n## MDMath | Canadian Society of Echocardiography\n\nexpress post uk to usa\n\n## Web Calculator Designer - Calculoid.com\n\nDosage calculator. Calculation of the administered activity in mbq and mci and the 2010 north america consensus guideline, eur j nucl med mol imaging.Math calculator from mathway will evaluate various math problems from basic arithmetic to advanced trigonometric expressions. you're welcome! let me take a look you'll be able to enter math.Medicalcalculators provides online calculators for medical and scientific use. Designed drug dosage calculator enter amount of drug you want to give.Practice questions practice your math skills with each of these questions. An explanation will be provided for each answer that is incorrect. If you find these questions useful, click here to sign up f.Medical calculators. Medical science is a branch of science that helps in treating and preventing the diseases that affect human beings. Doctors generally use different tests to diagnose the diseases o.Scientific calculator online and mobile friendly. Creates a series of calculations that can be printed, bookmarked, shared and modified. Keys: pi, e, standard gravity, gas constant, sin, cos, tan, asin.The only fault lies in the name. Perhaps the mathweenienobrainer technique would be more appropriate. At any rate, give dimensional analysis a try. At the end of a 12hour shift, when youre tired, thing.Online clinical calculators. Medcalc: pediatric dosing calculator disclaimer: all calculations must be confirmed before use.Medical calculators. Disclaimer: all calculations must be confirmed before use. The authors make no claims of the accuracy of the information contained herein; and these suggested doses are not a subst.\n\nexpress computers uk\n\n## Online ACFI Calculator | Question 11: Medication\n\nexpress star newspaper wolverhampton uk\n\n## Algebra Calculator - MathPapa\n\nThis is an online scientific calculator with double digit precision that support both button click and keyboard type. In addition, explore hundreds of other free calculators covering topics such as fin.Online calculator for quick calculations, along with a large collection of calculators on math, finance, fitness, and more, each with related calculator. Net's sole focus is to provide fast, compr.Com blog pharmacology med math for nurses master post (everything about dosage calculations and dimensional analysis. With practice) one of the most stressful parts of nursing school is nurs.Prescription. This includes the name of the medication, the dosage and form of the medication, the amount to be taken, the method of administration, and the frequency and duration the medication will b.\n\nmed familjen i london\n\n## Online Math Calculators\n\nThe weight based dose calculator is used for weight based dosing. The parameters for the calculator include dosage, weight, med amount, per volume.+ with help of this calculator you can: find the matrix determinant, the rank, raise the matrix to a power, find the sum and the multiplication of matrices, calculate the inverse matrix. Just type matr.Online math calculator is used to perform a variety of calculations. It is comprised of the forward and back controls which allow you to if you want to erase all data of the previous calculations from.Free online math calculators and converters. Mathematics calculation is made easier. this free online math web site will help you learn mathematics in a easier way. Easycalculation will also help you.Makes learning and applying dosage calculations— even reviewing basic math build the skills that assure patient safety and prevent medication errors.22 мая 2018 г. You will find a med calculator for bmi, creatinine clearance, metric to english conversion and more. You will find over 20 financial calculators.Calculator online. Simple and scientific. With calculation memory. for the purpose of checking your work, mathematical calculations entered into the online calculator can be left displayed on the tape.Here you will find many math calculators. They are free and show steps. Choose subject and use search to find the required solver. all math calculators. Didn't find the calculator you need? reque.This online maths calculator is very similar to the main calculator on the site except for the cool history feature. It lets you see online maths calculator maths calculator math calculator.Math calculator. Thousands maths online. i’m a can’t do math gay and who let me work with spreadsheets and numbers i’m good at my job but i still need the calculator app to do 2+2 to calculate for tip.Medical calculators, criteria sets and decision trees. In this calculator, mcgm is the abbreviation for micrograms. To make simple unit conversions, select the starting units with the pulldown s.General math solvers below, there is a collection of general math solvers and calculators covering issues like the fractions, percentages, factorization, prime numbers, divisibility and square roots.\n\nholiday inn express burton uk\n\n## MDCalc\n\nThis online scientific calculator has a full list of functions that can help you find the solution for any basic or complex math and scientific what are the functions this online scientific calculator.So the volume to give = 27 ml. It doesnt matter what type of units are used in this calculator. You can figure out how many grams to give or how many milligrams to give, microg.Online math calculator find answers for all your math problems in just a click. online math calculator : we people know about classic calculator in which we can use the mathematical operations like ad.This is a free online math calculator together with a variety of other free math calculators that compute standard deviation, percentage, fractions, and time, along with hundreds of other calculators a.Start studying paramedic med math (practice). Learn vocabulary, terms, and more with flashcards, games, and other study tools.Free online scientific notation calculator. Solve advanced problems in physics, mathematics and engineering. Math expression renderer, plots, unit converter, equation solver, complex numbers, calculati.Calculating medication dosage by weight. Medical dosage calculations that consider a patients weight are very common in obese patients and on pediatric wards. Its easy to imagine that the weight of the.Online exclusive. Author information nurses are often intimidated by the math that occurs in everyday practice. Patient safety depends on the follow these four steps to easily calculate your patients a.The dose driven ivdrip rate calculator is based on equation parameters that include desired dose, weight, amount of drug in iv bag, and iv bag volume.The following calculator will find mean, mode, median, lower and upper quartile, interquartile range of the given data set. The calculator will generate a step by step explanation on how to find these."
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.85822964,"math_prob":0.98064184,"size":19725,"snap":"2020-34-2020-40","text_gpt3_token_len":3818,"char_repetition_ratio":0.21616551,"word_repetition_ratio":0.2782398,"special_character_ratio":0.17799747,"punctuation_ratio":0.14948453,"nsfw_num_words":3,"has_unicode_error":false,"math_prob_llama3":0.99229234,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-08-08T08:24:24Z\",\"WARC-Record-ID\":\"<urn:uuid:21538750-f549-47a4-9aaa-e6314adba29b>\",\"Content-Length\":\"23940\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:fcb7fcd1-e3c5-423d-a2c9-e5e1cee253e8>\",\"WARC-Concurrent-To\":\"<urn:uuid:f4cd382d-3337-4049-9964-405f1258c1f9>\",\"WARC-IP-Address\":\"37.46.132.131\",\"WARC-Target-URI\":\"http://ydec.qudupydih.ru/2019/12/13_med-math-online-calculator.aspx\",\"WARC-Payload-Digest\":\"sha1:KQCEOFV5W6KXFD3LLCDHB6HIU77U5DK5\",\"WARC-Block-Digest\":\"sha1:N2KFAMBBDCDVVJXF5KRAWAC364KDIEIP\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-34/CC-MAIN-2020-34_segments_1596439737319.74_warc_CC-MAIN-20200808080642-20200808110642-00007.warc.gz\"}"} |
https://www.daniweb.com/programming/web-development/threads/436646/i-wont-help | [
"``````foreach(\\$search_exploded as \\$search_each)\n{\n@\\$x++;\nif(\\$x==1)\n@\\$construct .=\"keywords LIKE '%\\$search_each%'\";\nelse\n\\$construct .=\"AND keywords LIKE '%\\$search_each%'\";\n\n}\n\ni just wont to understand this foreach (\\$search_exploded as \\$search_each)\nwhat is the meaning\n``````\n\n## All 3 Replies\n\nIt means that for each search for love that exploded in our faces, there is love searching for each of us.\n\nlooks like there should be more code for this. All I can tell you about this so far is that is is;\n- Looping through an array called `\\$search_exploded` placing each value into the variable `\\$search_each`\n- It then adds 1 to `\\$x` (assuming that is was previously defined)\n- It then checks if `\\$x` is equal to 1 (first time through the loop)\n- If it is the first time through the loop it will concatinate `\"keywords LIKE '%\\$search_each%'\"` to the string `\\$construct` (also assuming that `\\$construct` has previously been defined)\n- if not it will concatinate `\"AND keywords LIKE '%\\$search_each%'\"` instead\n\nThe code is not written to clearly, although not required is is always best to use {} with `if` statements.\n\n``````\\$x = 0;\n// the \\$x++ is at the start of the loop so we will need to make its value 0\n// else it will never be evaluated as 1. usually you will put the plus counter\n//at the end of a loop.\n\\$construct = ''; // empty string\nforeach(\\$search_exploded as \\$search_each) {\n\\$x++;\n\nif(\\$x==1) {\n\\$construct .=\"keywords LIKE '%\\$search_each%'\";\n} else {\n\\$construct .=\"AND keywords LIKE '%\\$search_each%'\";\n}\n}\n``````\n``````<?php\n// If\n\\$search_exploded = array('searchValue1','searchValue2','searchValue3'); // this means \\$search_exploded=searchValue1;\\$search_exploded=searchValue2;\\$search_exploded=searchValue3\n\\$construct=\"\";\nforeach(\\$search_exploded as \\$x=>\\$search_each)\n{\n//\\$x -> index of an array; Here 0,1,2\n//\\$search_each -> Value of array ; hear 'searchValue1','searchValue2','searchValue3'\n\\$x++;\nif(\\$x==1)\n\\$construct .=\"keywords LIKE '%\\$search_each%'\";\nelse\n\\$construct .=\" AND keywords LIKE '%\\$search_each%'\";\n}\n\necho \\$construct; // Output is =>keywords LIKE '%searchValue1%' AND keywords LIKE '%searchValue2%' AND keywords LIKE '%searchValue3%'\n?>\n``````\nBe a part of the DaniWeb community\n\nWe're a friendly, industry-focused community of developers, IT pros, digital marketers, and technology enthusiasts meeting, networking, learning, and sharing knowledge."
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.82708454,"math_prob":0.72027254,"size":756,"snap":"2022-40-2023-06","text_gpt3_token_len":189,"char_repetition_ratio":0.12101064,"word_repetition_ratio":0.0,"special_character_ratio":0.25661376,"punctuation_ratio":0.13970588,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9503097,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-02-03T13:12:12Z\",\"WARC-Record-ID\":\"<urn:uuid:a5274584-853f-4ea2-99b1-428be8937409>\",\"Content-Length\":\"76473\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:a886ef55-3522-4f86-ab82-4488e22ce3ae>\",\"WARC-Concurrent-To\":\"<urn:uuid:d7ae4d0b-5946-4ac5-a83d-c0a3f9218e8c>\",\"WARC-IP-Address\":\"172.66.41.5\",\"WARC-Target-URI\":\"https://www.daniweb.com/programming/web-development/threads/436646/i-wont-help\",\"WARC-Payload-Digest\":\"sha1:56INZHZAIAMBWIHX7MKQWLAOZFSMPRIV\",\"WARC-Block-Digest\":\"sha1:46EX57TYROUY4GBTB4IB5WS7IPZ3J2EL\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-06/CC-MAIN-2023-06_segments_1674764500056.55_warc_CC-MAIN-20230203122526-20230203152526-00734.warc.gz\"}"} |
https://virtualnerd.com/pre-algebra/rational-numbers/solve-fraction-equations/solve-one-step-fraction-equations/fraction-multiplication-example | [
"# How Do You Solve an Equation Where You're Multiplying Fractions?\n\n### Note:\n\nSolving an equation with multiple fractions in different forms isn't so bad. This tutorial shows you how to convert a mixed fraction to an improper fraction in order to solve the equation. Then, you'll see how to convert the answer back to a mixed fraction to make sense of it. Follow along with this tutorial to see how it's done!\n\n### Keywords:\n\n• problem\n• equation\n• fraction\n• 1 step solution\n• solve by division\n• division property of equality\n• mixed fraction\n• improper fraction\n• improper\n• mixed\n• solve"
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9335313,"math_prob":0.91816515,"size":2147,"snap":"2023-40-2023-50","text_gpt3_token_len":423,"char_repetition_ratio":0.16752216,"word_repetition_ratio":0.02793296,"special_character_ratio":0.19236143,"punctuation_ratio":0.09950249,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9990788,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-10-03T20:36:14Z\",\"WARC-Record-ID\":\"<urn:uuid:94fa1a47-9b9f-4a35-9307-8df3531ee1ac>\",\"Content-Length\":\"38210\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:bf328a57-a13d-4f49-a2a0-59da2a7f8460>\",\"WARC-Concurrent-To\":\"<urn:uuid:236844e8-5cb1-41ab-819f-f9ec85912a8d>\",\"WARC-IP-Address\":\"99.86.229.71\",\"WARC-Target-URI\":\"https://virtualnerd.com/pre-algebra/rational-numbers/solve-fraction-equations/solve-one-step-fraction-equations/fraction-multiplication-example\",\"WARC-Payload-Digest\":\"sha1:KXORN5K52S64AACR3J25R7DPEXIIY5S7\",\"WARC-Block-Digest\":\"sha1:DTC3LIGJTVPDVKGMJVQSSPK7GR3T52ZY\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233511220.71_warc_CC-MAIN-20231003192425-20231003222425-00337.warc.gz\"}"} |
https://www.rubydoc.info/gems/scbi_plot/0.0.7 | [
"# scbi_plot\n\n## DESCRIPTION:\n\nscbi_plot is a simplified wrapper to create plots with gnuplot.\n\n## FEATURES/PROBLEMS:\n\n• Create histogram plots with numeric or string x axis\n\n• Create line and related plots (linespoints, points, impulses, etc…)\n\n## SYNOPSIS:\n\n### Histogram plot:\n\n``````# create Histogram\np=ScbiPlot::Histogram.new('with_string_axis.png','title')\n\n# generate graph\np.do_graph\n``````\n\n### Line plot:\n\n``````# Create lines plot\np=ScbiPlot::Lines.new('lines.png','title')\n\n# create some random data\nx=[]\ny1=[]\ny2=[]\ny3=[]\n\n10.times do |i|\nx.push i*10\ny1.push i+(rand*50).to_i\ny2.push i+(rand*50).to_i\ny3.push i+(rand*50).to_i\nend\n\n# draw another series with points\n\n# add a third series with impulses of width 4\n\n# add a vertical line at pos 5\n\n# create graph\np.do_graph\n``````\n\n## REQUIREMENTS:\n\n• gnuplot binary\n\n• gnuplot gem\n\n## INSTALL:\n\n• gem install scbi_plot"
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5541406,"math_prob":0.70480835,"size":2139,"snap":"2023-14-2023-23","text_gpt3_token_len":543,"char_repetition_ratio":0.09508197,"word_repetition_ratio":0.0,"special_character_ratio":0.25666198,"punctuation_ratio":0.1800948,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9850775,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-03-25T23:20:04Z\",\"WARC-Record-ID\":\"<urn:uuid:2b724d79-2a37-4a9a-9412-de60539071b1>\",\"Content-Length\":\"14413\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4f031451-88c3-4225-9338-88c77a7b29ac>\",\"WARC-Concurrent-To\":\"<urn:uuid:15d3e442-b058-4877-8078-98749c816ebe>\",\"WARC-IP-Address\":\"172.67.163.155\",\"WARC-Target-URI\":\"https://www.rubydoc.info/gems/scbi_plot/0.0.7\",\"WARC-Payload-Digest\":\"sha1:ZAYK7I57ACUXTABXFNONBN5NYVHCASSY\",\"WARC-Block-Digest\":\"sha1:3KSZHGKCUPEYHT3CYDWKGYKQY374RWH6\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-14/CC-MAIN-2023-14_segments_1679296945376.29_warc_CC-MAIN-20230325222822-20230326012822-00116.warc.gz\"}"} |
http://www.netlib.org/lapack/explore-html/d1/d89/cgemqr_8f_a735755730a44034cec76895ff38e035b.html | [
"",
null,
"LAPACK 3.10.0 LAPACK: Linear Algebra PACKage\n\n◆ cgemqr()\n\n subroutine cgemqr ( character SIDE, character TRANS, integer M, integer N, integer K, complex, dimension( lda, * ) A, integer LDA, complex, dimension( * ) T, integer TSIZE, complex, dimension( ldc, * ) C, integer LDC, complex, dimension( * ) WORK, integer LWORK, integer INFO )\n\nCGEMQR\n\nPurpose:\nCGEMQR overwrites the general real M-by-N matrix C with\n\nSIDE = 'L' SIDE = 'R'\nTRANS = 'N': Q * C C * Q\nTRANS = 'T': Q**H * C C * Q**H\n\nwhere Q is a complex unitary matrix defined as the product\nof blocked elementary reflectors computed by tall skinny\nQR factorization (CGEQR)\nParameters\n [in] SIDE SIDE is CHARACTER*1 = 'L': apply Q or Q**H from the Left; = 'R': apply Q or Q**H from the Right. [in] TRANS TRANS is CHARACTER*1 = 'N': No transpose, apply Q; = 'C': Conjugate transpose, apply Q**H. [in] M M is INTEGER The number of rows of the matrix A. M >=0. [in] N N is INTEGER The number of columns of the matrix C. N >= 0. [in] K K is INTEGER The number of elementary reflectors whose product defines the matrix Q. If SIDE = 'L', M >= K >= 0; if SIDE = 'R', N >= K >= 0. [in] A A is COMPLEX array, dimension (LDA,K) Part of the data structure to represent Q as returned by CGEQR. [in] LDA LDA is INTEGER The leading dimension of the array A. If SIDE = 'L', LDA >= max(1,M); if SIDE = 'R', LDA >= max(1,N). [in] T T is COMPLEX array, dimension (MAX(5,TSIZE)). Part of the data structure to represent Q as returned by CGEQR. [in] TSIZE TSIZE is INTEGER The dimension of the array T. TSIZE >= 5. [in,out] C C is COMPLEX array, dimension (LDC,N) On entry, the M-by-N matrix C. On exit, C is overwritten by Q*C or Q**H*C or C*Q**H or C*Q. [in] LDC LDC is INTEGER The leading dimension of the array C. LDC >= max(1,M). [out] WORK (workspace) COMPLEX array, dimension (MAX(1,LWORK)) [in] LWORK LWORK is INTEGER The dimension of the array WORK. If LWORK = -1, then a workspace query is assumed. The routine only calculates the size of the WORK array, returns this value as WORK(1), and no error message related to WORK is issued by XERBLA. [out] INFO INFO is INTEGER = 0: successful exit < 0: if INFO = -i, the i-th argument had an illegal value\nFurther Details\nThese details are particular for this LAPACK implementation. Users should not\ntake them for granted. These details may change in the future, and are not likely\ntrue for another LAPACK implementation. These details are relevant if one wants\nto try to understand the code. They are not part of the interface.\n\nIn this version,\n\nT(2): row block size (MB)\nT(3): column block size (NB)\nT(6:TSIZE): data structure needed for Q, computed by\nCLATSQR or CGEQRT\n\nDepending on the matrix dimensions M and N, and row and column\nblock sizes MB and NB returned by ILAENV, CGEQR will use either\nCLATSQR (if the matrix is tall-and-skinny) or CGEQRT to compute\nthe QR factorization.\nThis version of CGEMQR will use either CLAMTSQR or CGEMQRT to\nmultiply matrix Q by another matrix.\nFurther Details in CLAMTSQR or CGEMQRT.\n\nDefinition at line 170 of file cgemqr.f.\n\n172 *\n173 * -- LAPACK computational routine --\n174 * -- LAPACK is a software package provided by Univ. of Tennessee, --\n175 * -- Univ. of California Berkeley, Univ. of Colorado Denver and NAG Ltd..--\n176 *\n177 * .. Scalar Arguments ..\n178 CHARACTER SIDE, TRANS\n179 INTEGER INFO, LDA, M, N, K, TSIZE, LWORK, LDC\n180 * ..\n181 * .. Array Arguments ..\n182 COMPLEX A( LDA, * ), T( * ), C( LDC, * ), WORK( * )\n183 * ..\n184 *\n185 * =====================================================================\n186 *\n187 * ..\n188 * .. Local Scalars ..\n189 LOGICAL LEFT, RIGHT, TRAN, NOTRAN, LQUERY\n190 INTEGER MB, NB, LW, NBLCKS, MN\n191 * ..\n192 * .. External Functions ..\n193 LOGICAL LSAME\n194 EXTERNAL lsame\n195 * ..\n196 * .. External Subroutines ..\n197 EXTERNAL cgemqrt, clamtsqr, xerbla\n198 * ..\n199 * .. Intrinsic Functions ..\n200 INTRINSIC int, max, min, mod\n201 * ..\n202 * .. Executable Statements ..\n203 *\n204 * Test the input arguments\n205 *\n206 lquery = lwork.EQ.-1\n207 notran = lsame( trans, 'N' )\n208 tran = lsame( trans, 'C' )\n209 left = lsame( side, 'L' )\n210 right = lsame( side, 'R' )\n211 *\n212 mb = int( t( 2 ) )\n213 nb = int( t( 3 ) )\n214 IF( left ) THEN\n215 lw = n * nb\n216 mn = m\n217 ELSE\n218 lw = mb * nb\n219 mn = n\n220 END IF\n221 *\n222 IF( ( mb.GT.k ) .AND. ( mn.GT.k ) ) THEN\n223 IF( mod( mn - k, mb - k ).EQ.0 ) THEN\n224 nblcks = ( mn - k ) / ( mb - k )\n225 ELSE\n226 nblcks = ( mn - k ) / ( mb - k ) + 1\n227 END IF\n228 ELSE\n229 nblcks = 1\n230 END IF\n231 *\n232 info = 0\n233 IF( .NOT.left .AND. .NOT.right ) THEN\n234 info = -1\n235 ELSE IF( .NOT.tran .AND. .NOT.notran ) THEN\n236 info = -2\n237 ELSE IF( m.LT.0 ) THEN\n238 info = -3\n239 ELSE IF( n.LT.0 ) THEN\n240 info = -4\n241 ELSE IF( k.LT.0 .OR. k.GT.mn ) THEN\n242 info = -5\n243 ELSE IF( lda.LT.max( 1, mn ) ) THEN\n244 info = -7\n245 ELSE IF( tsize.LT.5 ) THEN\n246 info = -9\n247 ELSE IF( ldc.LT.max( 1, m ) ) THEN\n248 info = -11\n249 ELSE IF( ( lwork.LT.max( 1, lw ) ) .AND. ( .NOT.lquery ) ) THEN\n250 info = -13\n251 END IF\n252 *\n253 IF( info.EQ.0 ) THEN\n254 work( 1 ) = lw\n255 END IF\n256 *\n257 IF( info.NE.0 ) THEN\n258 CALL xerbla( 'CGEMQR', -info )\n259 RETURN\n260 ELSE IF( lquery ) THEN\n261 RETURN\n262 END IF\n263 *\n264 * Quick return if possible\n265 *\n266 IF( min( m, n, k ).EQ.0 ) THEN\n267 RETURN\n268 END IF\n269 *\n270 IF( ( left .AND. m.LE.k ) .OR. ( right .AND. n.LE.k )\n271 \\$ .OR. ( mb.LE.k ) .OR. ( mb.GE.max( m, n, k ) ) ) THEN\n272 CALL cgemqrt( side, trans, m, n, k, nb, a, lda, t( 6 ),\n273 \\$ nb, c, ldc, work, info )\n274 ELSE\n275 CALL clamtsqr( side, trans, m, n, k, mb, nb, a, lda, t( 6 ),\n276 \\$ nb, c, ldc, work, lwork, info )\n277 END IF\n278 *\n279 work( 1 ) = lw\n280 *\n281 RETURN\n282 *\n283 * End of CGEMQR\n284 *\nsubroutine clamtsqr(SIDE, TRANS, M, N, K, MB, NB, A, LDA, T, LDT, C, LDC, WORK, LWORK, INFO)\nCLAMTSQR\nDefinition: clamtsqr.f:198\nsubroutine xerbla(SRNAME, INFO)\nXERBLA\nDefinition: xerbla.f:60\nlogical function lsame(CA, CB)\nLSAME\nDefinition: lsame.f:53\nsubroutine cgemqrt(SIDE, TRANS, M, N, K, NB, V, LDV, T, LDT, C, LDC, WORK, INFO)\nCGEMQRT\nDefinition: cgemqrt.f:168\nHere is the call graph for this function:\nHere is the caller graph for this function:"
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"http://www.netlib.org/lapack/explore-html/lapack.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7266375,"math_prob":0.98675776,"size":3062,"snap":"2022-05-2022-21","text_gpt3_token_len":915,"char_repetition_ratio":0.13276652,"word_repetition_ratio":0.07090909,"special_character_ratio":0.2968648,"punctuation_ratio":0.15137614,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98963773,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-01-18T22:03:44Z\",\"WARC-Record-ID\":\"<urn:uuid:1d0b2f54-b689-472b-a2d5-ae83025725ce>\",\"Content-Length\":\"33344\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:52e3c9cc-4f20-43f3-8029-c572dbebb2b5>\",\"WARC-Concurrent-To\":\"<urn:uuid:f30f4f00-1e95-494a-a7fc-932518d5a4d7>\",\"WARC-IP-Address\":\"160.36.131.221\",\"WARC-Target-URI\":\"http://www.netlib.org/lapack/explore-html/d1/d89/cgemqr_8f_a735755730a44034cec76895ff38e035b.html\",\"WARC-Payload-Digest\":\"sha1:H257JSQVIWVH2UQEZ6D76Y7CFP6FRZME\",\"WARC-Block-Digest\":\"sha1:3KI65E6GVSQGCWCMVX5QUN3YPTKOYZC7\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-05/CC-MAIN-2022-05_segments_1642320301063.81_warc_CC-MAIN-20220118213028-20220119003028-00603.warc.gz\"}"} |
https://mat117.wisconsin.edu/book/03/3-the-normal-distribution/ | [
"## 3. The Normal Distribution\n\nFor the majority of the remainder of this class, we’ll be focusing on variables that have a (roughly) normal distribution. For example, data sets consisting of physical measurements (heights, weights, lengths of bones, and so on) for adults of the same species and sex often follow a similar pattern: most individuals are clumped around the average or mean of the population, with numbers decreasing the farther values are from the average in either direction.",
null,
"The shape of any normal curve is a single-peaked, symmetric distribution that is bell-shaped. A normally distributed random variable, or a variable with a normal probability distribution, is a continuous random variable that has a relative frequency histogram in the shape of a normal curve. This curve is also called the normal density curve. The actual functional notation for creating the normal curve is quite complex:",
null,
"where μ and σ are the mean and standard deviation of the population of data.\n\nWhat this formula tells us is that any mean μ and standard deviation σ completely define a unique normal curve. Recall that μ tells us the “center” of the peak while σ describes the overall “fatness” of the data set. A small σ value indicates a tall, skinny data set, while a larger value of σ results in a shorter, more spread out data set. Each normal distribution is indicated by the symbols N(μ,σ) . For example, the normal distribution N(0,1) is called the standard normal distribution, and it has a mean of 0 and a standard deviation of 1.\n\nProperties of a Normal Distribution\n\n1. A normal distribution is bell-shaped and symmetric about its mean.\n2. A normal distribution is completely defined by its mean, µ, and standard deviation, σ.\n3. The total area under a normal distribution curve equals 1.\n4. The x-axis is a horizontal asymptote for a normal distribution curve.\n\nA graphical representation of the Normal Distribution curve below:",
null,
"Because there are an infinite number of possibilities for µ and σ, there are an infinite number of normal curves. In order to determine probabilities for each normally distributed random variable, we would have to perform separate probability calculations for each normal distribution.",
null,
"One amazing fact about any normal distribution is called the 68-95-99.7 Rule, or more concisely, the empirical rule. This rule states that:\n\n• Roughly 68% of all data observations fall within one standard deviation on either side of the mean. Thus, there is a 68% chance of a variable having a value within one standard deviation of the mean\n• Roughly 95% of all data observations fall within two standard deviations on either side of the mean. Thus, there is a 95% chance of a variable having a value within two standard deviations of the mean\n• Roughly 99.7% of all data observations fall within three standard deviations on either side of the mean. Thus, there is a 99.7% chance of a variable having a value within three standard deviations of the mean\n\nA graphical representation of the empirical rule is shown in the following figure:",
null,
"##### Example:\n\nSuppose a variable has mean μ = 17 and standard deviation σ = 3.4. Then, according to the empirical rule:\n\n• Approximately 68% of individual data values will lie between: 17 – 3.4 = 13.6 and 17 + 3.4 = 20.4. In interval notation we write: (13.6, 20.4).\n• Approximately 95% of individual data values will lie between 17 – 2⋅3.4 = 10.2 and 17 + 2⋅3.4 = 23.8. In interval notation we write: (10.2, 23.8).\n• Approximately 99.7% of individual data values will lie between 17 – 3⋅3.4 = 6.8 and 17 + 3⋅3.4 = 27.2. In interval notation we write: (6.8, 27.2).\n\nThe results from the third bullet point illustrate how a data value of, say, 2.1 (which is less than 6.8) or a data value of, say, 33.2 (a value greater than 27.2) would both be very unusual, since almost all data values should lie between 6.8 and 27.2.\n\n#### Back to the Standard Normal Curve\n\nAll normal distributions, regardless of their mean and standard deviation, share the Empirical Rule. With some very simple mathematics, we can “transform” any normal distribution into the standard normal distribution. This is called a z-transform.",
null,
"",
null,
"Using the z-transformation, any data set that is normally distributed can be converted to the same standard normal distribution by the conversion:",
null,
"where X is the normally distributed random variable, and Z is a random variable following the standard normal distribution.\n\nNotice when X = μ that Z = (μ – μ)/σ = 0, which explains how Z transforms our mean to 0.\n\nProperties of the Standard Normal Distribution\n\n1. The standard normal distribution is bell-shaped and symmetric about its mean.\n2. The standard normal distribution is completely defined by its mean, µ = 0, and standard deviation, σ = 1.\n3. The total area under the standard normal distribution curve equals 1.\n4. The x-axis is a horizontal asymptote for the standard normal distribution curve.",
null,
""
] | [
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/section3-7.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/section3-8.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/Sec03.-NormalDis.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/Sec03.Normal-Dis2.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/unit3_04.jpg",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/section3-9.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/Sec03.-StdNorm3.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/section3-10.png",
null,
"https://mat117.wisconsin.edu/wp-content/uploads/2014/12/Sec03.-StdNorm.png",
null
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https://softmath.com/math-book-answers/sum-of-cubes/adding-subtracting-integers.html | [
"",
null,
"## What our customers say...\n\nThousands of users are using our software to conquer their algebra homework. Here are some of their experiences:\n\nEvery time I use the Algebrator program, I discover something new and useful, I think this program should be attached to each student computer in the US, especially considering its price.\nL.Y., Utah\n\nMy former algebra tutor got impatient whenever I couldnt figure out an equation. I eventually got tired of her so I decided to try the software. Im so impressed with it! I cant stress enough how great it is!\nMary Jones, NY\n\nSuper piece of software! I'm finally acing all of my algebra tests! Thanks a lot!\nAnne Mitowski, TX\n\nI liked the detailed, clearly explained step by step process that Algebrator uses. I'm able to go into my class and follow along with the teacher; it's amazing!\nLee Wyatt, TX\n\n## Search phrases used on 2013-01-02:\n\nStudents struggling with all kinds of algebra problems find out that our software is a life-saver. Here are the search phrases that today's searchers used to find our site. Can you find yours among them?\n\n• solving equations in excel\n• how to do LU on TI 89\n• what is 8% as a decimal\n• completing the square algebra exercises\n• transformations worksheets free printable grade\n• scott foresman math grade 6 online worksheets\n• how to square something calculator\n• how to cheat on a college algebra exam\n• e book on Algebra and Trigonometry: Graphing, Data and Analysis\n• free online ti calculators\n• pemutations and combinations free printable worksheets\n• free math worksheets distance formula\n• TI 89 to solve laplace transforms\n• mix fraction to decimal\n• math trivia in geometry\n• example of solving 2 binomial\n• TI 83 write program completing the square\n• glencoe mathematics algebra 2 answer key\n• Simultaneous Equation graphically solver\n• fraction equation calculator\n• Math poem\n• line chart, common factor for finding highest & lowest points\n• how to convert from long to minutes in java\n• online add and subtract rational expressions calculator\n• ti 89 cracks\n• simplify sqrt equation calculator\n• solving addition and subtraction equations calculator\n• worksheets ordered pairs scale factor\n• trinomial factoring calculator online\n• Completing Square Worksheet\n• maths algebra elimination and substitution free worksheets\n• distributive property for fractions\n• least common denominator tool\n• quadratic equation, solver on ti-86\n• signs of adding and subtracting integers\n• show me how to do a tree factor for the number 36 for fifth grade math\n• printable worksheet for third grade math\n• solving simultaneous equation in matlab\n• Exercise Worksheet Java Software Solutions\n• finding quadratic equation from table, difference\n• convert decimals to roots calculator\n• algebra problem set for 6th grade\n• middle school math with pizzazz for kids free online\n• math yr 11\n• free integer positive negative worksheets\n• glencoe mcgraw-hill algebra 1 answers\n• \"integers\" \"worksheet\" \"divide\" \"multiply\"\n• free saxon math homework sheets printouts\n• how to solve the equation 5+x≥-5 and graph it\n• 11+ exam online test\n• hyperbola graphs\n• exact answer square root free calculate\n• keys word problems algebra\n• general aptitude question\n• quadratic formula for third order\n• kinds maths worksheets\n• how to solve square roots with variables\n• convert decimal to fraction matlab\n• FREE PRINTABLE HOMEWORK HELP SHEETS\n• PRENTICE HALL MATHEMATICS WORD PROBLEMS\n• finding the radix of the numbers when quadratic equation was given\n• intermediate algebra cliff notes print\n• how to convert a decimal measurement to a mixed number\n• graphing calculater\n• Why should there be percentages when a number can be expressed as a fraction or a decimal?\n• Examples of Math Trivia\n• trinomial calculator\n• how to convert decimals to mixed numbers\n• factoring polynomials by decomposition\n• Free Algebra worksheets\n• Macintosh Pre-algebra accelerated book\n• sample math trivia for kids\n• equation worksheets\n• mcdougal littell math course 3 tutoring\n• nonlinear differential equations\n• simplification of rational algebraic expressions\n• evaluate definite integrals calculator\n• how to do solving systems on a ti 83 calculator\n• solve system of equations - 2 var - calc\n• matrix inverse"
] | [
null,
"https://softmath.com/r-solver/images/tutor.png",
null
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https://schoollearningcommons.info/question/if-the-zeros-of-f-cube-3-squqre-1-are-a-b-a-a-b-find-a-and-b-and-zeros-23104003-88/ | [
"## if the zeros of f(x)= x cube -3 x squqre +x+1 are a-b , a , a+b find a and b and zeros\n\nQuestion\n\nif the zeros of f(x)= x cube -3 x squqre +x+1 are a-b , a , a+b find a and b and zeros\n\nin progress 0\n1 month 2021-09-16T14:43:13+00:00 1 Answer 0 views 0\n\n1. Step-by-step explanation:\n\nsum of roots = -(-3)/1 = a-b+a+a+b = 3a\n\nso , a = 1\n\nproduct of roots = -(1)/1 = a(a²- b²)\n\n= 1(1 – b²)\n\nso , 1-b² = -1\n\nb² = 2\n\nso the values of a,b are 1,±√2 respectively\n\nplease mark as brainliest if you understand ☺️"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.60256803,"math_prob":0.99972886,"size":540,"snap":"2021-43-2021-49","text_gpt3_token_len":223,"char_repetition_ratio":0.09701493,"word_repetition_ratio":0.3392857,"special_character_ratio":0.4648148,"punctuation_ratio":0.10344828,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9995136,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-10-22T13:59:52Z\",\"WARC-Record-ID\":\"<urn:uuid:a70de21d-c2d9-489c-a09e-e96c0936fbb5>\",\"Content-Length\":\"65572\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:758c31dc-ac4c-450a-9159-8c0be6f929f6>\",\"WARC-Concurrent-To\":\"<urn:uuid:817199aa-d835-46ef-b2b2-118fc21247e9>\",\"WARC-IP-Address\":\"172.96.186.144\",\"WARC-Target-URI\":\"https://schoollearningcommons.info/question/if-the-zeros-of-f-cube-3-squqre-1-are-a-b-a-a-b-find-a-and-b-and-zeros-23104003-88/\",\"WARC-Payload-Digest\":\"sha1:VX6AXP5R3AWRB7OJV3DSMUILTEWRW77C\",\"WARC-Block-Digest\":\"sha1:BSOEKQK5YGB4ITW34KLXZPT5XVGRCZUC\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-43/CC-MAIN-2021-43_segments_1634323585507.26_warc_CC-MAIN-20211022114748-20211022144748-00334.warc.gz\"}"} |
https://www.jiskha.com/questions/108119/what-is-the-anode-and-cathode-of-this-problem-a-chemist-wishes-to-determine-the | [
"electrochemistry\n\nWhat is the anode and cathode of this problem?\n\nA chemist wishes to determine the concentration of CrO4-2 ions electrochemically. A cell is constructed consisting of saturated calomel electrode (SCE) and a silver wire coated with Ag2CrO4. The SCE is composed of mercury in contact with a saturated solution of calomel (Hg2Cl2). The electrolyte solution in the half-cell is saturated KCl. The E°cell of the SCE half-cell is +0.242 V with respect to the standard hydrogen electrode. The half-reaction for the reduction of Ag2CrO4 is shown below. (15 points)\n\nAg2CrO4(s) + 2e- 2Ag(s) + CrO4-2(aq) E°cell = 0.446 V\n\nI drew the SCE and AgCr is the wire, KCL is the electrolyte solution. There is Hg in contact with a saturated solution of calomel(HgCl).\n\nI said that Hg2Cl2 acts as the cathode and anode? Is that right.\n\n1. 👍\n2. 👎\n3. 👁\n1. I said that Hg2Cl2 acted as both the anode and cathode?\n\n1. 👍\n2. 👎\n\nSimilar Questions\n\n1. chemistry\n\nComplete the two reduction half reactions for the cell shown at the right, and show the line notation for the cell by dragging labels to the correct position. (The electrode on the left is the anode, and the one on the right is\n\n2. Physics\n\nThe anode (positive terminal) of an X-ray tube is at a potential of +115 000 V with respect to the cathode (negative terminal). (a) How much work (in joules) is done by the electric force when an electron is accelerated from the\n\n3. AP Chemistry\n\nSodium can be extracted by heating naturally occurring salt until it is molten. An electrochemical process is then used to extract the sodium. Cl2 is produced at the anode, and Na is collected at the cathode. 1. Write the\n\n4. Electrochemistry\n\nIn lab, we did an experiment with electrochemical cells with solutions of ZnSO4, CuSO4, Al2(SO4)3 and MgSO4 and their respective metal electrodes. There are a couple of post-lab questions that I'm not sure about: (1) Summarize\n\n1. Chemistry\n\n1. In the electrolysis of molten sodium chloride, sodium metal is produced at the anode & chlorine gas at the cathode sodium ions are produced at the cathode & chloride at the anode sodium ions are produced at the anode & chloride\n\n2. AP CHEMISTRY\n\nA voltaic cell is constructed that is based on the following reaction. Sn2+(aq) + Pb(s) -> Sn(s) + Pb2+(aq) (a) If the concentration of Sn2+ in the cathode half-cell is 1.80 M and the cell generates an emf of +0.219 V, what is the\n\n3. chemistry!\n\nIf the chemist mistakenly makes 275 mL of solution instead of the 200 mL, what molar concentration of sodium nitrate will the chemist have actually prepared? Answer in units of M\n\nIn a cathode ray tube, the number of electrons that reach the fluorescent screen is controlled by the A. cathode. B. deflecting plate. C. anode. D. grid. ? The part of the atom that accounts for electricity is the A. nucleus. B.\n\n1. Chemistry\n\nDesign an electrochemical cell using Pb(s) and Mn(s) and their solutions to answer the following questions. I just want to see if my answers are correct. I drew the cell already. Thanks 1. Give the line notation for this\n\n2. Chemistry\n\n1. Which of the following metals is oxidized by calcium ions? *potassium zinc iron lead 2. The first electrochemical cell was invented by ____. Michael Faraday *Alessandro Volta James Maxwell Benjamin Franklin 3. Why can't a lead\n\n3. Chemistry\n\n1. Sodium can be extracted by heating naturally occurring salt until it is molten. An electrochemical process is then used to extract the sodium. Cl2 is produced at the anode, and Na is collected at the cathode. A standard\n\n4. Physics\n\nThe anode (positive terminal) of an X-ray tube is at a potential of +125000 V with respect to the cathode (negative terminal). (a) How much work (in joules) is done by the electric force when an electron is accelerated from the"
] | [
null
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https://www.appannie.com/cn/apps/ios/app/fraction-to-decimal-and-decimals-to-fractions-converter/ | [
"# 分数计算器 4in1\n\n## 应用说明\n\nEverything you need to convert, calculate, simplify and compare fractions in one app!\n\nFraction Converter and Calculator is perfect for engineers, carpenters, builders, students and anyone who needs a comprehensive fraction app.\n\n► FRACTION CONVERTER\n- Converts fractions to decimals and vice versa.\n- Supports proper and improper fractions, mixed numbers, terminating and repeating decimals.\n- To convert a fraction to a decimal number, tap ‘Fractions', input a fraction or a mixed number and tap \"=\".\n- To convert a decimal number to a fraction, tap ‘Decimals’, enter a decimal number using the decimal point \".\" as separator (eg. 1.23) and tap \"=\".\nYou can use this converter for both terminating decimals and repeating decimals.\nFor repeating decimals enclose the repeating digits in parenthesis. Eg. type 0.24(3) for 0.24333... If the number is 5.123123..., type 5.(123).\n- Round fractions to the nearest 1/2, 1/4, 1/8, 1/16, 1/32, 1/64, 1/128, 1/256.\n\n► FRACTION CALCULATOR\n- Fraction calculator with steps for two and three fractions.\n- Performs basic operations (addition, subtraction, multiplication, and division) with proper and improper fractions, mixed numbers and whole numbers. Supports negative values.\n- To add, subtract, multiply, and divide three fractions, you should select a landscape orientation.\n- Round fractions to the nearest 1/2, 1/4, 1/8, 1/16, 1/32, 1/64, 1/128, 1/256.\n\n► FRACTION SIMPLIFIER\nCalculator for reducing fractions and mixed numbers.\n\n► COMPARE FRACTIONS CALCULATOR\nThe app compares proper and improper fractions and mixed numbers.\nYou can compare two or three fractions. To compare three fractions, you should select a landscape orientation.\n\nOTHER FEATURES:\n• Shows step-by-step solution.\n• History tape to view your recent calculations.\n• Back and forward buttons to check or recall recent calculations.\n• Sends results and history via email.\n• 'Undo' for the Clear command.\n• Personalize the look and feel of the app by changing the color of the theme.\n• The app supports both portrait and landscape orientation.\n\nAPP'S SETTINGS:\n- Rounding results to the desired number of decimal places. To round results to the nearest whole number, select 0 decimal places.\n- In Fraction Calculator and Fraction Converter, you can select to round fractions to the nearest 1/2, 1/4, 1/8, 1/16, 1/32, 1/64, 1/128, 1/256. By default, the app rounds fractions to the nearest 1/32.\nIf you do not need to round fractions, just select \"-\".\n- 7 color schemes.\n- Supports 18 languages:\nChinese, Czech, Danish, Dutch, English, Finnish, French, German, Greek, Italian, Japanese, Korean, Norwegian, Portuguese, Russian, Spanish, Swedish, Turkish.\n\nEVERYTHING YOU NEED FOR TEACHING AND LEARNING FRACTIONS\nFraction calculator and converter by Intemodino Group helps you solve various fraction problems.\nLearn and practice how to add, subtract, multiply, divide, compare, and simplify fractions. In addition, you can learn how to convert fractions to decimals and decimals to fractions.\nJust choose the fraction problem you want to solve from the list.\n\nTOPICS COVERED:\n2. Multiplying Fractions.\n3. Dividing Fractions.\n4. Comparing and Ordering Fractions.\n5. Simplifying Fractions.\n6. Converting Fractions to Decimals.\n7. Converting Decimals to Fractions.\n\nFraction Converter and Calculator is brought to you by Intemodino."
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.67005044,"math_prob":0.9663104,"size":3919,"snap":"2020-10-2020-16","text_gpt3_token_len":1163,"char_repetition_ratio":0.15810983,"word_repetition_ratio":0.07534247,"special_character_ratio":0.24776728,"punctuation_ratio":0.20689656,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9775139,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-02-23T17:34:11Z\",\"WARC-Record-ID\":\"<urn:uuid:85ebbe84-6ffd-43e5-a901-177d3fb4e655>\",\"Content-Length\":\"79799\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:53afbd5c-1e2e-4718-a4d3-504063691f41>\",\"WARC-Concurrent-To\":\"<urn:uuid:06a0fc98-e635-46e5-9aa5-f96adc609df9>\",\"WARC-IP-Address\":\"54.152.104.85\",\"WARC-Target-URI\":\"https://www.appannie.com/cn/apps/ios/app/fraction-to-decimal-and-decimals-to-fractions-converter/\",\"WARC-Payload-Digest\":\"sha1:ZBKMQRICBC5763QWXGXBUMZL6PCBXSDG\",\"WARC-Block-Digest\":\"sha1:6P4ADGBOWCPPUWCLW2DLNLUAFYQD4233\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-10/CC-MAIN-2020-10_segments_1581875145818.81_warc_CC-MAIN-20200223154628-20200223184628-00269.warc.gz\"}"} |
http://forums.wolfram.com/mathgroup/archive/2007/Oct/msg00672.html | [
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"Re: Efficient creation of regression design matrix\n\n• To: mathgroup at smc.vnet.net\n• Subject: [mg82320] Re: Efficient creation of regression design matrix\n• From: Ray Koopman <koopman at sfu.ca>\n• Date: Wed, 17 Oct 2007 04:11:32 -0400 (EDT)\n• References: <ff1ovf\\$8g5\\$1@smc.vnet.net>\n\n```On Oct 16, 12:24 am, \"Coleman, Mark\" <Mark.Cole... at LibertyMutual.com>\nwrote:\n> Hi,\n>\n> I'm searching for an efficient bit of code to create a design matrix of\n> 1's and 0's computed from categorical (non-numeric) variables, suitable\n> for use in regression problems. More precisely, imagine one has an n x 1\n> vector of k different non-numeric values. For argument sakes, let\n> k={Red,Blue,Green,Yellow}. I would like to create an n x k matrix\n> consisting of 1's and 0's, where a '1' appears in the row and column\n> location corresponding to the presence of an element of k. For example,\n> say the original data is\n>\n> Red\n> Blue\n> Blue\n> Yellow\n> Red\n> Green\n> .\n> .\n> .\n>\n> Then the corresponding design matrix would be (assuming we use the same\n> ordering of k):\n>\n> Original Red Blue Green Yellow\n> ====== ==============================\n> Red 1 0 0 0\n> Blue 0 1 0 0\n> Blue 0 1 0 0\n> Yellow 0 0 0 1\n> Red 1 0 0 0\n> Green 0 0 1 0\n>\n> And so on. I have some code that does this, but as is the norm, I'm sure\n> there are some great Mathematica one-liners that do a better job. In applied\n> problems that I work with, n can be up to 100,000 and k = 30\n>\n> Thanks,\n>\n> -Mark\n\nIf v is a list of values of variables, such as {red, blue, blue,\nyellow, red, green, ...}, and u is a list of the possible values in v,\nsuch as {red, blue, green, yellow}, then probably the simplest way to\nget what you asked for is\n\nx = Boole@Outer[SameQ, v, u] .\n\nA slightly more complicated, but much faster, way is\n\nx = v /. Thread[u -> IdentityMatrix@Length@u] .\n\n```\n\n• Prev by Date: Re: Re: format mixed integers & floats with text styling\n• Next by Date: Re: ProgressIndicator Questions\n• Previous by thread: Re: Efficient creation of regression design matrix\n• Next by thread: Mathematica Won't Activate"
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https://www.arxiv-vanity.com/papers/1402.5199/ | [
"# Embedding Quantum Universes into Classical Ones††thanks: This paper has been completed during the visits of the first author at the University of Technology Vienna (1997) and of the third author at the University of Auckland (1997). The first author has been partially supported by AURC A18/XXXXX/62090/F3414056, 1996. The second author was supported by DFG Research Grant No. HE 2489/2-1.\n\nCristian S. Calude,Peter H. Hertling,Karl Svozil Computer Science Department, The University of Auckland, Private Bag 92019, Auckland, New Zealand, e-mail: .Computer Science Department, The University of Auckland, Private Bag 92019, Auckland, New Zealand, e-mail: .Institut für Theoretische Physik, University of Technology Vienna, Wiedner Hauptstraße 8-10/136, A-1040 Vienna, Austria, e-mail: .\n###### Abstract\n\nDo the partial order and ortholattice operations of a quantum logic correspond to the logical implication and connectives of classical logic? Re-phrased, how far might a classical understanding of quantum mechanics be, in principle, possible? A celebrated result by Kochen and Specker answers the above question in the negative. However, this answer is just one among different possible ones, not all negative. It is our aim to discuss the above question in terms of mappings of quantum worlds into classical ones, more specifically, in terms of embeddings of quantum logics into classical logics; depending upon the type of restrictions imposed on embeddings the question may get negative or positive answers.\n\n## 1 Introduction\n\nQuantum mechanics is a very successful theory which appears to predict novel “counterintuitive” phenomena (see Wheeler , Greenberger, Horne and Zeilinger ) even almost a century after its development, cf. Schrödinger , Jammer [19, 20]. Yet, it can be safely stated that quantum theory is not understood (Feynman ). Indeed, it appears that progress is fostered by abandoning long–held beliefs and concepts rather than by attempts to derive it from some classical basis, cf. Greenberger and YaSin , Herzog, Kwiat, Weinfurter and Zeilinger and Bennett .\n\nBut just how far might a classical understanding of quantum mechanics be, in principle, possible? We shall attempt an answer to this question in terms of mappings of quantum worlds into classical ones, more specifically, in terms of embeddings of quantum logics into classical logics.\n\nOne physical motivation for this approach is a result proven for the first time by Kochen and Specker (cf. also Specker , Zierler and Schlessinger and John Bell ; see reviews by Mermin , Svozil and Tkadlec , and a forthcoming monograph by Svozil ) stating the impossibility to “complete” quantum physics by introducing noncontextual hidden parameter models. Such a possible “completion” had been suggested, though in not very concrete terms, by Einstein, Podolsky and Rosen (EPR) . These authors speculated that “elements of physical reality” exist irrespective of whether they are actually observed. Moreover, EPR conjectured, the quantum formalism can be “completed” or “embedded” into a larger theoretical framework which would reproduce the quantum theoretical results but would otherwise be classical and deterministic from an algebraic and logical point of view.\n\nA proper formalization of the term “element of physical reality” suggested by EPR can be given in terms of two-valued states or valuations, which can take on only one of the two values and , and which are interpretable as the classical logical truth assignments false and true, respectively. Kochen and Specker’s results state that for quantum systems representable by Hilbert spaces of dimension higher than two, there does not exist any such valuation defined on the set of closed linear subspaces of the space (these subspaces are interpretable as quantum mechanical propositions) preserving the lattice operations and the orthocomplement, even if one restricts the attention to lattice operations carried out among commuting (orthogonal) elements. As a consequence, the set of truth assignments on quantum logics is not separating and not unital. That is, there exist different quantum propositions which cannot be distinguished by any classical truth assignment.\n\nThe Kochen and Specker result, as it is commonly argued, e.g. by Peres and Mermin , is directed against the noncontextual hidden parameter program envisaged by EPR. Indeed, if one takes into account the entire Hilbert logic (of dimension larger than two) and if one considers all states thereon, any truth value assignment to quantum propositions prior to the actual measurement yields a contradiction. This can be proven by finitistic means, that is, with a finite number of one-dimensional closed linear subspaces (generating an infinite set whose intersection with the unit sphere is dense; cf. Havlicek and Svozil ). But, the Kochen–Specker argument continues, it is always possible to prove the existence of separable valuations or truth assignments for classical propositional systems identifiable with Boolean algebras. Hence, there does not exist any injective morphism from a quantum logic into some Boolean algebra.\n\nSince the previous reviews of the Kochen–Specker theorem by Peres [34, 35], Redhead , Clifton , Mermin , Svozil and Tkadlec , concentrated on the nonexistence of classical noncontextual elements of physical reality, we are going to discuss here some options and aspects of embeddings in greater detail. Particular emphasis will be given to embeddings of quantum universes into classical ones which do not necessarily preserve (binary lattice) operations identifiable with the logical or and and operations. Stated pointedly, if one is willing to abandon the preservation of quite commonly used logical functions, then it is possible to give a classical meaning to quantum physical statements, thus giving raise to an “understanding” of quantum mechanics.\n\nQuantum logic, according to Birkhoff , Mackey , Jauch , Kalmbach , Pulmannová , identifies logical entities with Hilbert space entities. In particular, elementary propositions are associated with closed linear subspaces of a Hilbert space through the origin (zero vector); the implication relation is associated with the set theoretical subset relation , and the logical or , and , and not operations are associated with the set theoretic intersection , with the linear span of subspaces and the orthogonal subspace , respectively. The trivial logical statement which is always true is identified with the entire Hilbert space , and its complement with the zero-dimensional subspace (zero vector). Two propositions and are orthogonal if and only if . Two propositions are co–measurable (commuting) if and only if there exist mutually orthogonal propositions such that and . Clearly, orthogonality implies co–measurability, since if and are orthogonal, we may identify with , respectively. The negation of is denoted by .\n\n## 2 Varieties of embeddings\n\nOne of the questions already raised in Specker’s almost forgotten first article 111In German. concerned an embedding of a quantum logical structure of propositions into a classical universe represented by a Boolean algebra . Thereby, it is taken as a matter of principle that such an embedding should preserve as much logico–algebraic structure as possible. An embedding of this kind can be formalized as a mapping with the following properties.222Specker had a modified notion of embedding in mind; see below. Let .\n\n(i)\n\nInjectivity: two different quantum logical propositions are mapped into two different propositions of the Boolean algebra, i.e., if then .\n\n(ii)\n\nPreservation of the order relation: if , then .\n\n(iii)\n\nPreservation of ortholattice operations, i.e. preservation of the\n\n(ortho-)complement:\n\n,\n\nor operation:\n\n,\n\nand operation:\n\n.\n\nAs it turns out, we cannot have an embedding from the quantum universe to the classical universe satisfying all three requirements (i)–(iii). In particular, a head-on approach requiring (iii) is doomed to failure, since the nonpreservation of ortholattice operations among nonco–measurable propositions is quite evident, given the nondistributive structure of quantum logics.\n\n### 2.1 Injective lattice morphisms\n\nHere we shall review the rather evident fact that there does not exist an injective lattice morphism from any nondistributive lattice into a Boolean algebra. We illustrate this obvious fact with an example that we need to refer to later on in this paper; the propositional structure encountered in the quantum mechanics of spin state measurements of a spin one-half particle along two different directions (mod ), that is, the modular, orthocomplemented lattice drawn in Figure 1 (where and ).\n\nClearly, is a nondistributive lattice, since for instance,\n\n p−∧(q−∨q+)=p−∧1=p−,\n\nwhereas\n\n (p−∧q−)∨(p−∧q+)=0∨0=0.\n\nHence,\n\n p−∧(q−∨q+)≠(p−∧q−)∨(p−∧q+).\n\nIn fact, is the smallest orthocomplemented nondistributive lattice.\n\nThe requirement (iii) that the embedding preserves all ortholattice operations (even for nonco–measurable and nonorthogonal propositions) would mean that . That is, the argument implies that the distributive law is not satisfied in the range of . But since the range of is a subset of a Boolean algebra and for any Boolean algebra the distributive law is satisfied, this yields a contradiction.\n\nCould we still hope for a reasonable kind of embedding of a quantum universe into a classical one by weakening our requirements, most notably (iii)? In the next three sections we are going to give different answers to this question. In the first section we restrict the set of propositions among which we wish to preserve the three operations complement , or , and and . We will see that the Kochen–Specker result gives a very strong negative answer even when the restriction is considerable. In the second section we analyze what happens if we try to preserve not all operations but just the complement. Here we will obtain a positive answer. In the third section we discuss a different embedding which preserves the order relation but no ortholattice operation.\n\n### 2.2 Injective order morphisms preserving ortholattice operations among orthogonal propositions\n\nLet us follow Zierler and Schlessinger and Kochen and Specker and weaken (iii) by requiring that the ortholattice operations need only to be preserved among orthogonal propositions. As shown by Kochen and Specker , this is equivalent to the requirement of separability by the set of valuations or two-valued probability measures or truth assignments on . As a matter of fact, Kochen and Specker proved nonseparability, but also much more—the nonexistence of valuations on Hilbert lattices associated with Hilbert spaces of dimension at least three. For related arguments and conjectures, based upon a theorem by Gleason , see Zierler and Schlessinger and John Bell .\n\nRather than rephrasing the Kochen and Specker argument concerning nonexistence of valuations in three-dimensional Hilbert logics in its original form or in terms of fewer subspaces (cf. Peres , Mermin ), or of Greechie diagrams, which represent orthogonality very nicely (cf. Svozil and Tkadlec , Svozil ), we shall give two geometric arguments which are derived from proof methods for Gleason’s theorem (see Piron , Cooke, Keane, and Moran , and Kalmbach ).\n\nLet be the lattice of closed linear subspaces of the three-dimensional real Hilbert space . A two-valued probability measure or valuation on is a map which maps the zero-dimensional subspace containing only the origin to , the full space to , and which is additive on orthogonal subspaces. This means that for two orthogonal subspaces the sum of the values and is equal to the value of the linear span of and . Hence, if are a tripod of pairwise orthogonal one-dimensional subspaces, then\n\n v(s1)+v(s2)+v(s3)=v(R3)=1.\n\nThe valuation must map one of these subspaces to and the other two to . We will show that there is no such map. In fact, we show that there is no map which is defined on all one-dimensional subspaces of and maps exactly one subspace out of each tripod of pairwise orthogonal one-dimensional subspaces to and the other two to .\n\nIn the following two geometric proofs we often identify a given one-dimensional subspace of with one of its two intersection points with the unit sphere\n\n S2={x∈R3 | ||x||=1}.\n\nIn the statements “a point (on the unit sphere) has value (or value )” or that “two points (on the unit sphere) are orthogonal” we always mean the corresponding one-dimensional subspaces. Note also that the intersection of a two-dimensional subspace with the unit sphere is a great circle.\n\nTo start the first proof, let us assume that a function satisfying the above condition exists. Let us consider an arbitrary tripod of orthogonal points and let us fix the point with value . By a rotation we can assume that it is the north pole with the coordinates . Then, by the condition above, all points on the equator must have value since they are orthogonal to the north pole.\n\nLet be a point in the northern hemisphere, but not equal to the north pole, that is . Let be the unique great circle which contains and the points in the equator, which are orthogonal to . Obviously, is the northern-most point on . To see this, rotate the sphere around the -axis so that comes to lie in the -plane; see Figure 2. Then the two points in the equator orthogonal to are just the points , and is the intersection of the plane through and with the unit sphere, hence\n\n C(q)={p∈R3 | (∃ α,β∈R) α2+β2=1 \\rm and p=αq+β(0,1,0)}.\n\nThis shows that has the largest -coordinate among all points in .",
null,
"Figure 2: The great circle C(q).\n\nAssume that has value . We claim that then all points on must have value . Indeed, since has value and the orthogonal point on the equator also has value , the one-dimensional subspace orthogonal to both of them must have value . But this subspace is orthogonal to all points on . Hence all points on must have value .\n\nNow we can apply the same argument to any point on (by the last consideration must have value ) and derive that all points on have value . The great circle divides the northern hemisphere into two regions, one containing the north pole, the other consisting of the points below or “lying between and the equator”, see Figure 2. The circles with certainly cover the region between and the equator.333This will be shown formally in the proof of the geometric lemma below. Hence any point in this region must have value .\n\nBut the circles cover also a part of the other region. In fact, we can iterate this process. We say that a point in the northern hemisphere can be reached from a point in the northern hemisphere, if there is a finite sequence of points in the northern hemisphere such that for . Our analysis above shows that if has value and can be reached from , then also has value .\n\nThe following geometric lemma due to Piron (see also Cooke, Keane, and Moran or Kalmbach ) is a consequence of the fact that the curve is tangent to the horizontal plane through the point :\n\nIf and are points in the northern hemisphere with , then can be reached from .\n\nThis result will be proved in Appendix A. We conclude that, if a point in the northern hemisphere has value , then every point in the northern hemisphere with must have value as well.\n\nConsider the tripod\n\nIn the following we give a second topological and geometric proof for this fact. In this proof we shall not use the geometric lemma above.\n\nFix an arbitrary point on the unit sphere with value . The great circle consisting of points orthogonal to this point splits into two disjoint sets, the set of points with value , and the set of points orthogonal to these points. They have value . If one of these two sets were open, then the other had to be open as well. But this is impossible since the circle is connected and cannot be the union of two disjoint open sets. Hence the circle must contain a point with value and a sequence of points , with value converging to . By a rotation we can assume that is the north pole and the circle lies in the -plane. Furthermore we can assume that all points have the same sign in the -coordinate. Otherwise, choose an infinite subsequence of the sequence with this property. In fact, by a rotation we can assume that all points have positive -coordinate (i.e. all points , lie as the point in Figure 2 and approach the north pole as tends to infinity). All points on the equator have value . By the first step in the proof of the geometric lemma in the appendix, all points in the northern hemisphere which lie between (the great circle through and ) and the equator can be reached from . Hence, as we have seen in the first proof, implies that all these points must have value . Since approaches the north pole, the union of the regions between and the equator is equal to the open right half of the northern hemisphere. Hence all points in this set have value . Let be a point in the left half of the northern hemisphere. It forms a tripod together with the point in the equator and the point in the right half. Since these two points have value , the point must have value . Hence all points in the left half of the northern hemisphere must have value . But this leads to a contradiction because there are tripods with two points in the left half, for example the tripod\n\n### 2.3 Injective morphisms preserving order as well as or and and operations\n\nWe have seen that we cannot hope to preserve the ortholattice operations, not even when we restrict ourselves to operations among orthogonal propositions.\n\nAn even stronger weakening of condition (iii) would be to require preservation of ortholattice operations merely among the center , i.e., among those propositions which are co–measurable (commuting) with all other propositions. It is not difficult to prove that in the case of complete Hilbert lattices (and not mere subalgebras thereof), the center consists of just the least lower and the greatest upper bound and thus is isomorphic to the two-element Boolean algebra . As it turns out, the requirement is trivially fulfilled and its implications are quite trivial as well.\n\nAnother weakening of (iii) is to restrict oneself to particular physical states and study the embeddability of quantum logics under these constraints; see Bell, Clifton .\n\nIn the following sections we analyze a completely different option: Is it possible to embed quantum logic into a Boolean algebra when one does not demand preservation of all ortholattice operations?\n\nOne method of embedding an arbitrary partially ordered set into a concrete orthomodular lattice which in turn can be embedded into a Boolean algebra has been used by Kalmbach and extended by Harding and Mayet and Navara . In these Kalmbach embeddings, as they may be called, the meets and joins are preserved but not the complement.\n\nThe Kalmbach embedding of some bounded lattice into a concrete orthomodular lattice may be thought of as the pasting of Boolean algebras corresponding to all maximal chains of .\n\nFirst, let us consider linear chains . Such chains generate Boolean algebras in the following way: from the first nonzero element on to the greatest element , form , where is the complement of relative to ; i.e., . is then an atom of the Boolean algebra generated by the bounded chain .\n\nTake, for example, a three-element chain as depicted in Figure 3a). In this case,\n\n A1 = a1∧(a0)′=a1∧1≡{a}∧{a,b}={a}, A2 = a2∧(a1)′=1∧(a1)′≡{a,b}∧{b}={b}.\n\nThis construction results in a four-element Boolean Kalmbach lattice with the two atoms and given in Figure 3b).\n\nTake, as a second example, a four-element chain as depicted in Figure 3c). In this case,\n\n A1 = a1∧(a0)′=a1∧1≡{a}∧{a,b,c}={a}, A2 = a2∧(a1)′≡{a,b}∧{b,c}={b}, A3 = a3∧(a2)′=1∧(a2)′≡{a,b,c}∧{c}={c}.\n\nThis construction results in an eight-element Boolean Kalmbach lattice with the three atoms , and depicted in Figure 3d).\n\nTo apply Kalmbach’s construction to any bounded lattice, all Boolean algebras generated by the maximal chains of the lattice are pasted together. An element common to two or more maximal chains must be common to the blocks they generate.\n\nTake, as a third example, the Boolean lattice drawn in Figure 3e). contains two linear chains of length three which are pasted together horizontally at their smallest and biggest elements. The resulting Kalmbach lattice is of the “Chinese lantern” type, see Figure 3f).\n\nTake, as a fourth example, the pentagon drawn in Figure 3g). It contains two linear chains: one is of length three, the other is of length 4. The resulting Boolean algebras and are again horizontally pasted together at their extremities . The resulting Kalmbach lattice is given in Figure 3h).\n\nIn the fifth example drawn in Figure 3i), the lattice has two maximal chains which share a common element. This element is common to the two Boolean algebras, hence central in . The construction of the five atoms proceeds as follows:\n\n A1 = {a}∧{a,b,c,d}={a}, A2 = {a,b,c}∧{b,c,d}={b,c}, A3 = B3={a,b,c,d}∧{d}={d}, B1 = {b}∧{a,b,c,d}={b}, B2 = {a,b,c}∧{a,c,d}={a,c},\n\nwhere the two sets of atoms and span two Boolean algebras pasted together at the extremities and at and . The resulting lattice is depicted in Figure 3j).\n\n### 2.4 Injective morphisms preserving order and complementation\n\nIn the following, we shall show that any orthoposet can be embedded into a Boolean algebra where in this case by an embedding we understand an injective mapping preserving the order relation and the orthocomplementation.\n\nA slightly stronger version of this fact using more topological notions has already been shown by Katrnoška . Zierler and Schlessinger constructed embeddings with more properties for orthomodular orthoposets [52, Theorem 2.1] and mentioned another slightly stronger version of the result above without explicit proof [52, Section 2, Remark 2].\n\nFor completeness sake we give the precise definition of an orthoposet. An orthoposet (or orthocomplemented poset) is a set which is endowed with a partial ordering , (i.e. a subset of satisfying (1) , (2) if and , then , (3) if and , then , for all ). Furthermore, contains distinguished elements and satisfying and , for all . Finally, is endowed with a function (orthocomplementation) from to satisfying the conditions (1) , (2) if , then , (3) the least upper bound of and exists and is , for all . Note that these conditions imply , , and that the greatest lower bound of and exists and is , for all .\n\nFor example, an arbitrary sublattice of the lattice of all closed linear subspaces of a Hilbert space is an orthoposet, if it contains the subspace and the full Hilbert space and is closed under the orthogonal complement operation. Namely, the subspace is the in the orthoposet, the full Hilbert space is the , the set-theoretic inclusion is the ordering , and the orthogonal complement operation is the orthocomplementation .\n\nIn the rest of this section we always assume that is an arbitrary orthoposet. We shall construct a Boolean algebra and an injective mapping which preserves the order relation and the orthocomplementation. The construction goes essentially along the same lines as the construction of Zierler and Schlessinger and Katrnoška and is similar to the proof of the Stone representation theorem for Boolean algebras, cf. Stone . It is interesting to note that for a finite orthoposet the constructed Boolean algebra will be finite as well.\n\nWe call a nonempty subset of an ideal if for all :\n\n1. if , then ,\n\n2. if and , then .\n\nClearly, if is an ideal, then . An ideal is maximal provided that if is an ideal and , then .\n\nLet be the set of all maximal ideals in , and let be the power set of considered as a Boolean algebra, i.e. is the Boolean algebra which consists of all subsets of . The order relation in is the set-theoretic inclusion, the ortholattice operations complement, or, and and are given by the set-theoretic complement, union, and intersection, and the elements and of the Boolean algebra are just the empty set and the full set . Consider the map\n\n φ:L→B\n\nwhich maps each element to the set\n\n φ(p)={I∈I | p∉I}\n\nof all maximal ideals which do not contain . We claim that the map\n\n1. is injective,\n\n2. preserves the order relation,\n\n3. preserves complementation.\n\nThis provides an embedding of quantum logic into classical logic which preserves the implication relation and the negation.444Note that for a finite orthoposet the Boolean algebra is finite as well. Indeed, if is finite, then it has only finitely many subsets, especially only finitely many maximal ideals. Hence is finite, and thus also its power set is finite.\n\nThe rest of this section consists of the proof of the three claims above. Let us start with claim (ii). Assume that satisfy . We have to show the inclusion\n\n φ(p)⊆φ(q).\n\nTake a maximal ideal . Then . If were contained in , then by condition 2. in the definition of an ideal also had to be contained in . Hence , thus proving that .\n\nBefore we come to claims (iii) and (i) we give another characterization of maximal ideals. We start with the following assertion which will also be needed later:\n\n \\rm If I is an ideal and r∈L with r∉I and r′∉I,\\rm then also the set J=I∪{s∈L∣s≤r} is an ideal. (1)\n\nHere is the proof: It is clear that satisfies condition 2. in the definition of an ideal. To show that it satisfies condition 1. assume to the contrary that there exists and , for some . Then one of the following conditions must be true; (I) , (II) and , (III) and , (IV) , . The first case is impossible since is an ideal. The second case is ruled out by the fact that (namely, would imply which would contradict our assumption ). The third case is impossible since implies which, combined with would imply , contrary to our assumption. Finally the fourth case is nothing but a reformulation of the third case with and interchanged. Thus we have proved that is an ideal and have proved the assertion (1).\n\nNext, we prove the following new characterization of maximal ideals:\n\n An ideal I is a maximal ideal iff r∉I implies r′∈I. (2)\n\nTo prove this first assume that for all , if , then and suppose is a proper subset of an ideal . Then there exists such that . By our hypothesis (for all , implies ), we have . Thus both and . This contradicts the fact that is an ideal.\n\nConversely, suppose that is a maximal ideal in and suppose, to the contrary, that for some\n\n r∉I and r′∉I. (3)\n\nOf course , since . Let\n\n J=I∪(r) (4)\n\nwhere is the principal ideal of (note that is indeed an ideal). Then, under assumption (3), using (1) above, we have that is an ideal which properly contains . This contradicts the maximality of and ends the proof of the assertion (2).\n\nFor claim (iii) we have to show the relation:\n\n φ(p′)=I∖φ(p),\n\nfor all . This can be restated as\n\n I∈φ(p′)iffI∉φ(p)\n\nfor all . But this means , which follows directly from condition 1. in the definition of an ideal and from assertion (2).\n\nWe proceed to claim (i), which states that is injective, i.e., if , then . But is equivalent to . Furthermore, if we can show that there is a maximal ideal such that and then it follows easily that . Indeed, means and means . It is therefore enough to prove that:\n\nIf , then there exists a maximal ideal such that and .\n\nTo prove this we note that since , we have . Let\n\n Ipq={K⊆L∣K is an ideal and p∉K and q∈K}.\n\nWe have to show that among the elements of there is a maximal ideal. Therefore we will use Zorn’s Lemma. In order to apply it to we have to show that is not empty and that every chain in has an upper bound.\n\nThe set is not empty since . Now we are going to show that every chain in has an upper bound. This means that, given a subset (chain) of with the property\n\n for allJ,K∈Cone hasJ⊆K \\rm or K⊆J,\n\nwe have to show that there is an element (upper bound) with for all . The union\n\n UC=⋃K∈CK\n\nof all ideals is the required upper bound! It is clear that all are subsets of . We have to show that is an element of . Since for all we also have . Similarly, since for some (even all) , we have . We still have to show that is an ideal. Given two propositions with and we conclude that must be contained in one of the ideals . Hence also . Now assume . Is it possible that the complement belongs to ? The answer is negative, since otherwise and , for some ideals . But since is a chain we have or , hence in the first case and in the second case. Both cases contradict the fact that and are ideals. Hence, is an ideal and thus an element of . We have proved that is not empty and that each chain in has an upper bound in .\n\nConsequently, we can apply Zorn’s Lemma to and obtain a maximal element in the ordered set . Thus\n\n p∉I and q∈I. (5)\n\nIt remains to show that is a maximal ideal in . Thus suppose, to the contrary, that is not a maximal ideal in .\n\nBy (2) there exists such that both and . Furthermore, since , then either or . Without loss of generality suppose\n\n p≰r. (6)\n\nIt follows, by (1), and since and , that is an ideal properly containing . But since, by Conditions (5) and (6), and , we have\n\nand .\n\nThus and, since , we deduce that properly contains , contradicting the fact that is a maximal element in . This ends the proof of claim (i), the claim that the map is injective.\n\nWe have shown:\n\nAny orthoposet can be embedded into a Boolean algebra where the embedding preserves the order relation and the complementation.\n\n### 2.5 Injective order preserving morphisms\n\nIn this section we analyze a different embedding suggested by Malhas [29, 30].\n\nWe consider an orthocomplemented lattice , i.e. a lattice with for all , with orthocomplementation, that is with a mapping satisfying the following three properties: a) , b) if , then , c) and . Here and .\n\nFurthermore, we will assume that is atomic555For every , there is an atom such that . An atom is an element with the property that if , then or . and satisfies the following additional property:\n\n for all x,y∈L,x≤y iff for every atom a∈L,a≤x impliesa≤y. (7)\n\nEvery atomic Boolean algebra and the lattice of closed subspaces of a separable Hilbert space satisfy the above conditions.\n\nConsider next a set 666Not containing the logical symbols . and let be the smallest set of words over the alphabet which contains and is closed under negation (if , then ) and implication (if , then ).777Define in a natural way , , . The elements of are called simple propositions and the elements of are called (compound) propositions.\n\nA valuation is a mapping\n\n t:W(U)→2\n\nsuch that and iff and . Clearly, every assignment can be extended to a unique valuation .\n\nA tautology is a proposition which is true under every possible valuation, i.e., , for every valuation . A set is consistent if there is a valuation making true every proposition in . Let and . We say that derives from , and write , in case for each valuation which makes true every proposition in (that is, , for all ). We define the set of consequences of by\n\n Con(K)={A∈W(U)∣K⊨A}.\n\nFinally, a set is a theory if is a fixed-point of the operator :\n\n Con(K)=K.\n\nIt is easy to see that is in fact a finitary closure operator, i.e., it satisfies the following four properties:\n\n• ,\n\n• if , then ,\n\n• ,\n\n• .\n\nThe first three properties can be proved easily. A topological proof for the fourth property can be found in Appendix B.\n\nThe main example of a theory can be obtained by taking a set of valuations and constructing the set of all propositions true under all valuations in :\n\n Th(X)={A∈W(U)∣t(A)=1, for allt∈X}.\n\nIn fact, every theory is of the above form, that is, for every theory there exists a set of valuations (depending upon ) such that Indeed, take\n\n XK={t:W(U)→2∣t valuation witht(A)=1, for all A∈K},\n\nand notice that\n\n Th(XK) = {B∈W(U)∣t(B)=1, for all t∈XK} = {B∈W(U)∣t(B)=1, for every valuation witht(A)=1, for all A∈K} = Con(K)=K.\n\nIn other words, theories are those sets of propositions which are true under a certain set of valuations (interpretations).\n\nLet now be a theory. Two elements are -equivalent, written , in case . The relation is an equivalence relation. The equivalence class of is and the factor set is denoted by ; for brevity, we will sometimes write instead of . The factor set comes with a natural partial order:\n\n [p]≤[q] ifp→q∈T.\n\nNote that in general, is not a Boolean algebra.888For instance, in case , for some . If has at least three elements, then does not have a minimum.\n\nIn a similar way we can define the -equivalence of two propositions:\n\n A≡TB if A↔B∈T.\n\nDenote by (shortly, ) the equivalence class of and note that for every ,\n\n [p]=[[p]]∩U.\n\nThe resulting Boolean algebra is the Lindenbaum algebra of .\n\nFix now an atomic orthocomplemented lattice satisfying (7). Let be a set of cardinality greater or equal to and fix a surjective mapping . For every atom , let be the assignment defined by iff . Take\n\n X={tsa∣a is an atom ofL}\\lx@notefootnoteRecallthat$ts$istheuniquevaluationextending$s$.\\rm and T=Th(X).\n\nMalhas [29, 30] has proven that the lattice is orthocomplemented, and, in fact, isomorphic to . Here is the argument. Note first that there exist two elements in such that . Clearly, , but . Indeed, for every atom , , so , a.s.o.\n\nSecondly, for every ,\n\n p→q∈T iff f(p)≤f(q).\n\nIf , then there exists an atom such that so , which—according to the definition of —mean , but . If , then , a contradiction. Conversely, if , then by (7) there exists an atom such that and . So, , i.e., .\n\nAs immediate consequences we deduce the validity of the following three relations: for all ,\n\n• iff ,\n\n• iff ,\n\n• .\n\nTwo simple propositions are conjugate in case .101010Of course, this relation is symmetrical. Define now the operation as follows: in case is a conjugate of . It is not difficult to see that the operation is well-defined and actually is an orthocomplementation. It follows that is an orthocomplemented lattice.\n\nTo finish the argument we will show that this lattice is isomorphic with . The isomorphism is given by the mapping defined by the formula . This is a well-defined function (because iff ), which is bijective ( implies , and surjective because is onto). If , then , i.e. . Finally, if is a conjugate of , then\n\n ψ([p]∗)=ψ([q])=f(q)=f(p)′=ψ([p])′.\n\nIn particular, there exists a theory whose induced orthoposet is isomorphic to the lattice of all closed subspaces of a separable Hilbert space. How does this relate to the Kochen-Specker theorem? The natural embedding\n\n Γ:U≡T→W(U)≡T, Γ([p])=[[p]]\n\nis order preserving and one-to-one, but in general it does not preserve orthocomplementation, i.e. in general . We always have , but sometimes . The reason is that for every pair of conjugate simple propositions one has , but the converse is not true.\n\nBy combining the inverse of the isomorphism with we obtain an embedding of into the Boolean Lindenbaum algebra . Thus, the above construction of Malhas gives us another method how to embed any quantum logic into a Boolean logic in case we require that only the order is preserved.111111In Section 2.4 we saw that it is possible to embed quantum logic into a Boolean logic preserving the order and the complement.\n\nNext we shall give a simple example of a Malhas type embedding . Consider again the finite quantum logic represented in Figure 1. Let us choose\n\n U={A,B,C,D,E,F,G,H}.\n\nSince contains more elements than , we can map surjectively onto ; e.g.,\n\n f(A) = 0, f(B) = p−, f(C) = p−, f(D) = p+, f(E) = q−, f(F) = q+, f(G) = 1, f(H) = 1.\n\nFor every atom , let us introduce the truth assignment"
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https://chemistry.stackexchange.com/questions/161636/why-do-ccl4-and-ch4-have-the-same-bond-angle | [
"# Why do CCl4 and CH4 have the same bond angle?\n\nI was reading about the molecular shape of compounds. I learned that the electronegativity of the central atom and the terminal atom in a molecule both play a role in determining bond angle. In $$\\ce{NH3}$$ and $$\\ce{NF3}$$, $$\\ce{F}$$ having higher electronegativity than $$\\ce{H}$$, $$\\ce{NF3}$$ has a smaller bond angle compared to $$\\ce{NH3}$$.\n\nApplying the same logic, it was expected that $$\\ce{CCl4}$$ would have a smaller bond angle than that of $$\\ce{CH4}$$. Surprisingly, I found that both of them have the same bond angle. Why is this the case?\n\n• A molecule is very much a 3-dimensional thing. Unless you have its model before your eyes (maybe only as a mental image, but it has to be a good one), you totally can't move further. Dec 23, 2021 at 15:58\n• You have 4 atoms of one element, singly bonded to carbon, so they get, on average, as far apart as possible, which means tetrahedrally around the central carbon: chemistry.stackexchange.com/a/118202/79678.\n– Ed V\nDec 23, 2021 at 16:03\n• A tetrahedron is a tetrahedron no matter how small - with apologies to Dr. Seuss… Dec 23, 2021 at 16:23\n• @melanieshebel When applying MathJax to formulas, why not to use mhchem \\ce{}? It makes generally cleaner MJ code and keeps symbols upright as expected. Dec 23, 2021 at 18:51\n• The molecules $\\ce{CCl4}$ or $\\ce{CH4}$ contain six angles $\\ce{Cl-C-Cl}$ or six $\\ce{H-C-H}$. Why should one of these angles be different from any other one ? Dec 24, 2021 at 13:08\n\nIn $$\\ce{NH3}$$ and $$\\ce{NF3}$$, $$\\ce{F}$$ having higher electronegativity than $$\\ce{H}$$, $$\\ce{NF3}$$ has a smaller bond angle compared to $$\\ce{NH3}$$.\n\nBoth of these compounds have a lone pair on the central atom. So the bound electrons and the lone pair (if you are using the simple \"electrons pair up\" model) compete for space.\n\nApplying the same logic, it was expected that CCl4 would have a smaller bond angle than that of CH4.\n\nAll electrons around carbon are involved in bonding, so all four pairs are the same. To apply the electronegativity argument, you should compare the distinct bond angles in $$\\ce{CH2F2}$$ or in $$\\ce{CH2Cl2}$$.\n\nWelcome to Stack exchange chemistry.\n\nConsider for a moment what is known as the isolobal concept, there are a series of atoms and groups which all present the same types of orbitals (or at least close to identical orbitals) and the number of electrons.\n\nConsider for a moment a methane molecule, if we were to break a C-H bond then the carbon atom would only have seven valance electrons. The carbon in an alkane such as methane has rehybridized its orbitals to give us four sp^3 orbitals. These are arranged in a tetrahedron around the carbon.\n\nA covalent bond is formed by sharing the one electron in the sp3 orbital of the carbon with an atomic orbital from another atom that has the right geometry to overlap with the sp3 orbital. The sp3 orbital has two pear-shaped lobes, one is large and one is small. These have opposite signs of the wavefunction.\n\nA hydrogen atom in the ground state has a single electron in an s orbital, this is a sphere-shaped orbital that can interact with the sp3 orbital to form both a bonding and an antibonding orbital. We will only concentrate in this answer on the bonding orbitals.\n\nThe sphere-shaped s orbital has the right geometry to interact with the sp3 orbital and it can result in the formation of an occupied (2 electrons in it) bonding orbital between the carbon and the hydrogen. This will be a sigma bond (single bond)\n\nIf we change to chlorine, then the outermost orbital (for the valence electrons) of the atom has also rehybridized to give us four sp3 orbitals. Three of these are occupied with two electrons while one in an isolated chlorine atom only has one. The orbital with only one electron can interact with the sp3 orbital on the carbon (bearing only one electron) to form two new molecular orbitals. One is antibonding and one is bonding.\n\nIf the bonding orbital between the carbon and the chlorine is occupied with two electrons then we have a bond. The C-Cl and C-H bonds will be different in length. But the angle between them will be dictated by the arrangement of the sp3 orbitals around the carbon atom.\n\nIf you still do not understand it then I would suggest that you fall back to VSEPR theory. As it is the festive season go and grab an orange and four cocktail sticks. Stab them into the orange in such a way that they are the greatest angle apart. You should find that the tips of them form a triangle-based pyramid (tetrahedron). It will not matter if you put grapes on the points of the cocktail sticks to represent hydrogen atoms in the methane. Or apples to represent the chlorine atoms in carbon tetrachloride. You will still have the same arrangement of the atoms in your model.\n\nYou can then hang it on the tree as a decoration or pull it apart and eat the fruits. When I can not lay my hands on my molecule modeling kit made of plastic balls and straws I tend to grab oranges and then draw atoms with a marker pen on the skin.\n\n• you have tried to explain it with M.O theory.But my ques. wasn't based on that. It was actually based on the e.n of the terminal atoms of the two molecules which play a significant role in bond angle.And you didn't even raise a word on that. Dec 23, 2021 at 17:10\n• The electronegativity does not matter: see my first comment and the linked tetrahedral figure. Ammonia is polar because it has three hydrogens attached and a lone pair of electrons. Nitrogen trifluoride is also polar and for the same reason. The electronegativity differences determine the respective dipole moments. But with 4 H atoms around the central carbon, they are, on average, as far apart as possible, hence the tetrahedral geometry, and methane is non-polar. Same principle for carbon tetrachloride. Simple as that.\n– Ed V\nDec 23, 2021 at 18:18\n• The electronegativity is not relevent to the shape of the molecule, I went through two methods of predicting the shape of the molecule. Dec 24, 2021 at 16:29"
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https://gitlab.collabora.com/gtucker/linux/-/commit/191e56880a6a638ce931859317f37deb084b6433 | [
"### calibrate: home in on correct lpj value more quickly\n\n```Binary chop with a jiffy-resync on each step to find an upper bound is\nslow, so just race in a tight-ish loop to find an underestimate.\n\nIf done with lots of individual steps, sometimes several hundreds of\niterations would be required, which would impose a significant overhead,\nand make the initial estimate very low. By taking slowly increasing steps\n\nE.g. an x86_64 2.67GHz could have fitted in 613 individual small delays,\nbut in reality should have been able to fit in a single delay 644 times\nlonger, so underestimated by 31 steps. To reach the equivalent of 644\nsmall delays with the accelerating scheme now requires about 130\niterations, so has <1/4th of the overhead, and can therefore be expected\nto underestimate by only 7 steps.\n\nAs now we have a better initial estimate we can binary chop over a smaller\nrange. With the loop overhead in the initial estimate kept low, and the\nstep sizes moderate, we won't have under-estimated by much, so chose as\ntight a range as we can.\nSigned-off-by:",
null,
"Phil Carmody <ext-phil.2.carmody@nokia.com>\nCc: Ingo Molnar <mingo@elte.hu>\nCc: Thomas Gleixner <tglx@linutronix.de>\nCc: \"H. Peter Anvin\" <hpa@zytor.com>\nTested-by:",
null,
"Stephen Boyd <sboyd@codeaurora.org>\nCc: Greg KH <greg@kroah.com>\nSigned-off-by:",
null,
"Andrew Morton <akpm@linux-foundation.org>\nSigned-off-by:",
null,
"Linus Torvalds <torvalds@linux-foundation.org>```\nparent 71c696b1\n ... ... @@ -110,8 +110,8 @@ static unsigned long __cpuinit calibrate_delay_direct(void) {return 0;} /* * This is the number of bits of precision for the loops_per_jiffy. Each * bit takes on average 1.5/HZ seconds. This (like the original) is a little * better than 1% * time we refine our estimate after the first takes 1.5/HZ seconds, so try * to start with a good estimate. * For the boot cpu we can skip the delay calibration and assign it a value * calculated based on the timer frequency. * For the rest of the CPUs we cannot assume that the timer frequency is same as ... ... @@ -121,38 +121,49 @@ static unsigned long __cpuinit calibrate_delay_direct(void) {return 0;} static unsigned long __cpuinit calibrate_delay_converge(void) { unsigned long lpj, ticks, loopbit; int lps_precision = LPS_PREC; /* First stage - slowly accelerate to find initial bounds */ unsigned long lpj, ticks, loopadd, chop_limit; int trials = 0, band = 0, trial_in_band = 0; lpj = (1<<12); while ((lpj <<= 1) != 0) { /* wait for \"start of\" clock tick */ ticks = jiffies; while (ticks == jiffies) /* nothing */; /* Go .. */ ticks = jiffies; __delay(lpj); ticks = jiffies - ticks; if (ticks) break; } /* wait for \"start of\" clock tick */ ticks = jiffies; while (ticks == jiffies) ; /* nothing */ /* Go .. */ ticks = jiffies; do { if (++trial_in_band == (1<> (LPS_PREC + 1); /* * Do a binary approximation to get lpj set to * equal one clock (up to lps_precision bits) * equal one clock (up to LPS_PREC bits) */ lpj >>= 1; loopbit = lpj; while (lps_precision-- && (loopbit >>= 1)) { lpj |= loopbit; while (loopadd > chop_limit) { lpj += loopadd; ticks = jiffies; while (ticks == jiffies) /* nothing */; ; /* nothing */ ticks = jiffies; __delay(lpj); if (jiffies != ticks) /* longer than 1 tick */ lpj &= ~loopbit; lpj -= loopadd; loopadd >>= 1; } return lpj; ... ...\nMarkdown is supported\n0% or\nYou are about to add 0 people to the discussion. Proceed with caution.\nFinish editing this message first!"
] | [
null,
"https://gitlab.collabora.com/gtucker/linux/-/blob/master/assets/no_avatar-849f9c04a3a0d0cea2424ae97b27447dc64a7dbfae83c036c45b403392f0e8ba.png",
null,
"https://gitlab.collabora.com/gtucker/linux/-/blob/master/assets/no_avatar-849f9c04a3a0d0cea2424ae97b27447dc64a7dbfae83c036c45b403392f0e8ba.png",
null,
"https://gitlab.collabora.com/gtucker/linux/-/blob/master/assets/no_avatar-849f9c04a3a0d0cea2424ae97b27447dc64a7dbfae83c036c45b403392f0e8ba.png",
null,
"https://gitlab.collabora.com/gtucker/linux/-/blob/master/assets/no_avatar-849f9c04a3a0d0cea2424ae97b27447dc64a7dbfae83c036c45b403392f0e8ba.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.87247264,"math_prob":0.94538337,"size":1546,"snap":"2020-24-2020-29","text_gpt3_token_len":406,"char_repetition_ratio":0.09468223,"word_repetition_ratio":0.0,"special_character_ratio":0.23156533,"punctuation_ratio":0.13141026,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.96377903,"pos_list":[0,1,2,3,4,5,6,7,8],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-04T13:17:24Z\",\"WARC-Record-ID\":\"<urn:uuid:b6985d7d-e234-41ce-ba55-921e508184d7>\",\"Content-Length\":\"153966\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5cefbf67-5154-44df-a383-642874eab00d>\",\"WARC-Concurrent-To\":\"<urn:uuid:8e10a54e-697a-45e7-87a1-b2cc228f889a>\",\"WARC-IP-Address\":\"46.235.227.170\",\"WARC-Target-URI\":\"https://gitlab.collabora.com/gtucker/linux/-/commit/191e56880a6a638ce931859317f37deb084b6433\",\"WARC-Payload-Digest\":\"sha1:3MRFVMHSAZYWJV4M7XGZI473GUT22UYA\",\"WARC-Block-Digest\":\"sha1:SCSY3E3KUCOA6MJWTTEFTBMNT7RKZCKD\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590347441088.63_warc_CC-MAIN-20200604125947-20200604155947-00150.warc.gz\"}"} |
https://solsarin.com/merge-sort-advantages-and-disadvantages/ | [
"",
null,
"## Merge Sort, an explanation of it\n\nWhat is Merge Sort? How does it work? Actual recursion vs. what I thought was recursion. An example of Merge Sort. What are the advantages and disadvantages?\n\nI’m currently taking the Udemy class JavaScript Algorithm and Data Structures Masterclass by Colt Steele. Which I would recommend to anyone wanting to learn more about algorithms in Javascript. One of the many subjects is about sorting algorithms. One, in particular, I will be discussing today is Merge Sort.\n\n# A side note about recursion\n\nWell, it turns out true recursion does take fewer lines of code but conceptually is a little harder to comprehend. The only reason I’m mentioning it here is that recursion is a key component to Merge Sort.\n\nWell, it turns out true recursion does take fewer lines of code but conceptually is a little harder to comprehend. The only reason I’m mentioning it here is that recursion is a key component to Merge Sort.\n\n# An example and explanation of Merge Sort\n\n## Firstly, we need a helper function.\n\nSo in the above helper function, the code takes in two arrays of whatever lengths, then compares the values sequentially of array-1 and array-2. One thing to note is that for this function to work, our arrays need to be sorted. This is already done because, as mentioned before, we have taken our unsorted Array and broken it down to singular elements within each array before executing this function.\n\n## What is Merge Sort Algorithm: How does it work, its Advantages and Disadvantages\n\nThe “Merge Sort” uses a recursive algorithm to achieve its results. The divide-and-conquer algorithm breaks down a big problem into smaller, more manageable pieces that look similar to the initial problem. It then solves these subproblems recursively and puts their solutions together to solve the original problem.\n\nBy the end of this tutorial, you will have a better understanding of the technical fundamentals of the “Merge Sort” with all the necessary details, along with practical examples.\n\n## Merge sort\n\nIn computer science, merge sort (also commonly spelled as mergesort) is an efficient, general-purpose, and comparison-based sorting algorithm. Most implementations produce a stable sort, which means that the order of equal elements is the same in the input and output. Merge sort is a divide and conquer algorithm that was invented by John von Neumann in 1945. A detailed description and analysis of the bottom-up merge sort appeared in a report by Goldstine and von Neumann as early as 1948.\n\n## Algorithm\n\nConceptually, a merge sort works as follows:\n\n1. Divide the unsorted list into n sublists, each containing one element (a list of one element is considered sorted).\n2. Repeatedly merge sublists to produce new sorted sublists until there is only one sublist remaining. This will be the sorted list.\n\n### Top-down implementation\n\nExample C-like code using indices for top-down merge sort algorithm that recursively splits the list (called runs in this example) into sublists until sublist size is 1, then merges those sublists to produce a sorted list. The copy back step is avoided by alternating the direction of the merge with each level of recursion (except for an initial one-time copy). To help understand this, consider an array with two elements. The elements are copied to B[], then merged back to A[]. If there are four elements when the bottom of the recursion level is reached, a single element runs from A[] are merged to B[], and then at the next higher level of recursion, those two-element runs are merged to A[]. This pattern continues with each level of recursion.\n\nSorting a set of items in a list is a task that occurs often in computer programming. Often, a human can perform this task intuitively. However, a computer program has to follow a sequence of exact instructions to accomplish this. This sequence of instructions is called an algorithm. A sorting algorithm is a method that can be used to place a list of unordered items into an ordered sequence. The sequence of order is determined by a key. Various sorting algorithms exist, and they differ in terms of their efficiency and performance. Some important and well-known sorting algorithms are the bubble sort, the selection sort, the insertion sort, and the quick sort.\n\n## Bubble Sort\n\nThe bubble sort algorithm works by repeatedly swapping adjacent elements that are not in order until the whole list of items is in sequence. In this way, items can be seen as bubbling up the list according to their key values.\n\nThe primary advantage of the bubble sort is that it is popular and easy to implement. Furthermore, in the bubble sort, elements are swapped in place without using additional temporary storage, so the space requirement is at a minimum. The main disadvantage of the bubble sort is the fact that it does not deal well with a list containing a huge number of items. This is because the bubble sort requires n-squared processing steps for every n number of elements to be sorted. As such, the bubble sort is mostly suitable for academic teaching but not for real-life applications.\n\n## Selection Sort\n\nThe selection sort works by repeatedly going through the list of items, each time selecting an item according to its ordering and placing it in the correct position in the sequence.\n\nThe main advantage of the selection sort is that it performs well on a small list. Furthermore, because it is an in-place sorting algorithm, no additional temporary storage is required beyond what is needed to hold the original list. The primary disadvantage of the selection sort is its poor efficiency when dealing with a huge list of items. Similar to the bubble sort, the selection sort requires an n-squared number of steps for sorting n elements. Additionally, its performance is easily influenced by the initial ordering of the items before the sorting process. Because of this, the selection sort is only suitable for a list of a few elements that are in random order.\n\n## Insertion Sort\n\nThe insertion sorts repeatedly scan the list of items, each time inserting the item in the unordered sequence into its correct position.\n\nThe main advantage of the insertion sort is its simplicity. It also exhibits a good performance when dealing with a small list. The insertion sort is an in-place sorting algorithm so the space requirement is minimal. The disadvantage of the insertion sort is that it does not perform as well as other, better sorting algorithms. With n-squared steps required for every n element to be sorted, the insertion sort does not deal well with a huge list. Therefore, the insertion sort is particularly useful only when sorting a list of a few items.\n\n## Quick Sort\n\nThe quicksort works on the divide-and-conquer principle. First, it partitions the list of items into two sublists based on a pivot element. All elements in the first sublist are arranged to be smaller than the pivot, while all elements in the second sublist are arranged to be larger than the pivot. The same partitioning and arranging process is performed repeatedly on the resulting sublists until the whole list of items is sorted.\n\nThe quicksort is regarded as the best sorting algorithm. This is because of its significant advantage in terms of efficiency because it is able to deal well with a huge list of items. Because it sorts in place, no additional storage is required as well. The slight disadvantage of quick sort is that its worst-case performance is similar to average performances of the bubble, insertion or selections sorts. In general, the quick sort produces the most effective and widely used method of sorting a list of any item size."
] | [
null,
"https://solsarin.com/wp-content/uploads/2021/11/merge-sort-advantages-and-disadvantages2.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9275996,"math_prob":0.7790978,"size":9990,"snap":"2022-40-2023-06","text_gpt3_token_len":1996,"char_repetition_ratio":0.14360105,"word_repetition_ratio":0.062796205,"special_character_ratio":0.1953954,"punctuation_ratio":0.093059935,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95264703,"pos_list":[0,1,2],"im_url_duplicate_count":[null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-02-02T01:40:32Z\",\"WARC-Record-ID\":\"<urn:uuid:aae776e2-f1ee-42ff-8027-cfab5cd9a80a>\",\"Content-Length\":\"71835\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:56d4817f-f4d5-414a-a4d2-64ff2cb65da0>\",\"WARC-Concurrent-To\":\"<urn:uuid:e74d0d46-3805-4d04-bd68-f4ef03dc4b37>\",\"WARC-IP-Address\":\"172.67.175.125\",\"WARC-Target-URI\":\"https://solsarin.com/merge-sort-advantages-and-disadvantages/\",\"WARC-Payload-Digest\":\"sha1:4CNRYELIOWXZRAXLVR5VQIEIAC4PYWYT\",\"WARC-Block-Digest\":\"sha1:BW7EDS2IAA2FQPNB5ALTYNSAJ6CEY55G\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-06/CC-MAIN-2023-06_segments_1674764499954.21_warc_CC-MAIN-20230202003408-20230202033408-00045.warc.gz\"}"} |
https://answers.everydaycalculation.com/gcf/50-45 | [
"Solutions by everydaycalculation.com\n\n## What is the GCF of 50 and 45?\n\nThe GCF of 50 and 45 is 5.\n\n#### Steps to find GCF\n\n1. Find the prime factorization of 50\n50 = 2 × 5 × 5\n2. Find the prime factorization of 45\n45 = 3 × 3 × 5\n3. To find the GCF, multiply all the prime factors common to both numbers:\n\nTherefore, GCF = 5\n\nMathStep (Works offline)",
null,
"Download our mobile app and learn how to find GCF of upto four numbers in your own time:"
] | [
null,
"https://answers.everydaycalculation.com/mathstep-app-icon.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.81666994,"math_prob":0.99410075,"size":557,"snap":"2021-31-2021-39","text_gpt3_token_len":176,"char_repetition_ratio":0.13562387,"word_repetition_ratio":0.0,"special_character_ratio":0.3859964,"punctuation_ratio":0.08108108,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9942918,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-27T00:54:49Z\",\"WARC-Record-ID\":\"<urn:uuid:fe3ba6b6-8a43-4f0b-bd92-8f7a522d555b>\",\"Content-Length\":\"5831\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:bea367dd-aca4-467a-85a2-27e60c8fada1>\",\"WARC-Concurrent-To\":\"<urn:uuid:77dae509-c1ee-40fe-b24d-a3197f851625>\",\"WARC-IP-Address\":\"96.126.107.130\",\"WARC-Target-URI\":\"https://answers.everydaycalculation.com/gcf/50-45\",\"WARC-Payload-Digest\":\"sha1:52IJUZ5R4I3FTOCPHMSOYV25SDYARLUM\",\"WARC-Block-Digest\":\"sha1:FTW3TJAM5TN6INQ5K2RD2JAP73ZBQ6O3\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780058222.43_warc_CC-MAIN-20210926235727-20210927025727-00209.warc.gz\"}"} |
https://roboloco.net/project-euler/problem-35/ | [
"# Project Euler Problem 35",
null,
"For problem 35, we need to compute how many circular primes there are below 1,000,000. Circular primes are numbers for which all rotations of a number are also primes, like (197->971->719).\n\nOnce again, we exploit all that old code for lazily generating primes to our advantage:\n\n;; From Euler-7\n(def primes (lazy-primes-cgrande))\n\n;; From Euler-27\n(defn prime? [n]\n(not-any? #(zero? (rem n %)) (take-while #(<= % (Math/sqrt n)) primes)))\n\n(defn rotate-str [s]\n(apply str (concat (rest s) [(first s)])))\n\n(defn circular-prime? [n]\n(every? prime?\n(map #(Integer/parseInt %)\n(take (count (str n)) (iterate rotate-str (str n))))))\n\n(defn euler-35 []\n(count (filter circular-prime? (take-while #(< % 1000000) primes))))\n\nThat’s a straightforward definition with reasonable performance. Peeking at clojure-euler, I noticed a function in clojure.seq-utils that could replace the rotate-str, reducing circular-prime? to a one-liner:\n\nuse '[clojure.contrib.seq-utils :only (rotations)])\n\n(defn circular-prime? [n]\n(every? prime? (map #(Integer/parseInt (apply str %)) (rotations (str n)))))\n\nNote that this whole program really boils down to two new lines of functionality; everything else is old code borrowed from previous problems or clojure-contrib."
] | [
null,
"https://roboloco.net/images/ivar.jpg",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7713636,"math_prob":0.9407664,"size":1236,"snap":"2021-31-2021-39","text_gpt3_token_len":325,"char_repetition_ratio":0.12581168,"word_repetition_ratio":0.03508772,"special_character_ratio":0.29773462,"punctuation_ratio":0.14410481,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98808926,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-22T08:17:51Z\",\"WARC-Record-ID\":\"<urn:uuid:40c32aca-58a0-4131-a32a-aaf8a760ca71>\",\"Content-Length\":\"11411\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c46a02b5-93d0-46a4-8f9c-3a292b18b5c8>\",\"WARC-Concurrent-To\":\"<urn:uuid:98dd5765-248d-423c-bf15-d0127716353b>\",\"WARC-IP-Address\":\"185.199.111.153\",\"WARC-Target-URI\":\"https://roboloco.net/project-euler/problem-35/\",\"WARC-Payload-Digest\":\"sha1:I5PPUZEYEWY52T6Q3A6YBTW4MIEJXPBL\",\"WARC-Block-Digest\":\"sha1:N5L5KUBA6WXFYKPHCMT76XELIG64K5FS\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780057337.81_warc_CC-MAIN-20210922072047-20210922102047-00158.warc.gz\"}"} |
https://mathematica.stackexchange.com/questions/98847/who-can-explain-the-strange-behavior-of-command-last | [
"# Who can explain the strange behavior of command “Last”\n\n## Situation\n\nI use Last to extract the last element of an expression. Let poly=a+b*c+Log[a]+z.\n\n## Problem\n\nWhen Using Last@poly, I expect the output is z. However, the command gave me Log[a].\n\n## Debug\n\nWith FullForm@poly, I found the output is Plus[a,Times[b,c],z,Log[a]]. So, Log[a] should be the correct answer of the command, but not my expected answer.\n\n## My Question\n\nThe strange behavior confuse me.\n\n1. I wonder whether elements of an expression in mathematica have definite order.\n2. If the answer is \"no\", is there any alternative other than Last to avoid the undetermined behavior, so that I can extract particular element ?\n\nI wonder whether elements of an expression in mathematica have definite order.\n\nYes, the one you get after evaluating an expression. See Polynomial Ordering in the Wolfram Documentation Center. In your case, poly = a + b*c + Log[a] + z evaluates to\n\na + b c + z + Log[a]\n\nSo Last does indeed do what it's supposed to.\n\nYou could try extracting the elements with patterns (depending on what terms you actually need to extract), or you could use something like PolynomialForm[%,TraditionalOrder->True] (found here).\n\nSome general information about term ordering in Mathematica\n\nFunctions in Mathematica can have the Orderless attribute, which means that Mathematica will (re)arrange the supplied terms in canonical order, as described in this tutorial. Canonical ordering is used as a standard way to arrange terms in commutative and associative functions (such as Plus or Times in your case) for purposes of for example pattern matching.\n\n• Can you please also mention Orderless and link to the relevant tutorial? – Szabolcs Nov 7 '15 at 10:04\n• I added the information, thanks. – Graumagier Nov 7 '15 at 10:18"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7566387,"math_prob":0.62429726,"size":1095,"snap":"2019-51-2020-05","text_gpt3_token_len":300,"char_repetition_ratio":0.08615949,"word_repetition_ratio":0.0,"special_character_ratio":0.2648402,"punctuation_ratio":0.18723404,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9896817,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-24T02:22:59Z\",\"WARC-Record-ID\":\"<urn:uuid:5b69fb5c-10ec-450f-9b2b-9f2f08b90a34>\",\"Content-Length\":\"141866\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:7b09abda-e0e5-48c6-b3e6-4edde53bb471>\",\"WARC-Concurrent-To\":\"<urn:uuid:4ce502c7-5768-4c50-bfee-ba3ee4b461b7>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://mathematica.stackexchange.com/questions/98847/who-can-explain-the-strange-behavior-of-command-last\",\"WARC-Payload-Digest\":\"sha1:TD7ARXIYL26STLOBB4RTXPXWQAAQMAF3\",\"WARC-Block-Digest\":\"sha1:NKWK2HTE4TZOUHRXLR7BS3E5EFSWYWKF\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250614880.58_warc_CC-MAIN-20200124011048-20200124040048-00258.warc.gz\"}"} |
https://cvgmt.sns.it/paper/414/ | [
"# Least Squares estimation of two ordered monotone regression curves\n\ncreated by santambro on 01 Sep 2009\nmodified on 30 Oct 2009\n\n[BibTeX]\n\nAccepted Paper\n\nInserted: 1 sep 2009\nLast Updated: 30 oct 2009\n\nJournal: Journal of Nonparametric Statistics\nYear: 2009\nNotes:\n\nThis is not a true calculus of variations paper. It's an application of convex optimization to statistics. But, curiously enough, the main issue which is addressed (L2 projection on increasing functions) is used in some optimal transport papers as well.\n\nAbstract:\n\nTo project (in the $L^2$ metric) a single function $f$ on the set of increasing functions one takes the primitive of $f$, then its convex hull, and then takes the derivative. Here the problem is more complicated: project a pair $(f,g)$ on the set of pairs of increasing functions, the former smaller than the latter. It is a regression problem with applications in statistics. The solution is not explicit but we solve it numerically through a projected subgradient algorithm from convex optimization.\n\nKeywords: regression, monotone curves, subgradient descent"
] | [
null
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https://climate-cms.org/2018/04/19/cartopy-maps.html | [
"# Improving maps with Cartopy¶\n\nCartopy is a library for creating plots on maps. We can use it to improve Xarray's plots (see plotting basics for the basics of Xarray plotting)\n\nLet's load the data we used in the last page, surface temperature for the ACCESS1.0 AMIP run March 1984:\n\nIn :\n%matplotlib inline\nimport xarray\ndatapath = \"http://dapds00.nci.org.au/thredds/dodsC/rr3/CMIP5/output1/CSIRO-BOM/ACCESS1-0/amip/mon/atmos/Amon/r1i1p1/latest/tas/tas_Amon_ACCESS1-0_amip_r1i1p1_197901-200812.nc\"\ndata = xarray.open_dataset(datapath)\nsurface_temp_slice = data.tas.sel(time = '1984-03')\nsurface_temp_slice.plot()\n\nOut:\n<matplotlib.collections.QuadMesh at 0x7f0abc9dee80>",
null,
"## Projections¶\n\nCartopy is based around projecting the data in different ways. To use it, we create an axis with a specific projection, then add plots onto that axis.\n\nNote that we don't need to tell the plot command about our co-ordinates, Xarray does that automatically for us\n\nIn :\nimport cartopy.crs as ccrs\nimport matplotlib.pyplot as plt\n\nax = plt.axes(projection=ccrs.PlateCarree())\n\nsurface_temp_slice.plot(ax=ax)\n\nOut:\n<matplotlib.collections.QuadMesh at 0x7f0aaeb45dd8>",
null,
"Cartopy has a bunch of different projections that you can use.\n\nIf the data is in a different projection to the axis it's important to give a transform to plot(). Our data is on a lat-lon grid, so we need to tell Cartopy to transform it from a PlateCarree projection to LambertConfromal\n\nIn :\nax = plt.axes(projection=ccrs.LambertConformal())\n\nsurface_temp_slice.plot(ax=ax, transform=ccrs.PlateCarree())\n\nOut:\n<matplotlib.collections.QuadMesh at 0x7f0aae197518>",
null,
"Cartopy also has some helper functions for showing coastlines etc., which can make it easier to interpret a plot. These work regardless of what projection you are using\n\nIn :\nax = plt.axes(projection=ccrs.Orthographic())\n\nsurface_temp_slice.plot(ax=ax, transform=ccrs.PlateCarree())\n\nax.coastlines()\n\nOut:\n<cartopy.mpl.feature_artist.FeatureArtist at 0x7f0aada05390>",
null,
"To restrict the plot's domain you can use ax.set_extent():\n\nIn :\nimport cartopy.crs as ccrs\nimport matplotlib.pyplot as plt\n\nax = plt.axes(projection=ccrs.NearsidePerspective(central_latitude=-20, central_longitude=120))\n\nsurface_temp_slice.plot(ax=ax, transform=ccrs.PlateCarree())\n\nax.coastlines()\nax.set_extent([100,160,-45,0])",
null,
""
] | [
null,
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 ",
null,
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 ",
null,
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 ",
null,
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 ",
null,
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omO0TF+YhgfvltQYT6bFB7T6YA7PXdtxunSwZbFmayT9UqyX39WssmhSlEuedoE6zcknHe/bcj4qVHk5qg8eEcmaz+veMBUB02b67n/6UQefTGJz9+rjI9m3xEubMXJ3WCyWSVGo8tnqXhN27bYaHZ2GLlqiMdUhGYt9TRuqqfbRSH0vDQUna5kYJil4jWdDgwbHc7q7+tx+cBQdm63MP7qVEYOOEVOlneVzAU9jOze5V4d5QtsUpQikbIpiNoDh5Q+pboIryPvuUczyc+XqFWQDHQ6Qd8rw7nt3hjmzI9hx2ZLlW6yMmje2kjKiRJpKVKxlkomYfeaXMnUNXmD1QIhIb4/p12/Wfjlu3z6X1PWmb97mEwKT7yYwKtLc/h9e+Cfpb8Qn6hj8PAwHnk2jvXb69PlPCNPLSgbJaY8mp+lJ+Wkg4KCwFgdnMkEXNfaovqY6iK8kmync0NY+VL1l9/n9Qhh2y8WquorwSYVt5K0a4pUrDRJsGMpVNEVmolUAmc+5g6ZWSrhPu6IW8ySh2ZncMuDScQlelaNH/7HwooXc1Cdyr7GTfU88EQcc2akk55au/SwrjCiuk0mRXLXnAi2brLwyw8Vr2z0ekHL1nr+/iuwFiHuUNdIqiL4YwIJ9PNwIH1KdRFeN75mzIljwuATXDUqgnoNq75P1rK1nth4hVUr8xk5viSckUk4fHpxNh+Xu0II6jfSc/KEgxata3aJvG2zlb79fNuk+WBFLk2a6+lzpfvQTr98l8fHr2fx718WMtMcXDsxEqOz6F59Q/nzNytzZqTz/MpE9Pq6RQQREQoLHo/m5smpREYJ4hN1xCcoxCfpiE/QLBAu6mVCaW3irHYh/LZH0uUc7+UW4ehhOx+9V8Dvv1lp2FBH4yY6GjfW0bGzgTbt/G/e9l9DIIjWVjf50yd4Zc0GjfUMHx/J809k8vDixEoVbla14qN0VhDwxDPRjBuRTqcOOhISFHR6QUSEICzKv9YADRrqSD7hoEXrmhtQDodkyyYL9z/s29K/RWsDn3+Yj5RQdt8qNdnGglnJ3LawHuddHMaEy/7FWEYNMe22KGZNTGPZE9n8794YfzWjQvy1z8bXX1nQGwVGIxiNAmOIIDJS0LKVnlZt9D5vwl10SQg/72pIRrqD37ZZWbemkC0bLOj12g79V58V8PrqhrRsa+SffTayVPcBZ1Md2iRlt0kO/ZjMBysL2P2HjauGhzLppggyUhwcP+Zg00Yrzzyey3ndjMy+O5KmzYNePmsTzoQVgyf41NOunx7N6MuO8+evZjqeW2JOpAhZTKS+oGVrA7fdFcWds7JwqKA6JPn5kpfeiqfzOb7tsPuCBo10rHgpj9+2WYmOUYiKFmRnqRw97ODIYQf9BocyZFRpCbKwUGXDejMH/rIx/vpQEhIrR/x7d9uJT9RRr75vv7uoj4nnnxJsWpfPxf1K30tIqIJeL7j86iiO/WslNq58mTqdYP6iOAZdeILREyNo0qjqUvuP35vZ9bumcy4qxWQSXD8xjBCT1vmllMy5M4e27fRExylYLRKrRbOoyMpS2fOnDZNJ0G+gif6DQmnf0TPhWi2S91YWsHWrjd+2WdDrBedcYGTIiDBOnXSQfNyBxaKF7mjd3sDP6ypWK2z6OocXHkqmXmMjA8cmMHt5FCEmrSXNUTnXmW+eLYM3Xs5nxJA0Bg8NZcatET77h6gO6pKJVxHZ1bRpV3WeizPO3U+AEY3TVkkpHxZCNEeL9hwL/ApcJ6W0O+PgrQDOQwthNFpKeaQ6918RvDKkIiQREYKZ98ay8O503vyiPiZT1Qf06HFhjB4XVvx5/bdm/jc1g5WfJNCwsX+ki4k3RbD5ZwvZWSrJx+3s260SGaVwVks95/Qw8eSDmSQ10HPOBSFs+rGQb78oZOMPhXToYqRZEx1DLz/FpKkRdL/QiClUYDIJ6jfQERpaMlrKdopNGyz06Gn0ubMIIZg8M4pn5qew5ass6jfUMetuzcdDbIykMF8lWs3nWJaV+HiByY1Dmi0/FNChk4FmDau3KfDT9xa2bLJyxQBTsbXt5u8tHD1iZ94j2j1t3WwjJ0dlwWNRoCv//qWU7PrdxtdfmbntlkxsdrjjnkgGDSl/SCIjQ+Xl5/OIilF47cNEmp3lfsVhRdCqnZG/99jIynQQE1ueEP/cms/S+0/wwItNaX9umJtSSnDSEMeAm+PoMdrOO0vT6N83nUl3JnHttQZidVW3YqgM3Jl01UbirWlb2upIslJKixDiUillgTMw5EZnqKHbgaellB8KIZYDk9GCn04GMqSUrYUQo4EngGur3wr38JnV+g8N4+d1BTy3MIs75/vvqOxlV5g4dNjBLZMyeG91YrHkVBUUWUA0a2GkWQv3krFJOGiYEMPMqWlIVfOzMPBKEw8+nFgs1Uy5KZznnsll3ddmLGZJQYHEYIRP1iSWIlopJb9us/HDejO/7bBxw43hbuv0hD79QjHoIC9XZeF9WdwwPZLIKAVFEUTFKORkqZhCBUcOOdi8wUKPi0vrewvyJVKCzQq6atjrT5gczuefFnJ+dyMXdDdiNAr27rExtH8a4yaG06qNge07bBw76qBnt1Tq1dMRESnIy5Pk56vExSm0bK2nVWsDF14UwqzbIvnjNwu33pLNZf1MmMq80/oNdKz+JpE5d2Vz180ZPLokzqNqJy5Bx9AxEYzrn8w9j8ZxSd8SIj18wMajt6RwxzONvRKsK2Li9dz8YH36j4xh8ZxkfvhEcs/CeM7ycA8xNbyBWttQE0v56tYhpSxa7oSg8ZoELgXGOL9/Ey0Y5IvAUOf/AKuApdWq3Asqdaw2N1tl/KAT3DGvpLP7oi5I0lW83LNL6NHxJF98n0RiUom04utmV2VQJBHu/8tGbKxSqr4iuJM2Zs/MJCpa4cEF0eTlqnzyUSHvvV2AzSbR6wQHD9jZ8kc9Il1ObuX74FaxSEoYe1UKdz0YQ1fn0dlhl53kqRfiadnGwI5Nhdw9K5Pxk8KZcnOJ7wJVldx2UyaxcQoPPBbrQ9s9y7sfvFvAB+8UcOhfOy1a6jnwj53/zY7kuhvCiuuz2yVpqSopJx3k50vCwwXh4YK0NJUDf9v55287e/fYOHlC5fY7I/jyczN9Lg1h/AT3BGhV4YN3Cln0RA7vfJRAw5alZworJe/m181m5t2Rzrk9Qrh9bhxWq2TysJOMuDmJfqM8t13nRcZ3OCTrV6bwyrPZNGmup++gcC4dGEbDJiXvLtAkGwhJtjpWBJVB56bH/XKsdudh347Vdm3m/litEEIBdgAt0SI0PwX8IqVs47zeGFgjpewshNgF9JdSnnBe+xvoLqXMqE47PKFS6/PIaIWHFydw97RUHntB4ZxuJu8/cgNrGcuxY8cchIYKYhINNbbL2KZt5TbF5s6PZkj/VNLTVDZtsHDRxSHc91AU3S8ysnWzlbdeyy9FsJVFyzYGDvxtKybZ6FiFbKfBfo+eIbz3eSK3T89g104bzyyPRa8XKIrgkWdiGDM0jQ/fzmfk+MpJ0q4YNSaMUWPCSEt1sHWzlTbtNMnUFXq9pjap36D0xNSqDfS4qIQgt2+18uTCHPb/Zefv/XauHRfq1gJCCMHocWF8vaaQ48cdtGilTYBHDtmx2yHsrJINvXbdjLzyVQQvPJrGmP4niI5RGHB1eIUE6wt0OsHoG6K4Znwk238x892XBUwckkzDJnpGXB/JwGHhXg0dXUmytp/wqq3wRO7bfzH7ZF8vpVSBc4QQUcAnQHt32Zx/y1YmXK75HZVWgna9wMS8ZzWinb8kgS49S+/6mpTyNo1lSbUs9u6y0a6j/za+AoHoGIVnl8eyeZOV+x+OIsFFAu5+YQjdL6ze+fpWbQwc2F/y7EyhArO55L03aKjjxRXx9DrvJHm5kphYrZ+ERyg890oc469Jo2UbPed2q959JCTqGOTFwbg3nN/NyIefxvHNWgvPP5fH0SMOzmrhuasZDKJ4QrGYJTdNyiD1lMqEWyXXTIwplqTDwhVuX5DE9p/D2f2bmfEz40hV3bc3XKncYQ29QdCjVyg9eoVy98I4Nv9YyFsv5vDOyzk88FAkF/b07bl6kkqD5FsxbB6cSHXpEU6XHiXCw0uLK7bZl1LmCCF+BHoAMUIIxUnAjYETzmzHgCbACacON0pKmVntRnhApUk2XNi4rJee6BdjufWmNO57QnLJ5b7rw9xh759W2neq/faLXc810vVcbTKoyhLP3QZCmKJJb1FhkkM5juLPYSEgrNrnorp2bLbQqbOB+Fht4t29x87nHxew5rNCLrokhDtvzmDl50nlJM3TASEE/Qea6D/Q+2pn1Ngwnnksl3bt9byzooCWrQ0sfy2SW2fmsPXHAu5+sh7xLgc2zr8knPMvqVhqz3eSr+pG5RSjq9gfrl4vuLhvGD0vC+X7rwq4785M2rbXc8/9UVV2hu6uvwSJtwTV0ckKIRIAm5QyWwgRClwOPAZ8D4wE3gcmAJ85f7La+XmL8/r6qt+5d3hd33o6Wnpe9xCWvR7HwrvT2b7JXK2b2LvLSvsalmTNUucxFajeU0W/L0qVcQz93Tdm+vQtkZaMIQJLGYc67TvoOXbUwbwHshnSL5WZkzPY/YcNRYG5j0Qz/Nowlj2Z7dExtS/+DSpyuBIopyuXXRFC+456bpmSSfIJB3PnR9GsuZ7nPmxC204mbrzyCJu+y/NbfVmO8FLphD2mVCqCEILLBoXz1fpEup5rZOTQNB5fkENujn8OeKqydloWuEPRqcpAwSEVn5IHNAC+F0LsRCPOr6WUa4B7gNuFEPuBOOBVZ/5XgQSnLvZWZ76AoVo2U527Gnl4cQJz/5fGm1/UJ7Fe1Yrbt8dGOw/e/CuCIkr3UF86gT982/obWZkqO3+z8dxLpUnWai3dvkaN9bzydhwfvV/I/fOi6NzVyNUDUnlgfjTh4Qqt2xg4fDDATsl9HGg2N5KJp403IQRPLSmvW9UbBJNnx3PBJWEsvP0kW38sYPq9CcU2sIGCK9ECROoLGTQtimEjslj8ZC79+6Qya3YkI0a71zXXBujwHPKoOnAdY2XHX7XKrYZDQCnlLig2h3b9/l+gu5vvLcCoKldYSVS7t3a/JJRrrovg3pvTyMqs2ln6nGyV+ASN/Dw57FCELJfOFKz/1syFPY2Eh5e8DqMRLG7Uim3aGpgzN4puPUJ4ZXkerVrr6dtPW5Lb7RJdLR30UN5TmK8OWjp3C+WVNU3JyXIwbchRvvk4h6MHrcX+HGoKlvgYpj/WhPmvNuajT61c3iedV95XsdvPnL5YGfhTsq2oL9R1PxJ+sf6/YUY02ZkqIy89wbU3RHLt5CifHaUAWmwqfd19iNXF9q1WVIcW+yoiQkFVtXhdZSXZsjh+zEFBviQvT+XgQQer3i2gbfvar9v2BQ4EiS6608RYWLI0kq+/MPPNmmzeWJRGXo7KWZ0juPKGJLr2DkywTndo08nEM+82YefmAt5clM57y2xMmRVF/yFhpSTb8ACHOjqTUIEqoM6j2iHB86WhOBTLkUN2li7KY9MGC1OmhzNmfDghJlGhdYGqSro2P8H2Q40rPPfuS0iYQOqMAoUwxUF2lspj83PYvMlK87N0/PG7jZgYhXmPRtOzV4hHvZ3dLpn/QA7ffWNGUWDKLZGMHBNWzs9BEXyZxGqLp3xfkJbq4PsNKq8uzqRRUwO33BdHizaldftHbfFeyzEpFZ/2ilQKPV6TUvLPlixeXJRDRpqjmGxdff0GimyLJHnFww5aVYQWT7/xNLY82a1WBkIIufagO4ur8hjQYm+dCz/jM8lWZvDt/8vGkqdy+fMPGzNui+Sq0eEeCdRmk3Rrc4KtB5tUWGZdJNnKktqOLRbyclU6dTUSl+Cb7lhKyc7tVjp0NpQ7WVW2jjONZAGy1BBsVsnHb+WwYlkWfQaGM+X2WGKdp/fSHe69nBWhQA2pFskCxCiFSCnZttHCC4uyycpUuXl2NJdfqVndBIJkk084+N9Nmeh0sPTl2GJ1mztUhmxPF8muPtDJp7xDWu6qcyTrVUavSsjkNm07FAG+AAAgAElEQVQNLH05jmdfiGXlm/nMuyfLo97K4QBdDTpEqs16n/O6h9D78lCfCRa0TaNzLgjxSLBApdrlq26sJp/TieP2ClUnBqNg9ORo3vmuMQaDYNzlx1j5YpZP4Y7CFAsOKdymykAIQbeLTby6Kom758Wy5LEs3vKDH2ZP2L7Fyv59NoSAUUPT+fsvzxNFXQh9rqL4lOoiAnrXXc4x8taH8dqsOyWdgvzy0qjDLkstrbzBk3lSbe5AZypqgoDT0xyMujKNxx7yHkkhOlbHrQ/Fs3xVA37fZmHc5cfY+FV2lR3FF5FtuiOiVKoIQgi6X2zi5Q+S+GhlPiteDAzRXjUslKWvxHHsqAOrWXLdqHT27fHu5Ka2jhNPE111Jr7aAq/qgn1Hqh9mO98mWHBvFn/tsbHsjXgMBsGJ43aSjzs4dNDOy8/lcv/DUZxMdlBQICkskBQWao5ZEhN1DB8dSqt23u1offF1UJNL5pqsq7ZZW/irXXfMyCQqWvDjdxYWvRBL566l+0GWhxNfANs3FrJofhYJ9Q088EozzyorL2Z9Di+ySJF/hOaG9FLfpyTbmTo6lbHXhTJpasXkXFVkZqjMnpHJzl9thIYJlr9W/hmVRUX9sqJr7lQG/lIXfPBPOQsstxjV6tc6py4IOMkWvTQpJcsX5/HCklxMoYKGjXQ0bKSjQWMddqtkxzbN1V5YmCA0VCE0TBAaJvj3gJ2PPyggqb6OEWPCuPDiEBKSdBiN5Z+zO5J9f0UekVEKZ3cy0PQsPVLxTsRBkq0+/NGuP3+3MnNKBmt+SuL26Zlce104vfu6P0HmiWxPWcO5/ep/GDOrHj2ucO9Q3V8k6w7pyVbmjtrHPXOjGHBl9Y4rl0WRzXdhgcqNY1Jx2CQnk1WWvhTLed08E60v/dJdnkCS7Ht/n+9T3mtbb/9vkawVpdKDyWKWpdwZpqU6GN4/lZfejKODh6O1Dofkxx+srHq3gD27rJxMVnn+9bhyA64syW7daObBOzPp0NnInl1WsrNU2nYw0r6jgXadjLTvaKRpC305dUWQZKsPf7TruadzsFnh9jlRjB+exvRbI+jZq3JOicxSxw/fFLJ0UR6LV7dyK80GkmQBMvamcceEEzz1RkPadtImA2+e6XyB68GajDQHE65JpUUrPfv32Vj1dT3iIz3sg1TR6iCQJLvy724+5R3XemudI1mvW07enLtUFmX9xT4yN5tho8I8EixonpJ69zUVk+qmn8w8+lAOqaccOOyaKZPNDla7wG6T2O2anen33xQy485orhym7fJmZTrY/aedfX9a+fHbQl54JpvMdJULepp4/HlNjeENvlg5FMMH9YW/yLGypFYXbJITEnXs32tj1bv5ZGY46FLF6Bm9rzDx0qJs/l6fzKX9y/vZyFJDyXJUz/9GRWjbMYQ7FiZy300neff7phiMglMu9dXXa4RbnbMVcQk6nl+RwKQRp7Ba4ZmF2Sx8zL3kXpXTYDpkse+qQFjxeJvo6jJOa6CjdWsL+WuvjUcWVc5dXY+LQ7isn4nff7Wh04HeoDn1EDqB3iDQ67X4U6Oui2CAi2f+mFgdl/RSuKRXyWDNyVK585YMVr2Zw/U3ah7FauvmgD/h7zYGgrTr1VdY/Hgh331tZsWqBCIiqzbhCyGYels0Ly3OdkuyADEVSJbeNrt8Qe8BEby2KIN//7bSpoN71UZ1oibY7ZImzfQsfjWBCcNO8dkH+VxyicHvKgoIzKrpTD6McNpIVkrJgvuzCY8QzJycgeqQGIyCBU9Ee42TpSiC2+4pP0tXxcl3VIzCnPnRTBiexsAhYSTWO3Nn1ECiLGl7I/GiFVJF+Ro21pOXK1m0PJbmFbhK9AW9Ljfx4Ox0MjMcbmOm1QTadjKx73eLR5KtKg7stzGyfwotWmshlYaPCefIITsP35dD+w4GmrkJGun63GvDqkatBfcQKJxWSfaJ52IxF0oUHRh18OmqQt5+I5/Zbgg0kGjewsA1Y8O4fngqZ7XSExerEBOnEBunEBOr/W3cRE+7Dr5HYw3CN1Q0wFufbWTHPw0xGAUOqid9K4qg7dlG9u6yclFvf29AlVZjmIT7SApdupl496UsWrU3cvY5VXN47w7RMQoRkYJ5T8fxxgu5IOGv3TYGDjax7mszk6dVLImXfa6ng3SDkmwFcCDcdn5vgdiEEHRzcXStQ9KosY5rBqdx8B87TZvradZcR7Pmepo215HUUF98fFBKya6dNlJOOoiMUoiKEsQn6oirV/UXdcvsKC7tF0pmukp2hoOsTJXMDJVjR2xkZar8tcdGbLzC9VMiuGKgySf9rStyc1TCI4THI5DVhc0m0es54yYBg4sVSXU3Ett3MrJvl83vJFsWZUk3Q40gTslj0MhIDEbBvdNO0qt/ODfeGUdkVHmp2mKWCIVyFjQpJx08/2weN04Pp3HTkqEbl6BgMUuaNtcz6roIlj2VTUSkpjb7Z3/lT5udDinX2+ZiXYZfJFl/vYimzfWs+iKBfXtsHDnkYPcfNr5cbebIITtZmSqNmmiEe+SQA1WVtGxtIDdXJSdbJSVZJSxc0K2nie49Q+h2UUilTk7pdIJOTvtCt5OGQ/Ljd2ZWvJLP04/kMG5iOCPGhBEV7b1zpKc6uHZQCs1bGliwKJbQMIWjh+1YLdKjqc3JZAfbNllIS3UwdGSY29DVUkp2bLXyyXv5fPulmZfeiuO87v5ditY1lO2LrhuVHTvr+ebL6vk+rioyVE2aPH9IJEt6J/LWkye5/oqj3HJfPOOGKaUmx7lzsvnxewvXjApl5JgwmjqX+6s/LuT9lVqE4lFjte9++q6QZU/l0LKNAb1BUJCvEhau0PUCPd+vs1S4oewLaopwa9uReH/itKoL3KFZc71bHVJeoeTYEQeH/7UTn6Cj63mGUh1TSsm+v1S2bDSzdnUBC+7LpH4DHe06GGnUVEfjpnoaN9VTr76C0SjQ6cGgF+gN2tHe7EyVzEyVrEwVS4HKed2MJCTqijuZTgdX9DNxRT8Tu3fZePbpXJ5fnMvt90Ux+rryy7H9e23s2W7GYpF8tcbMiJGhhIYJ+vc4SUSEoFlzHcnJKkuej+ZCZ3wsKSULHs7l++8s5OaodL9Qc384tE8Kw0aEctVQEzYrpKQ4OHjAwacfF2I0CoZcbWKtKmnXTl+hJGdws2EhpSQnW5JrFUgVLBbJxh8tnDjuYOCQUNqdfWZ49QKIT9Cx709rOQuRGKdvgiw1sBJuESKi9Uxf0Jh9w2N57YFDrFul8ODCaJo116MI2LHNyo03hZOWpjL66nRattJTv6HCr9ttXNDDyMEDdux2yar383htWS53zI3h0n4mhBD88auVho119OprwmSQzJkbVWpDrToWDIEk3DNZkvVqJ/vHkUbVrsQXXZq3PL68VNeNL7tdsvdPGwf22zh+xM7xow6OHbGTmuJwmnlpeex2UBSIiVWIiVGIjlUw6OHX7VbatjfQb6CJKwaYaNBQh9Ui+fF7C6s/LuCXjVYu6mVi4k0RdOxSWhrNzVG5+rIU+lwaQniEIClJYcq0cHQ6UbyslxJWvFHAeysL+XytZj7mcEjaNE9hzTfxtG5boh5JOeng1Zfz+ekHK1HRgnr1dDRoqNC7TwihYYKffrCw4Wcr736SUOHzMQiphTHfYWPHdhu/7bDy2682Cgs022VF0Z7Fud1C0Ovg808KeXJpLIOGVJ58fN34qgl8+HY+H76Tz6mTDq66JozZ95W4RfRls9Qs9Ry3e7aAsXmJSlxRvLGWpLDitXxefj6P51+J49wLjKz/1sz9d2Uz6/YIhowMZ8dmM5kZKjYbJCYp3HVrFrk5kuhYhddXJdLsLG0iPJXiYGS/FN79MolWTSs6ueWlwR7gbgx2aHrCL3ayT+7p51PeO8/+plx9zki0K4D6gAN4WUq5RAjRBVgOhAOHgHFSyjznb+YAkwA78D8p5TfVaUNFqPUkW5nB6MuSwxc7Vx0Si1my8WcL36418/06Mw0b6Thx3EGrNgaGDg/l0kGeVQVPzc8mN0flqae0DTyLRbJvj02z0d1rY+9eO/v32YmIFHTsaODpJdFERChIKWnfMoVzzjWQkKgjMUkhKUkhIVEhMVFHVpbK/r/sxSk9TaVlKx1t2xkYPjqswlM+WtslH75XwJLFeVzez8Q55xo451wDjZvoilcF+w6ofLaqgFXvFjB2ohaCvLL6Z6gdO9YAv++wMHt6Bo8sjuO87sZyB098JVlPOG6PrRbJtjOcAmDFq/ns3WPj0ae1qAyH/rUzc2omTZvruW9+aYsbHRJVleTbdRgMgsfmZrJ5gwWLRdLvylBuuzemOFacO+TkqoSHi0rr7wNJso/vHuBT3rs7rHVHsvWB+lLKnUKICGA7MAx4E7hdSrlBCDERaCGlnCuEOBtYCVyAFmBxHdBaVtXJhRecNpINdGgMT/CVZF1hs0l+22GlYSMdjZtoA8oT+Z84ZmdwrxR6XBJCbJTg4EE7B/62c1YLPR07GWh3tp527fW0a2cgJrZ8GcePOTh21MGpUw7SUlVSU1VOnXKQmqISFa3Qpq2eNm31tG2np0lTXTFpVBQWxmaTbPjRwuqPCtjws5U33o6lq4thf062yhefm/l4VSFHjji4algo11wbRotWVVcV1AaSVVXJdcNSGX1dBENGuLePrS7JAmSpbg44OEoCPXoi2aP/mDm5OZnoaIHFAo8vyGHTr/WK/QFbzJLly/J4/60CZs6OZOS4sOLVTWGhyo5fLHz5WSHbtlh59rUELBZo39GAXi88kuyJ4w769DjF8tdiufTyylk4BJJkH9k90Ke893b4ymt9QohPgaXAKilljPO7xmixvzoIIe4BpJTycee1r4CHpJRbqtMOT6gRnWxtGHDVgcEg6NbDtw2l2HiFeU/FoqoQqlO5bmIYZ3cwEBrq/RnkZKtYrZLuF/onqOSxI3ZWvJbPl6vNNGuuY/iIUBY+Fk10jELqKQfrv7Pw3TcWtmyxckkvIzfPCOeCXqFVklxrI75aXYjqgMHDS6s7crJVPnk/nwsuDKFVh5CAWGS4RsR1NU9yddf3x6Y81ryWzznnGcjOkrRrbyA7WyXRGW4+xCSYOTuKAYNDeeieLJYtzuWc843YLJLtW62c3cFA78tCmDM3ysWfbMVChM6ZbfXHhZUm2UDCXVThqkAI0RzoCmwG/hRCXCWl/BwtpldjZ7ZGwC8uPzvu/C4gqHUbX3UdoaEKg4cXOWuuOOZZ6ikHa9eY2bnTxu+/2TiVohJiEnTrbuCe+yJp0rTqrycvV2XSuAwuH2DinY/jadZcj0FI/txlY9L1mRw8aOeSXiEMHmLiyUUa8QKY/bDLW1sm1fffzCcl2cHUsekk1VNISNKRWE/H118UEBml8N6b+egNgv5Dwug/JIzmLQO/yae4kGCH80P55m3FbRBJV7Rua+DtjxNIPu7g1+1WFEXw6OJYEmIr/5yT6inodPDtWjPffFVIv4G+69sr4/y9svCHnaxTVbAKTceaJ4SYDCwRQsxFCwNeZMDsrgEBO+YZJFkP8BbV1pejhWYvHWfjZguPzM+lQQMdjz8VzXnnG7Db4OWX8hk2OJ1Zt0Uw8YZwCnzogJFKyeCVUjLn/mx69jTy0AORRd+y+x8HUyZkMntOJIOGhJayw7SdgSeJl78Vz4njDtJSHKSeUklNcXD8qJ0+l4cy+RbNImTXThtffVbA1NGnGDMhnBtmxngp1T1OHbfy24Z8/vmzkAO7zRw7YKH3VdGMubU+0fHu31+ztibSTzn455SB2DLmhvFKaVMzIQQNG+tp2Nh1yFb+pQkh6H6hkS7nGln4YA59LjN5DFfkCYE4du7pxNehbWkc2pbm9fdCCD0awb4lpfwMQEr5F9Dfeb01cKUz+zHANRRLY+BEVe/d673VhE62NsFf9ni+kKwvnTHzhI0li/NY942ZSVPCmTgpjPBwhaNH7Ey+IYtevYzcPtf7wHcl2Y8/KmTZsny++DK+WE1x8qSDYcMyuHlWBNeMrp4zlKq6yqvNSDvlYNzQVG6dE8XAISXPx/UdunOnuG1DIe+8ns/eHQWc3yeC1p1CadnBRFIjA5++ms73q7MZfmMiV02IxxBSnmyX3/Uvqiq5/+lEtwdVEnUa2brTubszyfMFi57KJSdbcvSInT59TYy9rur9oV3TZL/oZO//42qf8i7o/Knb+oQQK4A0KeXtLt8lSilThRAK8DrwvZTyDZeNr+5oaoJvqesbX7UJtY1kw5wbcQcP2ln8dB6bN1uZfnM4Y8eFkZWlcvGFqWz/q4FXPakryQ4ZnM4dd0XQq5dGCsePO5h4fSZXXh3K1Fuq7+wkIMvFWkDK+/fauHFMGktejaPLedqzq+gd5uaoXHLuSaY/3JDeV0VjCitPoocP2HjjsWSO/G1h4t31ubB/VCkdcLg1h9uuO0nbTiH8b25cOf1wEcn6E8eSVa6+4hRPLo3l4TnZrPkxqbh/VVZK9RfJ3v37NT7lfbzLR+6sC3oCPwG70MR7CdwLtAFucX7+WEp5r8tv5gCTARun24Rr95GGtWIA+Au1lWSLsGe3jaefymP9OguKAhf1NPLiyortX6GEZO12SZtWKdwzJ5I/d9nYvt1Kfr7k+glh3HRbpF82eU53fwhk/T99Z+bhuzNZ8UkijZpUfLhDVSXntE5m856GbpfcR+0xxbrGnRvzeHn+CS69OoYRNyUV54nX5ZGb7WDG6JNcNjicCTNKr1oCQbI2KbhrVibtOxj4ZYOFcy8wctOsqnmg8xfJ3rlzhE95n+y66szzJxtEzeLsDgZefT22lC+Cgkr0e71esPCRKH7dYeOinkZm3RpBy5aaHWyBWqf6pkf4QgRVJeJefU1MujmS6denM2JsGB06Gmh3tsGtTbSiCBKTdJxKcZTyJVCEJvosClRtM61fL2i1LJ5Z41MYOikBg7GkvMhoHU+vqMf0EcnEJugYcm1kubL8jQlTwpk5JYNX3olnyth02ncweIw6UROoq0ESfUGlSbambF7/66iOGdWYsWGMGevHm6mDqM5O+NgbwklIVPh1m5V1awrZv89OfLxC774mbrgpgvoNdFjMkl82WLDbJKkeSLYsWrQx0ry1gV1fpzDg6tJqm4QkPU+8Wo8Z1ybT/+pwQkyBJZ0OnY1c3MfEGy/lc+f90Tz7ZA6XXBpCVoajwvDigUJdDZLoC3wi2f+CE2tX1GQoF18sB3x5/meKlFobIISg/1Vh9L8qTIsi4JAcOmjnkw8KGNbvFGd3NPDnHzbadzAw8aZI2nfy3a551MQo3liaVY5kdUhatTbQvlMI61fnMXhUZMCEF4OQmsrggSiG9U/lh+/MTLwxgi8/LeSeW7NYtyHRp0nDnziTHcT4pJP1hqAk6x7+mpzq2iSniIpPoNUk/N03s9PtbN9i5YIeRmLjdF7LL1IXFN+PQzLq0uPMfSaBLueXX55v+r6AF57K4s0vGpCkL31SLBDjLC3VQVaWStOWBn7dauX6kek0b6Hjk68SfTpA4y+d7Iwdvi29lp73Tp3TyZ65ipAgTisMQlY61QVEx+vpOyiMqDh9lUhPpxPceHsMj96Tjrmw/OmsHr1DKSxQ+WNH+aO4OmS5VF0kJOpo1dqAUYEePYwMHGzi0EEHCx/MrnbZlYED4VOqiwiSbBA1ClWVHPrXzhefFvLJqgIs5hKiKEu67kjFX+RyOtF/aDhtOhh5dkFmuWuKIhhxXRQfvpHjU1n+fi533R9FWLhg1XuFrPu65nzv2lWdT6kuIkiyQdQo5j2QQ79eqax4PZ8vPjPT9+JTvPpiHvn5lYgCjHuprjYSsUnYyyUhBHfNj2fLT4X8sDa/3G+uHBHB79stXND1FKOHp3P4kO/RDarb9gYNdbzzUTwAM24smQSslsA+TxXhU6qLCJJsEDWKO+ZEcvOsCA4dtNO+g55FS2P4Y6eNq/qlcejfEjKpjnNpV9RGEjYJOwnRKo8vjeOxe9M58ndpiTEiSmH1L435Ym08J0+qFFTGhs8PaHe2gZ+3J7FuQyIATz+aQ+fWJznwty1gdTqk8CnVRXgl2bqqBwmiPBThPQVaNxoRoXDrnZGs/iaRPbts/PSDhWeXxzLtlgjGj0hnz5+BG8hlUVkCVlXJlo0W/HX6slNXI7feF8PtU9IoyLZiEI7iZFRU6tXXkZWpcvSIw291VgTXiS0xSVdsYdChs7Z5N+HaDI4drXzMMN/qVnxKdRF1866DCAiKyKUqm1auSZXeJdH6DXT07BWCxbm/M3psGA8siOKGcRk8sTCHo4cDM5h9RRHZ2qSCTSoUWARzbs3ixjFp7NzuPhptVXDViHB6X2Fizi3p2O2lH1q+1DHv6VieeiKPq6/K4Nsfa24CckX/QSZ6XRqC1SKZNiGT7KzKqXZ8gSqFT6kuIkiyQQQMqoTtW63cOCGD22dm8tWXhez/y8Y3a8288nwu3641o9eVSI/9B4by4WfxSAmjhqYzdUIGK9/M56F7s9m62XN0gfQ0R6kNtEBg0YIs8nJVZtwdzco38ovJtzooWiXOmhODTieYMDSFj1bmkZtTQmKXDwxl+dsJHPzHzntv5pMvdeR78RBXVbiuaFwhhGDBE9GYQgUSyYypmX7X0QZ1skEEUUkc/MfOtIkZ3DEri8v7mzj/AiPvryzglhsz+fDdAtLTVa4ZGcrEySURBHRIzmqu4977I9myJZGhV4Wwe6eVJg0V7pqVxcP3ZJF10s7H7+QzbGAql5yXwv13ZdG/dyp3/i8roEvqndstTJ4ZxYjxEWxYbyY/zzdpzpeDLXq9YNFrCUyfHc2Wn80M7nmCubels3WTBVWVxMQq9Owdwoljdg7srxlptizhJtXTsWhZLJkZkpxslcfm+2b94CvOZEnWJy9c/ghy+F9EbTuM4MaTXkDqOX5SZdSQNK6fHM74CeFunad40/2WPVWck6Py+GO5vPduIX37hjD+ujDiG+pZ97WZC7obmfdANiNGhzF+Yglp++NAhFnqOHHUzvirUlizuQEmk8KAbidYsTqJpPp6n8IZuYMqPdt9ZqY7WPNJAZ9/mEd+nuSqa8IYfm0Ym36ysOTxHGbcEcWE8Z4jOgRyPL63soBnn8olPU1l3YZELr841S+HEUZsvMmnvKt6vlDnDiNU6uxckEyD8AaLRTJzWiajxoYxaWr13SoWISpKYeEj0Tw8Lwq9XuuHZilo2UqrY/HzsYwamkbvy0KKI0r4Szj47IN8Bl4dhsnpT8AYQrEuuapQhEQpG0vOqX6IjdcxbkokE6aEsW+3jU/eL2DCNWl8+l0S515gZPb0DDJTbNx2R+AdyZTFtePCOHnCwfNL8lj1XoHfyq2rqgBf4BPJBsn1v4Ei6bE6URKWL80jLk7hppn+I1hXFBFsWRQtyMIjfNeAVUTCRX2+sFDl0/fyeH5liXvCqGiF9V8VcP20SPeBTKqI8lKxoH1HI+07GsnLyeC6Yam0aGVAqtCo8ekzzP/fHRGs+9rM8WMVh1eqDOqqKsAXBF0dBlEOFTkAc3gh4AYNdGz40UqEHgr8vwntEc88nsvkaRHExflnm0GHxCx1fPxWLl3ODaFNGz1F4V4eeS6eySNO0atvKG3a1AzZPfh4LL//aiU9zcGFvUIYOsy3wJ6BgBCCL9YlIqXk809P+qXMIMkG8Z+C3S6x28Fk8r3j2+2SpUvyePP1AkaN1oLzhSnuGVmHwJ0IaK7ixtXyJbns/8vGk4urFp/LE6SUvP5CLi+9k1jq+7PO0lOvvg5HoR2dy95xIFd8ISZBt4tKiFVBLV5xnC6/D/6M8hskWT+ioodZky4G/2uoaNNLSsnff9nZsN7ML5us/PqrDZNJ8OjjUfTr55sj51dezmfjBiurv4ynebOqdSuTy6B1eNGnJp9w8N4qM0cO2fl9p4233o/H5IPXqMoiJkZx68glLl7hwN92OnYpcXNYVv1QU2q2sht83jY4q4v135p59ulcFj7hv0mtOiQrhGgMrADqAw7gZSnlEiFEF+AFwIQWZuYWKeU252+WAAOBfGCilHJn9VrgGX414TpTTTDOVPy63cqhf+3Mn5vD1ImZJJ9QGX9dGBs2JbL8xRgefjCXu+/K9upX4PAhOy8tz+fpRdHVCmNeGfy+187KN/Kp30DH2x/EkVTP/8t2s1kSGi7Yv6+82dR1UyN5aWluuQME/wX8stFCQqKOKddn+K1Mu1R8Sp5+DtwupTwbuBC4WQjRHngCeFBKeQ7woPMzQohBQEspZWtgGhoRBwyVItkggZ5ZuON/WYwaksa7bxXw9HMxzF8YRf8BJmJjFbp1M7L2m3hsNsmgAemcTHa/ySGl5L57c7jp5giaVlGCrQo6dDRgsUhmzY4gLt49wXo7QuwNq1bmE5+gY+jI8HLXuvcMIS5ex1erC6vblDoHKaFBQ4WPv/Qee85XVMdOVkp5skgSlVLmAfuAhoAKRDuzxQDHnf8PQZN8kVJuAaKFEPX81pgy8EqyRSdbgiQaGPjLm5Q3P5wxipZCLPDJWwVMHZ9BQa7k1y31+O7rRPqcbyRMlCaryEiFZxbFMGJkKFOmZFJYWP5e1n5lITNDZdKU6oUZryy++8bMWS311dILeiPgHVssXDkszK1FgxCCKwaa+PP303PU9XRi5m2R/LXXzqybyrtqrCr8dRhBCNEc6ApsAW4DnhJCHEGTYuc4szUCjrr87Ljzu4DgjNv4qslotHURD83PZv9+O5NuCOfSl0OICFc4u33JXFuWaAHumhXFv/84uHt2DkuXRZciNj0QH6cQZigpI0QoFEj/mfeUxclkB4uezOPtD+ICVgdSsnObhYcXRGESpdtidh5rNZkE5gAf562NiI5ReP/TeFZ/Ushdt/rHubencZu58yhZvx91e60shBARwCq0EN95Qojpzv8/FUKMAF4DrsC94V3AXmStJtmqnA2vLb5nH0AAACAASURBVH5EayO2brOyZq2Zn9cnERPj+7MVQrD4yViGjkhl2PB0GjXUER2j0LSpjvbtDGzfbiMjUyUutmKyLoLq4R3ZfLAusNkkM2dkMWFSGK3bGrzmryoO/esgPEKhXv3y7SgiXZ1RYLbI4g2umup7OmSpTbXT0ecVRXD1NWF+I1lPh7hiujQlpkvT4s+HV2x2m08IoUcj2LeklJ85v54gpfyfVr5cJYR4xfn9MaCJy88bAyeqc/8VocZJtqId17rqL7Iu4OcNFqbdnMnip2MqRbBFMJkEH76TwIatZrKzJVlZKv8csLN6tRmbTfLH7zb69Kme7abBdenvgTfmLcwlPDxwhx2KoKoSgxcOP37UQYNGJUPodB3aOd2E6w/44cTXa8AeKeWzLt8dF0L0llL+KIToC/zt/H41cAvwvhCiB5AlpUyp7g14gl9JNngyrHbii08KeHJeDi+/EEvPi6pOhFFRCn37ljfpstlkcQjzEBE4n0PJyQ7ee6+ALZuTULzsXJWV9iqLpCQdaakVW1WknXLQKoDSdFVR1s1koE26/IFqmnD1BMYBu4QQv6FN0fcCNwJLhBA6wAxMBZBSrhFCDBJC/INmwnVDNW+/QvhMstoGiucBpKMGj/cE4TNSTjpY+EA2n3+SQPt2gSEEQ0VHxPyI+HgFu01SUCCJjvaevzq+C0LDBIUFstQEUhbndgvhu7WFjJsUWKm6uigiXX+TrT+lZoda9clZSrkR8KSfOt/Db2ZUucJKwofICEpxCqIEvlgF+MtywJeIBmFCdZsO7bXSuYuBzu1CMKB4THUBRqPg7nsiuXpYOv/4weVfRe9l2xYrZ3c0VDiB9OwTwtZNFqwWjYy/Wl1A2qnAbfidyZBS+JTqImr1xldV4MsSsa7qrSqDLz4vpEULPX/ts9G2rffXbEDB7AeLABWJUk21UUUbYFNvjCAuVuG60RksezmWc883esxbrXswq0TFKG77U1H/iYvX0aK1nifmZfPzejNCwPk9QljwTGxA7ulMxplsIuo3knWg+F1lYHPjAd6badV/VW1hLpQoOk3a++03Kw89kItQQKpw95yaXc56sh7wF0aMCCM8TmH65Exm3xPJiNGhXnW0lUXjlkYO/pPr9pqrNcHwUWH8tN7CM8/H0rSlgcG9Uzj4t40WrQOnqy1L/GeC0FADIcxOG2p8nWiTOp9TEL7BXCgZdU06C+fnYrVK7rkjhwcfjuT7nxKYNj2cPpeePo9NVYHiJQH0utTEG+/G8dH7BYwYnM6vfoy7BdqgL/QhSuzIseE890ocnf/f3nlHuVGdffi5aqvt1V6XdbdxN8bYlJhm0yExEDokBAidAB8kdFJIAdKoIYnpoRfTA6G3YGqMbYwL2Ab37u1Fu5Lmfn9IWmu106SZ0Uq7es6Zc3al0cxoNPOb9773LXv4KCsRXHBJETdcUUdbG2nLhFRLPnEau4U9137GJAHp0V1ywmk/Ukp+eXU9/ardvPB8GyuWh9i4Mcx+B+RRVOTi3PML6de/d513F1AoYPpELy+/UMl55xTwfxfWceM1DfhCkkKhX67RDI8+2MKJpyWfxXb6WYUMrnHz++vrOtvh9EQaerpF1yq92SeblMjGUmy1lkwgXRN0mXLhPjC3hdWrQtz99zIOOTSP+R+2c/Ip+fzyusa0tJHuaYQQHH98Ae+/14+tW8OceWZdZ0Ebr9Be9K6SujqFfz/fyulndq9ZYOZ4fv/XMt5/s401q/U77qZTeMMIU12Ek9menfdAb+7xZbp2QaaIaG/DTORArO5A4vLF++08dF8Lzz0wgGFF+Vx1fgWPPNTG7L0KefWVAOsWC6rdfqrd5soVZjNFRS7uv6+cgQNdnHxKrWHlMNB2Rzz5aCuzD/PTL8XKXvW1Ci6XYMjw5Kc8rIiK3hA+/r2Y2NopulZRFGFqyUZ6pXLGh52pL/rFVDLFSjXi+l81cNftZdREs46mTPQxcZyXP95RzwN3VbHn1OR8sW4hdBcw5y91Gi359HgEf/5zKePHeTj/vHo6OlJTkJdfDPDDUwtTvjYWfNbB9H3zNFvlJEM6rLlMEN3e7C7I+BCujgQ/rpnogVQ7iGYbO2sVpkzqGsL0/CPVuFz2Vq1PBjP1B9TE2G3T8QohuPnmUs45r44rf97AbXeUJhV5sG5tiB07FSbvoR0aFhl6d99m7LorLHIRUKlYZheJ+7a7mFG80KYrWyxbXQFm6BFLtkO6TS851JFS0tQkKS5OCOdxix4TWDNoXXBhKTuXIPqLER6P4G93l7F+Q5ifnl3Pffe1mK6W9cLzAQ49LA+3O/lzGHOrFff3sWO7QgduOjQTkewjZuE6MRJLl4UrpbklG7FdZIPSo7nkhNM+ausUiopE2lJas438fMGDD5Uz++A8Pv6ogznf38mK5fpZYnV1Cg890ML5FyQ/4RVPZX93l8yvmNjGlnS4o5xwfzkpuL3ZXZC0yOqJaFDqex+U3ukC7hFWrw5TMzj3wNLCjaCi1M2ZPy7kwfvLOe+8Qk46oZbtW5RoI8fu3De3hSOP9jN8hMF1bHCzV1a5qa8L67amSfdcgFOCaxd9WmSTEdG+hlFdAjORA16kiaVrnYFvloc5/6I6zv5xUdbUHehJhBCcfFIBBx/i55l5bQSkRIEuS3OrwpNPtHLO+YXUKtaytTxeQUWVm20aLXv0SIfoZuIkrzS5ZCO9+g7N5HjeVPnwowDHnbKdG28o5ewz7E2XjfeLqi1WfaU9zXnnFfLkE62c9ePaLq6D1laFO25tZtp0H8OiYVdWr52aYR42rLVexCYd1m4miK5UhKklG8kK0zQYN3kQlG4TKX36QeAB6cEv9NfJRLZsDXPGubU8NLeCA/bLvNhXc0Lb/UZJ12Nv0kQv777bjwceaeGM0+o4aFYeZeWC555pY/pePq69odhwG3pCG39dzj6ygD9cvZN75g2geqC9t1mytQuSTYHtiSLg2eoKMEOPiWwwDbOuvY25DzRzwnH5GSmwVogPuGuRoN6CKYLfYriSzyc48+xCjj8hn3vnthAMwguvVFIzxPqtEBMnRQpO+EkpCz9r538ftXP08bu27UQBozACN7KLr9iusK50CW62Rg6YwXaRNYoesCsesq+xszbMw4+18M6r/Xv6UHqUgBSGEy7FJkzj4hIXV1xpbLlaYehILxvXhbqIXwqRYSnRZXJO2COQTgquFUtWCFFDpMX3ACAM3COlvEsI8SSwW3S1cqBOSjkt+plrgbOJDHsvk1K+YeHwdUlaZHMhWOln1eogJ5+xk3PPKmTYUGcGH3bUks0UOgzMoqAUeNPQjXjwEA9ffBJwfD9msFsgbffdWnMXhIArpJSLoh1rFwgh3pRSnhJbQQjxF6A++vd44CRgPJEmim8JIcZIh4p9GN6xOVHVxuhGNRPCWiy0f4JgUPLmuwEuv6qOX15Vxlmnq090tUtj/3IQJReJEEfQIR9gfKW5QUO9vPxMs+nPqhU3csq90HUfPT9WtyJvUsotwJbo381CiOXAYGBF3GonAQdF/z4GeFJKGQLWCCFWAnsBn6Z+FNpkxcSXVcJqkxUG95ivh4p/79gZ5q13ArzxdoB3/xtg+FAP999VxawDrPthgzrfycykVVhjlXQNgSE9ufV6opOMBRdoUyynpaZDeDNCdG3apRBiODCVOMEUQuwPbJFSfht9aTDwcdzHNkZfc4SsEdkuQmlQm8CVJWFamzaF+d2v6nnznQBul6CgQBAMSQ7cz89hB/u56cYyBlS78TrYAdYOYuJr5tZPHDwXZpmLXquUpprwffRuG/vOSr4mbbLHoCe6qUyA9Uh0gQ3hWVFXwTwiPtb4IcSpwBPxq6odguUD0KBHRVariLcrA4YvTlJXp7DkyyB33tnM9Cl5fLN4EB4PkS6sJS58vixTHgu02PxT51n0tQZSdI/FhC/evbbo83au/r21FF3z+3dGGNMXXaB+zQeWf0tg+beq78UjhPAQEdhHpJQvxr3uBn4ITItbfQMwJO7/GmBT8kdtDkdEVq9NhNJHfbxSSt54vZ3bb2tm3bowkyZ52WcfHzdcXtpZf6DQfqOn12E0XA8SyaLToj2N8ZjDx/hYvTrM2GmRa77QZW+LHC3iz1FYCtuq0jkquBqb848biX/cyM7/G154W2sLDwDLpJR3JLx+KLBcShkvoi8BjwkhbiPiJhgNfJbScZsgJZHVi3HNhEaGQdx46bnZ8m1bw3zycQdfLQkyYpiHIUPc3PrXZoJByS+uKmL27LzO8nveXEib7QR1hLgDV9r87VNm+Fn8WYCjTixJy/60SEygsEN07c8MsxTCNRM4HVgihFhIRLKvk1K+BpxMV1cBUsplQoingWVEnssXORVZACZENtEqNWrv4kTX2mwh3Ah3/K2Jx59o5Xvfy2P3yV7mf9DBunUhLr+0mDnf795VNV8Y58k3S30LSKs7bKZFE2RKnnxHms7L7nvl8/g/62lvV8jLM96nWuEZu2vFwi7RjVmjTuwjaaxFF8wHdctPSnmWxus3AzenvlfzJG3JulHS1kfLThIrgBl9h0bpo8xgeFfsimxDUST33NfCnX9r5sgj/Lz/dn8GDIj85q4eFJb4aAKjYtpBExd5okjqDcv7IgGl6+00bLSX8VPzuPz0zfzhn9UU6uSRaM1POCW8XdvROFsE3BS9+FLKmugC2OWmMFNF3Z2mC0VRJFdc2cA3K4M8P6+SsbtZq+CUTSQOy5OJPU1HMoATaF17asLkcgl+fWc1D95ex/nHbeT2+ysZM06740Kqx2B3CJ0T6blGZGvxFzP0uMiqWZTZknsUDEp+cXU9a9eFefqJSooKs8/C7ym0BFnLpeDP8JZCihT4RPcrt8Pl5qdXVDB0lJcLT9vOr/9cwf4H59u2X5eQSYV0JUvaBDc7n7mmcEwVOqRHc4lvapiNtAckTzzSwr77b2PnToXHHq7o9QKbrmr+WgSki0APxz8HUqin7BNhfCLM0ccW8Od7+3PjVbUscDjVNrFxqF042ppbCnNLFpLSLxCWLt2lw+Hi3ukW5/o6hT/+vhGAeU+2cvB+23j37Xb+8bdyHv1XJYUFvVtgMwUzYUOJnVeT6cTqdDO/SdP8/PaOflx98U5WrVIISnfn4mxXBPtF126xFdLcko0YqmG2Wpt28shDLdw/t4U5P8znzzc38eBjFUyY5KXMIGfSi8swW2ub0ma4f6101hgxn5w/wzPDnMZIhGMlAbUI4nI8w2nGzHwuuqqcn5+9lXufG0h55a4JLzWhdeJ4ImK7C18mOOiyVEDN0OM+2XSTjMXgF5LmZoXHHmqhtFRww5X1nHteAdMmewCJN8Nq4gakui/OSKTBeNKqW2RBtpoVBqTDLfKDk4rZsDbEVedu467Hq/H6ta8joweDHcR31O0xwc1SV4AZstL0CUtXtyFQ98WeRnWPPtLGzP3y2H2ql82bFM4+O5eWBRFRTlwC0q27tEgvLTJ7oy9cQqouqXDBL8oYOMTDjZfvQNHxYxgJrN0ujsTOummjFzf5Sklk3RZnehOrYql1vdXz+aaTDz5oZ84cP/vs6+Oaa4soyPlfVUkm5z8mtolLQHpUl0wnFaEVQnD9HytZ9HmAT943dhnpET8h5ZToOm7hJ3a21Fp6ACHEiUKI4ujfNwghnhNCTDP6XAxHr2C9FuBKD88UNyl5FLvaDdcbP97DypUhfnaJvU0Lc5gnJrRGQ1m3SghVphAvxDEh/G5lpNHiXvvZF9IV2368KGZH7YKMdhf8Ukr5jBBiP+Bw4C/AP4C9zXw4ZaVTcBkuvYGpe3hZtMh619Ec2Y2VCeBESzfmZhgzzktenuDrr4wf9law2q1ZLe7W7s62GR5dEHt6Hw38I1rly3RWieEZz4Qhe09SUuyiucn+X3druIOt4Q4CUhgu7XFLjt6D1yc444JS/nV3Q9r2GWu46Fi8a6pktk92oxBiLpHuCq8KIfJIwkDNfIeXQ4RNPtWXLAkyebL6adLrNBCjNmxv63E1oTWqIWAm3dXIKon5XP0pDskzPRQwjH5JQKcMiyNOLOb+uxpYvaKDUSopt4ntn9SyyhJJxsLMiLoFmc9JwBHAX6SU9UKIgcCVZj+ctSJrdNG3yDz8wtowX1Ekb7/dzjnnpKfwcjagNcFlNEEVjL5fkKaaqolYHdrqpapaeYDk+V3sfUA+y79s7yayatd4KqKbDD1RtwAyO9FAStkKPCeE6C+EGBp9eYXeZ+LJGJENJzxRwwbhI940THI89WQbUoHDj8hzfF99hVZF3ZXl0hAxv8vcSCBVC9sOrA67K/q52bk9teNXa3RqNfonRux7KdF70dF7LpNcFwkIIeYAfwUGAduAoUREdqKZzzsusonimU189lkHp52ej8eTvd8h24mVDyx0dWRMPdpkiS+BqPbQqOznZuM6+9xKiRawXaIbX47RdsHN7Po/vwP2Ad6SUu4hhJhFpG+YKVIe57hQCEthuDiFVv1NO9m4IczgGu39aGVYZRvZKl7pIpUZ+RiJlmZA8XRdpJfifnnUpmjJmsGJCWu7i89keHRBUEq5E3AJIVxSyneJdMQ1heFZ6u0hWnrs2Gm9pXOO7KBH2mBHKa9ys2xxO+cct5n772okIL0EHMqM65DuLkvGYCG6QAhRI4R4RwixTAixRAhxadx7lwghVkRfvyXu9WuFECuFEMuFEIcZHF19tBPuB0R6g91BpG2NKTLGJ9sTGD3ZL76kiKuvauTl/1RSVKS+btBEURI9zMz8G1lSHRYFwkxWVUDxpK0RYE+hJbRORUnHitAPG+1j5Pg89j6okPv/soPvn1ZGQT6487v+7lp+ays4PZFmGmuXcAi4Qkq5KCqGC4QQbwADgB8Ak6SUISFEFYAQYjyRiIHxRDrVviWEGKPT52sx0ApcTqSXWClgOjspq0XWyJrWa/gI4De4fY49Lp9/vxTgtVcDnHBSrmZBi8akFRif66B04xf2hrP1FsqrPPzunsEALPy4jVNnfsuc00u5+IZ+XdZTu97tFt540dUSXCeiDqxsUkq5BdgS/btZCLGcSBfa84BbpJSh6Hs7oh85Bngy+voaIcRKYC/gU41dzJJSxhJ7/wUghPjS7PFl1JjfuOiLM8WI9TjmWH8kysC5ZpYZT2LvqpS3o1GbICA9BHF3W+zCSZ9zQHpsKUQU46Jf9uN7hxbhzzd3fTvpwkurW8Gmot1CiOFE/KWfArsBBwghPhFCvCuE2DO62mBgfdzHNkZfS9zWhUKIJcA4IcSXcct3gGmRdT66ILN0PGmO+r6fe+e2MO/pNk48Of3WrJVJl2wnXmj1JjrTEc6XLDGhTXxYGLWqr+zvoazSTUl5ar97otDaZenGC60jIxING6Zt9Sravl1lahNRV8E84LKoResByqSU+wghZgDPACNR7z+udgSPA/8h0tX2mrjXm6SUtaYOCosim+0CasT6UCFDPC3c9MdSzjyjjtmH+Kms7N3fORXstDpTwSsU3TbfVia1kqku1v2z3Sev4s9VixKJvy5MKFTUWBdm/BR7YrOdEF0nHvxaUWYFI0ZTMGJ05/91b7+h/vmIoM4DHonWFoCItfocgJTycyFEWAhRCWwgEusaowbYlLhNKWUD0EAS4VpqmKhdoB2eZWfDtkxk6cIA55xVh88Hxx7r56ZoC5ocyWEUbmdkiRYKZyfceqJJY0xgY3/HLw11CqUVzjy4rLoX7Iq5TcSGEK4HgGVSyjviXnsBOBhACLEb4IuGYr0EnCyE8AkhRgCjgc8c+WJk+cSXVZqkXzf1tnJwHu+9287HH3Vwwin5/OeVdq67UVJUvOviVCwWVTby35nx71n1mRlZJgHptZyinOloCW2L9PaIMbFzp0zLzH+8ZW3kynAUC1MeQoiZRGb9lwghFka3dh3wIPBA1K/aDpwBIKVcJoR4GlhGJHjkIp3IAstktcgaiYupoZGOhm38roORoz3MOS6fl19oo61NUlerdBHZvoJe3KaRuyCTRzxmrFgtt1hA8Thi2Z14XgW3XbuFA44qxpe3a98d0t1lf3bH9ibrP7YVa9EF80HzIvyxxmduJuJrdZyMUovE7giKdOkuRlgN6P7HH7az8usQ770d4Pa/l1NQIGhp6btRBjm640Qp0D2+V8iIsXm88K86/X1bjGowjOF2INJDiwzP+LJEWkRWrb2M2pKI0cSa090VLr2xPwALPg/icsOr7/Zj7PisNv6zEr8I6S569FQmV4uSZ0l8z72mP0/PraVux67vZ8ZqtiuULJEgbhRcqvdpDn0snzEjocvmCIRxU/1M3dOLlJCfL6gekEFpiDk6KdTxVcauvtYUHsg7Ffurr4Wli1bZdbvxbq2Y77tmpI9Djivhob9u5/KbB6a+P0QXcbfDr+uI0GaplWoG4+iC6NPLrPXZmxBC8Ofby1i3Jkztzsz1K/Zlik2WQiwQiurSpHhosinZIlXiZ/ubFD9Nih+AH11axSdvN7NqaSDlbSdazxlZt4BICJeZJRvp3SppEr0Qo4qhBVz2S4UrLmngX/8e0C0TpwT98CK9+E0wU+za+kjAaJja03GumYCa0MYiQ3qiW0CT4ocimHNONU/e28Blt5ZR5m61dR9OlURMib5syWY6RpNjQek2XIw48rhCxkzwcu/t6evFlEmopbzGL3rt28PSWgp0pcteYYmnwaQFm9hyW5FCs/i43cw+sYIF7zVSvyOY9HWbLHq+Y6d927mJLwskG76TmPCQWJqtJ0q1CSE47dwSPn6vLS37641o1Z8odgXwi2C3JRvQKgHaKrUFONEfG49a/eWiUg/7HlnG+09v6/ZeTGydaG6a9qapmd1I0RJpcRdkc3eEGKN287F+TYj2gCTPn/3fJ12kOgSNCe3GcKnueuNcO1PavtMoKjP7rhRV4sgfVXHzuas56fxKPF7ta8+p4X9kNLILJ5IistVKNYMpkXUJRTOKIIyrV4ioEXl+wZARHlZ/3cGE3bOn55dVS8Qo1rin28NvCecbrjPInfwIxEyN3WRRE14zDB+fj7/AxbpV7Ywc7zf9uUSXQqoin4gjI8i+LrKKRb9ab2HytDzmPdLEDZN9uHpJy4S+MOm1SUOIC1N0SzjVtSAWreNVif3NyxeEQ92VKBnhTBR5u0TXDrI1csAMhiJrJuDfLWRWW7MBHR/a9vCu73/aVfn89rx1XHNZA5f/eTAer8DvqdfdtlHtAqP3jcLkjDsv9F4RLXNwUixmrSU7NLbDAk78zQtc7bhcAsVmIYoX3R4X3MzRe9vJevM0IL26E2NGWWZ6AptIQbGbGx8cxraNQd59QV9cewtGkQNmPp+JmLVi1a6p2BRXsuhdawFF3zoWbkF7yEWH9HQueiTrmlAQaU2j7UZu4it9qFluVhz4HdJtq6M+z+9i2gGFrPm63XjlHIC+0O4Mq7dKqnQ3O3U4tqEmtC5kyr5XPZrqwhQUdxW/Dtm1QI2Vgi6J7sB0V+fqzRNfps0Mq5WUUq1f4DRGFoQaB80p453n69mxOTtCjbKRneEimhQ/bhTNxeuQI6/RYjqtC6m6pHw8tSEadoaoGdX1uBKNjy6xyzYOUtNi4fZiS9aWXyIo3bqtw7O5fbia8A8c5uOo08u576YtPXBEOeLxCkV1iS+Cnc0UuNpZsbCVMbsXJD3Z6kRPvJjY2m2t9/lkhF3+zdQypnojJ17Yj68XtbHw85zbINNJ7DzQouSxLVzUudiFXtSBXhKC0Wjq49cbmX5QccrHFcOsP9eI2KjWVqHtxZas4dnOtEISTmDoMlB5FLn9MH5GEV98m8/YPbXPkVHeu1E4kNFstfEEiEGVNIPohkxsUghQYWMef6LQxvvw7W65nSwtAcEnbzbyo59Xd3ndaqJB4nXTo3ULsGalCiFqgIeBAUAYuEdKeZcQ4tfAuUAsXe46KeVr0c9cC5wNhIg0XlRvHmYDGTfxpUZYujQvgqB04zKqO2vwfqppnOGgxO3J3tA1MxiNVPSGoTGLJ1OF2gx61046BHjZZ83UjPZT0t9PME6I7BbF+MnJHhFca1ZqCLhCSrko2rF2gRDizeh7t0opb41fWQgxHjgJGE+kieJbQogxTrWgyTiR1bqpnZixtYoQqAaIx6NI0SNVnDIJrd/UrXNeesqCTCYSxem5Bq8IkV/oVr3GVIu42JhGq7Vdp1oJWblFpJRbgC3Rv5uFEMuBwbFNq3zkGOBJKWUIWCOEWAnsBXya+lFok9RVYuXCVxC6Szb6d8dPL+TLjzI/1MgpnMwCLHS14xVhzaVV8aWtEpYZ9Nxq9UqB5vtGrqr+NT62bTDXrVcvhtlKvHJaisXY5JMVQgwHprJLMC8WQiwSQtwnhIgVwhhMpF14jI3sEmXbseWsxX4AK+UErdBTVu702SUseL+RcLhvW6o9SUxs45f1wfLO4texAtiZQCpV5Mr6eQi0hGlr2WVhm3W/OCGOdk2edcMGkY26CuYR8bE2A38HRkkppxKxdP8aW1XjCBzB1Jnq7R0QUqX/YB/VQ/L44M1WZh1R2NOHk0ODeKFVc1EUiJ6LEFGb+IyfIxBCUDnQx/aNHQzdzbgYjhaJrg073DF2Cq2Wu6B5wyqaN64y/rwQHiIC+4iU8kUAKeX2uFXuBV6O/r0BGBL3Xg2wKemDNonhWUpGYK1ku7iF4thwRG/iDEwU/NC5Ho+9aBBzb13P7odUasYxWglEN0r7NbKGDGsfmKg5UeiyX4T0/LHpJj68SknodGHUqNEJAtKLC4UO6aalMUT9jhBVA1N3jaj5jp0QXUtoXA5Fg0dTNHh05/9bP9cMAngAWCalvCP2ghBiQNRfC/BD4Kvo3y8BjwkhbiPiJhgNfGbh6HXJehPV7NPUh/bNYmX2e9qsUl68ewMfvtbEAUeVpLydTEYroD+ZiZ9il30Fz52q0u8X3X2fsRA6tWvEzHHUKwWa77WaSJRY+HYdQat/9gAAIABJREFU4/cuQRYW0KJAiTuAgst2UYz/LXtCcK3M2QkhZgKnA0uEEAuJSPZ1wGlCiKlEzKQ1wPkAUsplQoingWVAELjIqcgCyDCR1fPdZmqpRSEEZ1zej3tu2srMw4txuzMvCiITaFK6DnWNwubsFGWniFVAS/xudrofPnutln2Oruz2upOWaPx9mK7wO4vRBfNBNef3NZ3P3AzcnPpezZMWkbXDd5PJoVB7HlBI4V1uPnilkVlz9Cv5ZxKZXJ5yY7Bc8734hoIlrq6dXHeGe943Hu9+iEUP+F3mY7FjgtlUG2TFZ41c8JdRhp+xS3QTr4m0CW5m3tq2YFn9Eq3PTLU49QhKt6ULSAjBUaeW8fGbTVklsmaQUrJtfTtLP2pg2ceNbFkTABl5XUo6FyQUlXs4/YYRDJtgTeiSyTJsTIgeUBOzVIoA2U3iMbRH5wH0rrtn79jAfsf2o6A4+ds0Jrox0bTDB+6o4PZ1kU0mBMuNkpVCa5Wxu+fz2J07evowbKGlIcSSDxtYOr+BpZ80EupQmLhvKbsfWMbR5xbgckUSMaRwgYg8ZISAb5c085ezl3HkOYM44uxBGdM9Iia89eFC1ZvZiYk9gMawcfiY2r2VJxTWLmthwZt13PKfKZ2vl7gD3dY1S6KFalV07Q7LzNBBqi2YiC7IrgSBZIi3LsJC58Fg8MxoVPIpGe6noXYNm2q9FJUl5IUbDN30hpJGQ3ojKy3RXwiwfnkTm1e14iv2Uz7QT9lAP7Ub21j2/g6Wf7CDTV83MWp6OWNnVnDOT0ZSPaoQIQQVCTVeE4eog8cUMG6vEu69ahVfvl/PMRfXUDU4j/JqHx6fPQ/eMhtrFsRoUfIodLWrRnKoTYbFo3Z+raLg4qm/rOcHF9WQX+pDN7wlReJHC040Rkyaviyy6cQlpGE7lniSeQAks91UEALC4cyuZbBuaROv3PkdG79poWZ8ER3tULc5QP3mNoqr8hh/QBWHnD+CUTPK8fnduBKmfGtNVKzyDizggodm8N5D63jmjo3UbWqncUc73zt5MD+6chB5+dn10A5IH37RoXqtOeGj9IowS+fXs21dgINO7g90H/qDOUtU6wGdONKMF1yn0maNEM5N7vc4GSWyhsVIeuh3CChew4mLloYwbo8gvyizRERKyYYVzfzn72tZs7iRw84byjl3TcLrc9EetYKllAhh38PB5RbM/ukwZv90GACtDUGe/cM33HDMV5x+ywQm7uHXjySJxksXJDmMT3dhk6B0q44kjK6Vdp24bEWRPPPXdRx/+VA83l1imBhtES+gYVy2WaOJApwu0e3TjRTtoDe7HGLUbg1SOSAzcumDHQqL3q3ni/82s/zDWqSEWWfUcOafx+Pzd/8t7BRYNQpKvfz4TxNZ9NpW7rt4MQeeNIDvXzTE0IWgFkeqNjwf4t1peAz1aYw6CCjebrHFah1o1Vj8bh1Swowju4dtqRETxcTJQidE11HB7b2GrHWRdao9st2EcTl6kTgYy5w0z96+gWWfNDLt6AHMOqOGAaMKHBdSM0w9opqRe5bx+FVLuOuCZVz+wKRu66SS9bc+GBEkvd+3WGfSSG/iS88nm4xwx2feaZUV9IowC9+uY7/j+lmeNEy0sGMib2VS2knBzU18qdAXIwj0KKnwsnOz+g0ZxqWb3toU0p48MRKdRAspHJLMf3EH1z48nuIRFbqf7QlK+uXR2hhi2mFVad2v3gShV4TSNvnTLeQx7vf1EOKrD+s58pxBXdaxIzEj/vpL9LWngu33f18WWS2yOVQrpYI3GtelokiWLWji9Qc2Mu3wKprC3QUzmUD0ZEmcjFr0+lZKB+TjH96PVkXfTaMYWY0aD9g8i99nn2P68/4TW9j/xGpKqsy7WOprQ/gL3Xjz7Hc/acXmhmWeYyFeiSz7qAFfvosBI8xVDkv1/kv83e0QXav0aUs2E2nXsEqMLhYniiy/dPsaFr6xnZk/rGbWaQNs335rU4hNq1qRCgyfXIRXx4+5eWUz8373NT/92xTNdexA6/ybIc8V5NAzB9PWFOKuC5Zx7dO7mxoar13SxJ3nLOG0349l6qH9ur3vpCtIrXZDk5KvmRqcSvPGPNHBvFvXcewlQ7q5dtSMAj0fr+HDU2f9HhPcnMg6j5UbN4YiXWm/SJrrghx21mAOOsW6wDbXB3nu9vXUbumguS5I7eYOmhtCDBpVgJSSLd+1MWJKMaP3KKatOczW79rYuTVIOCxRQpLm2g6Ov2EsI/Yos+GbOYMiXTSF8znowrEsfv8z/vvvBqYdPbDz/cThdKm7lVVfNDD3Z8uQQGFp8teJXqhVsVt7KG4k3HbORyx4o5ZwSLLXUeYmvILS08WSNTuxZkRMcMO4bNumGXKWrAU028k4WWU9BYLSk9JF5fa6aG60LuxtzSH++tPlDJtQyAEn9Ke43ENpPx/lg/M7Lb3WphArFzSyemETVTV5TNq/DF+/YtxeF263wFfgprR/drTAFkJw9BVjePpXy5hyaLVmpMGC+W08fuVyTrlld1743VJ8VYWqHRGKXalnQ9mNVrlPrZKXbc0hnvrjWs64cWQ3q17LWk50FSRau3ZY9vHbdFpwhdJ7VdaSyPaF0CwjJu5XzqO/+oYv39nBoWcMYvqRlUnN5G9a3UbtToVnb1vHiMlF/PjXI7p8Pj4esqDYw+4HVbD7QbsmtDKp8n+yjNm7gqqhBXz67EZmnjqky/UUDip8/twG3vjbKn58+1QqhxbQuKOd4n7qDxE9qzI2g2+lrq9Z9O4JtWN0o/Dkb1cxcWYpk/e3bwRidySA44LbezXWXNHucAY2McwUpsyu5Ob99+bz95t5/vaVfPBSLcf/ZgIlcWLgVsmiCHUovDX3Oz56aj3lg/MZMrmMw68bx45wcudab0QQlG7Lk1ROs/vh/Vn1aR0zT40UqpdSsvDfm3nz7pVU1BRwzr3TqagpYO5PPmX2uSPxF6ZuF6hZmKlUybIzlfaTl7ez7qtGfv/8xE63ht3GSxhXl4e1USSF0YSaE51SMmDuzTEyxifrNO2K19Bfq3dx66ZQumHi7ALG7lfFW//8lluP+4jvXzmWPecMVLVq6za18dD/fUlxpY+fP7cPRf3tz3+Pkaqv22y8qtXIiY0rmqmZuKvY+VdvbuWtu1dx4u8mM3JGxGJ/6OIFDN29lIPPH6G6Db3fRi8yIC9uKJ4Y4hUvJGXuFv0vYQK1cp9bv2tl3k2ruPbB3fAXqFe4UovvTjaqIDG9NuPqFkDftmQzCVNPeJ11nJ4Y8/hcHHHpaCYf0p+nrl/K589upHSAHxlWEC5BXoGbvAI3X7yyhQN/MoxZZw9DCEGGXOYpkShORqmtsVFRrK3L9jUtlA2IWP0dbWH+/acVnHTTLoHd/HUTG5c38pM79qe9JUw4qFBYnt7MusSkg/hhfyrhXW3NId6Yu475T2/i2CtHMXyiflJDoqiGpbCtfY9TmWLJ0ucnvtxI210GLqGgRDvc9jYGTyjh0qf2Zuk72wh1KHg9AiUsaW8J0d4a5ie3TWHkntpFqc2SaZOHyRBr63Lk1RN49JIvqN8RwuXzULN7BYOnDyAQ1eoPn9zAtOOHoSiSe376P4ZOLuXYG8b34JF3RS1cy6fjs/zqvZ08esMKJuxXwbUvTmfEYHuKa9sluvEPkHR1RQCiRYlTQwhRAzwMDADCwL1Syjvj3v8F8CegSkpZG33tTuBIoAU4U0q5KPWD18cxSzYmntksBFbw+FzsfkQkrMupnlTZhtooonp0MRc+sS9PXbmYNQvruOSlWZ3vffPBVpa9uZkLnzmAp369grrN7ZQNUWgNdxW2AnfEmkyHKJgJ20p0DbhRcKOwbUM7j1y7gnPvmsjo6bFJruRKN2pV1ko0VmLnwkr3i3S2obH4jAgBV0gpF0Xbgi8QQrwhpVwRFeBDgLWd+xLiSCKtwscIIfYG/gnsY+kIdEhZZON9fZmQMeI0VrsnZBNOdQ3WoqDMx6l3703jlgClAyL+6eVvb+bFXy/mqGsm8b9569j6TSNHXj2JRS+t19yO2qgoUfD0rMxd27Hf9lDCkoevXs5h59QwdnoJTtSIjSd2LsLSfLyrXrKO04JrRUKiHWm3RP9uFkIsJ9KFdgVwG3AlkQ61MY4hYvkipfxUCFEqhKiWUm5N/Si0MbyaYsO6vmqRxqMWn9mTGImhUXv2THpouD0uymsinV23rW7i6Z8vQAlL3rpzBf1HFXPqHTPYtLSeYFvXY45ZsWoUuLrXkoiJrhulSy+uyPrOpc++ds863B7BIWfVdL7mdwXTUqc28aFhNQQrdsy2HqdNBZaEEMOBqcCnQogfAOullEsSJqAHA/FP643R13pGZGPEfKjZgqavN9UIgl6IZvGfFH9nu85f1fAiLnz2QMoG5ePLj1yijdsCvHrLUub82rmU4VhpRbUSi6UWOjIseG077z+xmWue3sNUCnGyQ38tC1Trd7Qr5tXO+RQtd0H9jtU07FhtbhsRV8E84DIivtnrgUPVVlV5LbNbguvN2tshzmo/pp4QpLt4c44IQenWt55NFpxxuQX9RxV3ee3lGxdTUObDl+8m1BHG43NmwlRNYAEawgWqrxvFIX/7vzqe/O0qLrlvMuUDUsvGix/6x7ArISAmuAqiZ40MDYkrqxxFWeWubr3rvnlLdT0hhIeIwD4ipXxRCDEJGA4sFhEztgb4QgixF7ABGBL38Rpgk+XvoEGPhXBlYlRBX/K7OkGqDzczsbwHXjSO5W9t5o1bl7P92yYOvGA39jtrdEr7s7OYTLviVY28KXB10NEW5qGrV3DGzWMZOqFrtTSr8cXx1qiaQKYyGknnRFciNgRHPAAsk1LeASCl/IpItEFk+0J8B0yTUtYJIV4CLgaeEkLsA9Q75Y8Fh0TWjmIvOXLEM2hiGYMmlsFl42nY3Mq9p3zA8OmV1EzuHgqn56dNF62Kj9f+uZJhU0oZd0A/gtKacGmJZmzkkGi0JJNCrDb6SLvgWqhdIISYCZwOLBFCLCRiF18npXwtbjVJ1E0gpXxVCHGUEGIVkRCus1LeuQmSElnd2NYMtEz7MkaTXtlM6cACjrh2Mi//9ksufObAbu+3hvPwukI0qNT2BaiwIYPLiO1rWvjkqQ1c88KMztfi7xu3jFjTTgmYnSIZ765wqjayxeiC+YCuAEkpRyb8/7PU95gchiKbjVZpWLpSHrq2hjMrgsApjFIzM91tMuGQgbxw3cKU/LN6RXWSjWlWcxUE28PM+9UyDjt/KGXV3f2w8UJlJrrAyIrtdkwysUKX+kSa3ja0iM/ws1VwM6h9k91kVVptPG6h6F5Mqfp8e6olcqaRyvlL/IyTHSFcHhcl1X7qN7ZRNcK4VXkMo4eHVmZjULo7U4H1CLaHefjSxRRV+jjwRzWG62vtq8sxSZetD70uFrVJY0RN6NMRXdAbyFiR1evJlMMa6WoblMpvmIww+4u9tLd2Fz6vy95SfDExCWgkKcQEUErJE1cvwVfg5uy/jMPt6X6eU33w6Fmj8SQ74aXV1DHt5ETWPoIqfaeytVdYDvsxK8x+V5BgIIwvv+fnAmIC+NWbW9i6upWfzZuJ19tuZS6nEy3RTEzvNZPJZmZfsXvRju0lg8i5C8yhd4PkhuE57CSouOkIhJG+PNqVrpdx7P8iT/q6JbS3hHjlluWceMuUzi4PrjSOgTs6MzMj7g6r7oX4dGS1e9d2q7cXy0NSImtlCK9WF7OvkUparl51pTyN1iR9BSEEbQ0dlA5STxRoDnWd4EoUvVKPcRaXWb/ju3NXM3KvCkbOqKRUp2+YWl3ZZK1GrZGfEpcRlkp0gdZ27e6yoEaftmTT4RvtifbiidZP57E4ZH1YqYakRbuNjfzM4smgqIM9Tx7Bh3NXcMLtqRVQagjtEufE2NpkLMHmne18/sx6Ln1hv5SOQ+0e87uCthXqMevPNUPsPrVdbHM9vjIPLZG0ip0FkXsjIQszynYJdOwG3/OUUXz++LdsWLyTmt3NdXlVQy15QatUp1r6+IcPfceUowZSWu3XtWKTIaB4uxgeWg0VYyhJPMTtiKFVs8it0JtvuYwRWadEM0fmkKxAG4my1+/moEsm8PyVnzPr0glMPGoIQqMASyr+UbWaG4mvtTUG+fzZDVwyb2bS249sTyPWNWFkF5voiu3frt5tnYkG2BsmljR92V1gBzkBzZEKWqIcH0A/7vsjKB1UwDu3fsVnj65mv/PHMmLfarx+bUGXUrJpSR2r52/DX+LloDNSi2cFWLOgloHjSygZWIgiuyfvONXIMnE/dhSM6dHaBb14usay+rWFu/uT0jmrmiPHwGnVnPZIf1a8sYmPH17JS9cvYNSBg/jehZMoG1LUZYKwZWc7L/3yC+rWN9Oys50DzlZvzhhPOKiwcv52dq5toXRgPmUD88kv9bLg2fV8Pm8dR18zAVCvX6uWMZmq8Op3Jk69ZqzafEjaBbevW7JqQtoXaQ+n3yJP1T4x6lbhdWWn6eDSmHARQjD28CGMPXwIgcYOFj65ksd+9BYTjxnO986fiK/Qx5qPtvD6rz9n4pzh7H3+JJ67+L9MOnUC0F0cAbZ808gXz29g8SsbqRxayKAJpaz9opb6zQGatgcYd1A1F8/bn7KByXUbjglvfHZZvM/Vjkng+DhaI3+uEVpFum2d/Oq9GmumdkHywqJIkRHWbKpuir7Qkyuo2B/NkSnC7S/xse95E5ly/Cj+e/uXPHjcawzbu5q1n23lyJv2ZuiM/tSubaKoOp9nL/2Io27ck9LBuzrGhoMKH939JV++vIHpxw/h3Ee+R9Uw/Y6yVokXRUW6ulm7VmoyJyYupCLobpQu/mO77+8+HcKVKeT8upmPmnDriYNLKI4Kc2GlnyN+txcbFm5n9Xub+PGTh1FQHinYUjGsmLOenM2n//qGJ8//Lz/610EUVvrZurye/9y4gLJqPxc8exCFFZH1g1EN0Bo6q7kK9NCqkRA7X4luhjDCVO0EvW3HsKMjrSIFin7hq+QI50TWEXLC2XeJuTOSsaj1BFmvCWDNHv2o2aNf92PwuNj3p+MIdyg8c9F8aqZVsvy1DRzyf+OZeuwQEvpC6RKra2BWCFMhvnaCXfsx43tNRxJRn7dkXUImFYcHOQHNYX/zzbAUhA2sp1RinGdeMJ6OlhAdrUHOef5QyivUj9uM1adWRMasIGqdLzXLNHE/sX0YWbF6BKW701WW9g7UfV1k1TAjopngl02FMKJP+GV7I4mZdWZEVwjB7F/EN2hMbqLISJASBVHN52qVxH2k4gaIv+Zjgp82sbUgskKIGiItvgcQaaB4j5TyLiHEb4m0/1aIdKI9M9o+HCHEncCRRDojnCmlXGTtC2hjeuIrWUs2m+hQeWAk077DDOm3DNStolQefJlewDsVejo9WC20S+08p2qZ2hWCpUhXpyvGruaN6juy9OkQcIWUclG0Y+0CIcSbwJ+klL8CEEJcAvwauFAIcRQwSko5RgixN/BPILXcbBMk0RI8eZdButALMculyFpHr0iKmWvCm0WR5l4RVq0ZoFV1KtmHp36sq301BpLdrpmRWywW1wmxteKTjVqnW6J/NwshlgODpZQr4lYrZJeUzyFi+SKl/FQIUSqEqHaqmaKjjtNUQ7nULEtwpshKDucJdsv/l4R1hNsucbH7Aav2sMlz8AGSWDjGrmLkVq3cxMQHW7DJJyuEGA5MBT6N/v974AygHpgVXW0wsD7uYxujr2WfyCaiJZ5Okiv4kn1oWs4JP2NeiqKj5SpISXBUrmm7OzNo7cuO/cQmuxSS//62+pUV9YdVbfNaalvWmtpE1FUwD7hMStkMIKW8AbhBCHE1cAnwG1D1wTgmEkl2q9V2GWgW/7Dx0N1C5qzZHJ20Kx7dYa7bvUuEpJS8f+tiKkaUMP7gAeSXdW9wqLkdLVeBxr61hDeZaAszZQ7tFl2tzC4twkEbrXiNTVUUDKOiYFjn/6u3f6i6nhDCQ0RgH5FSvqiyyhPAv4mI7AZgSNx7NcCm5A/aHEmJbE9YopmGUVSFpo/O5nAmPXQt9+hbPoesrUwhjKA1zle/ZckOvn5zA/0nVvHBbYvZ+8Ip7HPasKRiYa0QVDzdOsPaPaEYL7pmBVftIWXGnZDnCtIesM+CsiFO9gFgmZTyjs5tCjFaSrkq+u8xQMxH+xJwMfCUEGIfoN4pfyyYENlsF9aQ4tbN/8/WMDOr2P279vRsvRGrXl/D+GNGs/d5k6hf18jr18xnw+db2eNH46lb00j9t7XsXN1Iw8YWqsaUMu2YGnabNVBze8lGn6i13g5KdzeL1a4Ov6kIrup2pBuXUFTFuGF79zq8KWMthGsmcDqwRAixkIgpcR1wjhBiLJGwrrXABZFdyVeFEEcJIVYRCeE6y+LR65I1CtoTxVlymCepWrE2WdPJxDK7XAJ3XkTQyoaWcMJDh/HRXYv44E//o2J0GdVjihm2zwBKBhaw4j/reOeuFQw5cBh5IogSb9m57HuYqLkEuk122fDw0nIrJHP+4kPJYp/74LGNlo+tEwudEaSU80E1S+U1nc/8LOUdJkmPK1dOPPsu8da0kWXoSULc1GJLS4eVsG3pzs7/3T43+/98z87/8+L8t+GgwuhZg1S3rdZtGfQn4dSsWLM4EdYVE11FKIbbU3N/hRG0Kj5WfFxn+Vg6yWV8pUa8gPbVYXkOewipiJuSIAB68bhlQ4tZ9Z/vVN/LS5gg++bN9Rx7x35JNapU89WnGv2gh12iG5vMS3ayK0bj9nbqtyZXFEeXnMiqk7NCrWHGLxpv4SVjzfVFEuNx4ykaXEzDhmbDbWxdVofb66JqTCmpV/ONoCa8MXeDE00SrVi5atvRS7RY8OImxu1fxcJXtqS8zy6EsydhJVmM02p7sZCGpMv26DiXcC6KQM2aU11P43Wrowk7/ZFWSTbTqnlrKwX9C2lTSWcNIyhwR6zWr19fz26HJleBKxli7oZwZ6qqfefUrJWrFZIWvx2XUAhLt+o2Wuo7eP/BNVz06F72iazswyJrF1rZX1bTdc3Okqe9dkAvRMsfaYaeFuhtK+qp2K2i2+uxybeWkIfFjyxn2avrOPa+Q4FIy/VkXAZmiS+UrZZ4YWc6bUxQYyMiI4FV20biMb3192+Zcng1/UfYWMg85y5IH9keMpZDHT2Bdgml22SV3fUOGtc1Ujq0RPP9FS99y9f//pYfPnQ4xQMLiVXiapfqdTGcEN8YdvtdYdfkm6JhncajZpC0hiPJG+s/2ciSN7fyf8/um9IxaWIhuiDTSauiBXqwV5giXTlrNovQ868CIF2mJ5ZC0k1hdSEt21u7vO5zhZBSooQUvrj/K2bfuC/FAws7XQd6pCq+qfTvSkV09SzWZP24sWiEph0BnrpuKSf+cSresl0PIlvIWbLG5CzQHOkmcWIpMdMtPkGidFgJmxd09R+2bG/j9as+oKM5SNGAAgbu0d/6MamIr91Wr12TXS5k5wRcp1shQZyDiodQUGHlB1v54N6V7HHcUEbuVQWol2tMmZzIRuhLQmp2kskOUpmQSsUqN5Ol5Emzte/k6CKWIBGWguJhZdR9V08wKHF5XGxfup33rn6HMUcMZ8lT37DfL/Y02FrqqAmvXRlyifMZqU5uhqULt1C6jfhaatuZe8p/KRuYz4yThzNtjnr8sGXCmTOpaje9Lq22Q3FrX2hahaxzXRA6CdkQWpRuoQbteg2xgkLFg4spqCrg8YMfp2pCFfXf1nHgDfsw/MAhTPnxRPLL/SgyffHciRlydouuIt26k41613x8V4TX/7KMSUcM4rArJiQ9aZYUOUu25+hIg0WpIHq90KYzGSQZoXZFRcHpGGCXx8XR9x9NR3MHG+ZvYMD4UsqHlwKQX+7vsm6rxtyBGV9tqqQiukYNDmOTjS4hDQVS7f2GUAEtTWEGTS/r9l44pNCW4OO2RE5k7Scd4pkjezDrnrEqxr4iHyMPH6k6aWb0IEqn+Npl6ca+U3zygxmLtCkcefBMOW44nz74DXseN4SgdON3BWlrCPLUzxew5gsb02p7cXSBI5HzHYrbcMmRI5XRQ0hxd1sU6SKouE3H8dqd7toa9nYu7WGPIwk8IenusqSKIgVBxU274umcOIyJbu36Vpa9vaVTYAGGTKtiy9K6ztqxAcXLK3/9mtIBfq5/b1b3HaSIlIqpJRtJ+WrIZKFMte2NGcx876T3rbG67nYs+pd97t5ZT9ZIaJ2caIuvaqUmtHk2nXMXCooUKOjXHTBzHTaG82nZ0caCuYtZ8Px6RsyoZMhBwzvf/3b+VobvVYXbG7neNn1Vx8p3N/GLVw6goNTG6IJebMmamPjKXDE1QyDU9StqXXh9rYBNR1QE7Pje2VZTQa2mgFtIfE52Y6W78NolupE02GhGl46fVi2zsr05yNPnvsewfQYwaPcqxhw+dNd220IsfGoVU4+LdCZY/eFWXrr+f/zwN5PsFVjI+WQzhYCKddDbJ6yyASN/qpb1aIfA2/lw1IqkMVP3NpnarDG6VqmLnCOvS9/SdqmIaPw5iCU7GE2KAbSF3Pznho8YMr0/My+ayD8OfonCijyWv7ae79+0N89dNp+q4YVMPnoIi19cxzu3L+WMu6YxfI9yU98vKfpyCFc6UBPPHL0DveG52SgEp0PCjBptqtW9dcp6Dyq7zomR4GoRE9h4yzXxYbTy01revmUhpYMKmXXVVDYt2klesZfGzS0UVPh5/Mx3mXT4QGb9bBzvzf2GxS+s44KHZtB/ZFFKx2SE1GikaAYhRA2RFt8DiHRBuEdKeZcQ4k/AD4B2YDVwlpSyMfqZa4GzidRTukxK+Ya1b6CN4+qWaQKq5a910o+bwxq6YtzZZcFY9Oz0xyZa7zFbN5VJNa3jihdcUBddU37XUH6X/ze+u4rXb1rM4b+ZwYj9ByKEYNiMKi547WiOCHW6AAAD50lEQVQe/dE7BJo6GDermgMvHMtLv1rEtlVNXPD4vlT0czAt3pq7IARcIaVcFO1Yu0AI8SbwBnCNlFIRQtwCXAtcK4SYAJwEjCfSRPEtIcQYKZ3xWVhWwI7wrovNSgX4VMmEGNdEv7Vdx6N3A5n1LfdEYkBPEP8bJHMOkmkXb+Z3jfl7O4f/Np7/sBSE0U+pNXITLHtpNZ/cvYQ5d8+mardyRNQPLaVk/j+WUliVh7/Mx2dPfMeKtzdTvVsJP3ngexQWCoJSe7+WsdZ+ZguwJfp3sxBiOTBYSvlW3GqfAMdH/54DPCmlDAFrhBArgb2AT1M+CB1MiWxI6W5JqDnRXcgeEVqzdMQFZydDplm4yRyP4ZA8lcgGsku8Q9IVuTZVQp/cDkdZqBW6iRdes9a16ugLV6c2acXRxqzYjpYgH9+9mDXvb+C4uQdTPjxSkaw97IFgB+/+4X9s+7qeE/62H/+9bRE1U8o59IoJDJpUhi/Bgk61m4IuNoVnCSGGA1PpLphnE2kLDjAY+DjuvY3R1xzBUGTVBDYTiLegM00Eewq7zoOZ7ZjO6kpYz+lW5MmeA72Y1lRn/42EM9iZtio1C2N33V7375RogYekm/pgRFCrfY2dr0tFsvrt9Xx42xcM2WcAJz9+JP7SvM73WzY18MpVH1E6pIiTHjqE0kKF4/+0q46D3rGp1cJNFWlDCFfUVTCPiI+1Oe7164GglDImsmqWoGMikrK7wGqxbTXihTNH76RD8Zh2p9g1uZSq+0atR53TfbvcyJR8xzGBBdjaUUI4GGb1a9/x1cNL8BZ6OOTGfamZUd3lM2veX8vbv/sfe50zgamnjol2g+jojDU2KrRua8yxhiVbq2yjTm4z/LgQwkNEYB+RUr4Y9/pPgKOA2XGrbwCGxP1fA2xK/qDNYfuslJbLIKS4bBflGMlOWuUmubIDM6m26YjRjb9W4mNs1fyuVob/sTAwJcH6dyVYk3p+5KbNzXzz4kq+fmEl5aPK2OfKfRg4Y0B00iyatdXQzid3L2btR5uYc8f+DJxcCUCBq2tjxLB0EZYu/K7uacN2J3VIjRCuciopp7Lz/29ZqrWJB4BlUso7Yi8IIY4ArgIOkFK2x637EvCYEOI2Im6C0cBnVo5fD6E3oSaEWAMMc2rnOXLkyHrWSimHW9lAkjrTbX9CiJnAB8ASIsN+CVwP3An4gFgv+E+klBdFP3Mt8FMilccdDeHSFdkcOXLkyGGNzJzVypEjR45eQk5kc+TIkcNBciKbI0eOHA6SE9kcOXLkcJCcyObIkSOHg+RENkeOHDkcJCeyOXLkyOEgOZHNkSNHDgf5f65G2ksJg5ebAAAAAElFTkSuQmCC ",
null
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http://www.4orienteering.com/elevation_relief/45/ | [
"Training Network: Wilderness Survival | Fitness Training",
null,
"The Sport:\n\n• The Skills:\n\n•",
null,
"# Contour Intervals\n\nBefore the elevation of any point on the map can be determined, the user must know the contour interval for the map he is using. The contour interval measurement given in the marginal information is the vertical distance between adjacent contour lines. To determine the elevation of a point on the map—\n\na. Determine the contour interval and the unit of measure used, for example, feet, meters, or yards (Figure 10-2).",
null,
"Figure 10-2. Contour interval note.\n\nb. Find the numbered index contour line nearest the point of which you are trying to determine the elevation (Figure 10-3).",
null,
"Figure 10-3. Points on contour lines.\n\nc. Determine if you are going from lower elevation to higher, or vice versa. In Figure 10-3, point (a) is between the index contour lines. The lower index contour line is numbered 500, which means any point on that line is at an elevation of 500 meters above mean sea level. The upper index contour line is numbered 600, or 600 meters. Going from the lower to the upper index contour line shows an increase in elevation.\n\nd. Determine the exact elevation of point (a), start at the index contour line numbered 500 and count the number of intermediate contour lines to point (a). Locate point (a) on the second intermediate contour line above the 500-meter index contour line. The contour interval is 20 meters (Figure 10-2), thus each one of the intermediate contour lines crossed to get to point (a) adds 20 meters to the 500-meter index contour line. The elevation of point (a) is 540 meters; the elevation has increased.\n\ne. Determine the elevation of point (b). Go to the nearest index contour line. In this case, it is the upper index contour line numbered 600. Locate point (b) on the intermediate contour line immediately below the 600-meter index contour line. Below means downhill or a lower elevation. Therefore, point (b) is located at an elevation of 580 meters. Remember, if you are increasing elevation, add the contour interval to the nearest index contour line. If you are decreasing elevation, subtract the contour interval from the nearest index contour line.\n\nf. Determine the elevation to a hilltop point (c). Add one-half the contour interval to the elevation of the last contour line. In this example, the last contour line before the hilltop is an index contour line numbered 600. Add one-half the contour interval, 10 meters, to the index contour line. The elevation of the hilltop would be 610 meters.\n\ng. There may be times when you need to determine the elevation of points to a greater accuracy. To do this, you must determine how far between the two contour lines the point lies. However, most military needs are satisfied by estimating the elevation of points between contour lines (Figure 10-4).",
null,
"Figure 10-4. Points between contour lines.\n\n(1) If the point is less than one-fourth the distance between contour lines, the elevation will be the same as the last contour line. In Figure 10-4, the elevation of point a will be 100 meters. To estimate the elevation of a point between one-fourth and three-fourths of the distance between contour lines, add one-half the contour interval to the last contour line.\n\n(2) Point b is one-half the distance between contour lines. The contour line immediately below point b is at an elevation of 160 meters. The contour interval is 20 meters; thus one-half the contour interval is 10 meters. In this case, add 10 meters to the last contour line of 160 meters. The elevation of point b would be about 170 meters.\n\n(3) A point located more than three-fourths of the distance between contour lines is considered to be at the same elevation as the next contour line. Point c is located three-fourths of the distance between contour lines. In Figure 10-4, point c would be considered to be at an elevation of 180 meters.\n\nh. To estimate the elevation to the bottom of a depression, subtract one-half the contour interval from the value of the lowest contour line before the depression. In Figure 10-5, the lowest contour line before the depression is 240 meters in elevation. Thus, the elevation at the edge of the depression is 240 meters. To determine the elevation at the bottom of the depression, subtract one-half the contour interval. The contour interval for this example is 20 meters. Subtract 10 meters from the lowest contour line immediately before the depression. The result is that the elevation at the bottom of the depression is 230 meters. The tick marks on the contour line forming a depression always point to lower elevations.",
null,
"Figure 10-5. Depression.\n\ni. In addition to the contour lines, bench marks and spot elevations are used to indicate points of known elevations on the map.\n\n(1) Bench marks, the more accurate of the two, are symbolized by a black X, such as X BM 214. The 214 indicates that the center of the X is at an elevation of 214 units of measure (feet, meters, or yards) above mean sea level. To determine the units of measure, refer to the contour interval in the marginal information.\n\n(2) Spot elevations are shown by a brown X and are usually located at road junctions and on hilltops and other prominent terrain features. If the elevation is shown in black numerals, it has been checked for accuracy; if it is in brown, it has not been checked.\n\n NOTE: New maps are being printed using a dot instead of brown Xs.",
null,
""
] | [
null,
"http://www.4orienteering.com/top_mid.jpg",
null,
"http://www.4orienteering.com/content_top.gif",
null,
"http://www.4orienteering.com/images/fig10-2.gif",
null,
"http://www.4orienteering.com/images/fig10-3.gif",
null,
"http://www.4orienteering.com/images/fig10-4.gif",
null,
"http://www.4orienteering.com/images/fig10-5.gif",
null,
"http://www.4orienteering.com/content_bottom.gif",
null
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https://www.colorhexa.com/b5b2b5 | [
"# #b5b2b5 Color Information\n\nIn a RGB color space, hex #b5b2b5 is composed of 71% red, 69.8% green and 71% blue. Whereas in a CMYK color space, it is composed of 0% cyan, 1.7% magenta, 0% yellow and 29% black. It has a hue angle of 300 degrees, a saturation of 2% and a lightness of 70.4%. #b5b2b5 color hex could be obtained by blending #ffffff with #6b656b. Closest websafe color is: #cc99cc.\n\n• R 71\n• G 70\n• B 71\nRGB color chart\n• C 0\n• M 2\n• Y 0\n• K 29\nCMYK color chart\n\n#b5b2b5 color description : Grayish magenta.\n\n# #b5b2b5 Color Conversion\n\nThe hexadecimal color #b5b2b5 has RGB values of R:181, G:178, B:181 and CMYK values of C:0, M:0.02, Y:0, K:0.29. Its decimal value is 11907765.\n\nHex triplet RGB Decimal b5b2b5 `#b5b2b5` 181, 178, 181 `rgb(181,178,181)` 71, 69.8, 71 `rgb(71%,69.8%,71%)` 0, 2, 0, 29 300°, 2, 70.4 `hsl(300,2%,70.4%)` 300°, 1.7, 71 cc99cc `#cc99cc`\nCIE-LAB 72.892, 1.616, -1.158 43.315, 45.001, 50.118 0.313, 0.325, 45.001 72.892, 1.988, 324.37 72.892, 1.53, -1.993 67.083, -2.137, 2.662 10110101, 10110010, 10110101\n\n# Color Schemes with #b5b2b5\n\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b2b5b2\n``#b2b5b2` `rgb(178,181,178)``\nComplementary Color\n• #b4b2b5\n``#b4b2b5` `rgb(180,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b4\n``#b5b2b4` `rgb(181,178,180)``\nAnalogous Color\n• #b2b5b4\n``#b2b5b4` `rgb(178,181,180)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b4b5b2\n``#b4b5b2` `rgb(180,181,178)``\nSplit Complementary Color\n• #b2b5b5\n``#b2b5b5` `rgb(178,181,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b5b2\n``#b5b5b2` `rgb(181,181,178)``\nTriadic Color\n• #b2b2b5\n``#b2b2b5` `rgb(178,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b5b2\n``#b5b5b2` `rgb(181,181,178)``\n• #b2b5b2\n``#b2b5b2` `rgb(178,181,178)``\nTetradic Color\n• #908b90\n``#908b90` `rgb(144,139,144)``\n• #9c989c\n``#9c989c` `rgb(156,152,156)``\n• #a9a5a9\n``#a9a5a9` `rgb(169,165,169)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #c1bfc1\n``#c1bfc1` `rgb(193,191,193)``\n• #ceccce\n``#ceccce` `rgb(206,204,206)``\n• #dad9da\n``#dad9da` `rgb(218,217,218)``\nMonochromatic Color\n\n# Alternatives to #b5b2b5\n\nBelow, you can see some colors close to #b5b2b5. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #b4b2b5\n``#b4b2b5` `rgb(180,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #b5b2b4\n``#b5b2b4` `rgb(181,178,180)``\nSimilar Colors\n\n# #b5b2b5 Preview\n\nText with hexadecimal color #b5b2b5\n\nThis text has a font color of #b5b2b5.\n\n``<span style=\"color:#b5b2b5;\">Text here</span>``\n#b5b2b5 background color\n\nThis paragraph has a background color of #b5b2b5.\n\n``<p style=\"background-color:#b5b2b5;\">Content here</p>``\n#b5b2b5 border color\n\nThis element has a border color of #b5b2b5.\n\n``<div style=\"border:1px solid #b5b2b5;\">Content here</div>``\nCSS codes\n``.text {color:#b5b2b5;}``\n``.background {background-color:#b5b2b5;}``\n``.border {border:1px solid #b5b2b5;}``\n\n# Shades and Tints of #b5b2b5\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #030303 is the darkest color, while #f8f8f8 is the lightest one.\n\n• #030303\n``#030303` `rgb(3,3,3)``\n• #0d0d0d\n``#0d0d0d` `rgb(13,13,13)``\n• #171617\n``#171617` `rgb(23,22,23)``\n• #212021\n``#212021` `rgb(33,32,33)``\n• #2b292b\n``#2b292b` `rgb(43,41,43)``\n• #353335\n``#353335` `rgb(53,51,53)``\n• #3f3d3f\n``#3f3d3f` `rgb(63,61,63)``\n• #494649\n``#494649` `rgb(73,70,73)``\n• #535053\n``#535053` `rgb(83,80,83)``\n• #5d595d\n``#5d595d` `rgb(93,89,93)``\n• #676367\n``#676367` `rgb(103,99,103)``\n• #716d71\n``#716d71` `rgb(113,109,113)``\n• #7b767b\n``#7b767b` `rgb(123,118,123)``\nShade Color Variation\n• #858085\n``#858085` `rgb(133,128,133)``\n• #8f8a8f\n``#8f8a8f` `rgb(143,138,143)``\n• #989498\n``#989498` `rgb(152,148,152)``\n• #a29ea2\n``#a29ea2` `rgb(162,158,162)``\n• #aba8ab\n``#aba8ab` `rgb(171,168,171)``\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #bfbcbf\n``#bfbcbf` `rgb(191,188,191)``\n• #c8c6c8\n``#c8c6c8` `rgb(200,198,200)``\n• #d2d0d2\n``#d2d0d2` `rgb(210,208,210)``\n• #dbdadb\n``#dbdadb` `rgb(219,218,219)``\n• #e5e4e5\n``#e5e4e5` `rgb(229,228,229)``\n• #efeeef\n``#efeeef` `rgb(239,238,239)``\n• #f8f8f8\n``#f8f8f8` `rgb(248,248,248)``\nTint Color Variation\n\n# Tones of #b5b2b5\n\nA tone is produced by adding gray to any pure hue. In this case, #b5b2b5 is the less saturated color, while #fb6cfb is the most saturated one.\n\n• #b5b2b5\n``#b5b2b5` `rgb(181,178,181)``\n• #bbacbb\n``#bbacbb` `rgb(187,172,187)``\n• #c1a6c1\n``#c1a6c1` `rgb(193,166,193)``\n• #c6a1c6\n``#c6a1c6` `rgb(198,161,198)``\n• #cc9bcc\n``#cc9bcc` `rgb(204,155,204)``\n• #d295d2\n``#d295d2` `rgb(210,149,210)``\n• #d88fd8\n``#d88fd8` `rgb(216,143,216)``\n• #de89de\n``#de89de` `rgb(222,137,222)``\n• #e384e3\n``#e384e3` `rgb(227,132,227)``\n• #e97ee9\n``#e97ee9` `rgb(233,126,233)``\n• #ef78ef\n``#ef78ef` `rgb(239,120,239)``\n• #f572f5\n``#f572f5` `rgb(245,114,245)``\n• #fb6cfb\n``#fb6cfb` `rgb(251,108,251)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #b5b2b5 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population"
] | [
null
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https://vixatunes.com/music/b-e-y-o-n-c-e-s-w-e-e-t-d-r-e-a-m-s-s-t-o-r-m-u-l-t-r-a-p-r-i-v-a-t-e-c-l-u-b-r-e-w-o-r-k-e-d-mix | [
"",
null,
"Download B E Y O N C E S W E E T D R E A M S S T O R M U L T R A P R I V A T E C L U B R E W O R K E D Mix Mp3\nB E Y O N C E S W E E T D R E A M S S T O R M U L T R A P R I V A T E C L U B R E W O R K E D Mix Mp3 Download free, Download Mp3 B E Y O N C E S W E E T D R E A M S S T O R M U L T R A P R I V A T E C L U B R E W O R K E D Mix Song, Download B E Y O N C E S W E E T D R E A M S S T O R M U L T R A P R I V A T E C L U B R E W O R K E D Mix Mp3",
null,
""
] | [
null,
"https://vixatunes.com/includes/themes/vixa/assets/images/shadow.png",
null,
"https://vixatunes.com/ad.gif",
null
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http://www.lmfdb.org/EllipticCurve/Q/53312/k/1 | [
"Show commands for: Magma / Pari/GP / SageMath\n\n## Minimal Weierstrass equation\n\nsage: E = EllipticCurve([0, 1, 0, -354433, 56005599]) # or\n\nsage: E = EllipticCurve(\"53312ba4\")\n\ngp: E = ellinit([0, 1, 0, -354433, 56005599]) \\\\ or\n\ngp: E = ellinit(\"53312ba4\")\n\nmagma: E := EllipticCurve([0, 1, 0, -354433, 56005599]); // or\n\nmagma: E := EllipticCurve(\"53312ba4\");\n\n$$y^2 = x^{3} + x^{2} - 354433 x + 56005599$$\n\n## Mordell-Weil group structure\n\n$$\\Z\\times \\Z/{2}\\Z$$\n\n### Infinite order Mordell-Weil generator and height\n\nsage: E.gens()\n\nmagma: Generators(E);\n\n $$P$$ = $$\\left(-85, -9248\\right)$$ $$\\hat{h}(P)$$ ≈ $0.4849310505061373$\n\n## Torsion generators\n\nsage: E.torsion_subgroup().gens()\n\ngp: elltors(E)\n\nmagma: TorsionSubgroup(E);\n\n$$\\left(-663, 0\\right)$$\n\n## Integral points\n\nsage: E.integral_points()\n\nmagma: IntegralPoints(E);\n\n$$\\left(-663, 0\\right)$$, $$(-213,\\pm 11040)$$, $$(-85,\\pm 9248)$$, $$(170,\\pm 833)$$, $$(493,\\pm 1156)$$, $$(1003,\\pm 26656)$$\n\n## Invariants\n\n sage: E.conductor().factor() gp: ellglobalred(E) magma: Conductor(E); Conductor: $$53312$$ = $$2^{6} \\cdot 7^{2} \\cdot 17$$ sage: E.discriminant().factor() gp: E.disc magma: Discriminant(E); Discriminant: $$1488852539293564928$$ = $$2^{19} \\cdot 7^{6} \\cdot 17^{6}$$ sage: E.j_invariant().factor() gp: E.j magma: jInvariant(E); j-invariant: $$\\frac{159661140625}{48275138}$$ = $$2^{-1} \\cdot 5^{6} \\cdot 7^{3} \\cdot 17^{-6} \\cdot 31^{3}$$ Endomorphism ring: $$\\Z$$ Geometric endomorphism ring: $$\\Z$$ (no potential complex multiplication) Sato-Tate group: $\\mathrm{SU}(2)$\n\n## BSD invariants\n\n sage: E.rank() magma: Rank(E); Rank: $$1$$ sage: E.regulator() magma: Regulator(E); Regulator: $$0.484931050506$$ sage: E.period_lattice().omega() gp: E.omega magma: RealPeriod(E); Real period: $$0.249110870501$$ sage: E.tamagawa_numbers() gp: gr=ellglobalred(E); [[gr[i,1],gr[i]] | i<-[1..#gr[,1]]] magma: TamagawaNumbers(E); Tamagawa product: $$96$$ = $$2^{2}\\cdot2^{2}\\cdot( 2 \\cdot 3 )$$ sage: E.torsion_order() gp: elltors(E) magma: Order(TorsionSubgroup(E)); Torsion order: $$2$$ sage: E.sha().an_numerical() magma: MordellWeilShaInformation(E); Analytic order of Ш: $$1$$ (exact)\n\n## Modular invariants\n\nModular form 53312.2.a.k\n\nsage: E.q_eigenform(20)\n\ngp: xy = elltaniyama(E);\n\ngp: x*deriv(xy)/(2*xy+E.a1*xy+E.a3)\n\nmagma: ModularForm(E);\n\n$$q - 2q^{3} + q^{9} - 6q^{11} + 2q^{13} + q^{17} - 4q^{19} + O(q^{20})$$\n\n sage: E.modular_degree() magma: ModularDegree(E); Modular degree: 663552 $$\\Gamma_0(N)$$-optimal: no Manin constant: 1\n\n#### Special L-value\n\nsage: r = E.rank();\n\nsage: E.lseries().dokchitser().derivative(1,r)/r.factorial()\n\ngp: ar = ellanalyticrank(E);\n\ngp: ar/factorial(ar)\n\nmagma: Lr1 where r,Lr1 := AnalyticRank(E: Precision:=12);\n\n$$L'(E,1)$$ ≈ $$2.89923830699$$\n\n## Local data\n\nThis elliptic curve is not semistable.\n\nsage: E.local_data()\n\ngp: ellglobalred(E)\n\nmagma: [LocalInformation(E,p) : p in BadPrimes(E)];\n\nprime Tamagawa number Kodaira symbol Reduction type Root number ord($$N$$) ord($$\\Delta$$) ord$$(j)_{-}$$\n$$2$$ $$4$$ $$I_9^{*}$$ Additive 1 6 19 1\n$$7$$ $$4$$ $$I_0^{*}$$ Additive -1 2 6 0\n$$17$$ $$6$$ $$I_{6}$$ Split multiplicative -1 1 6 6\n\n## Galois representations\n\nThe image of the 2-adic representation attached to this elliptic curve is the subgroup of $\\GL(2,\\Z_2)$ with Rouse label X17.\n\nThis subgroup is the pull-back of the subgroup of $\\GL(2,\\Z_2/2^3\\Z_2)$ generated by $\\left(\\begin{array}{rr} 1 & 0 \\\\ 2 & 1 \\end{array}\\right),\\left(\\begin{array}{rr} 1 & 0 \\\\ 0 & 7 \\end{array}\\right),\\left(\\begin{array}{rr} 1 & 1 \\\\ 0 & 5 \\end{array}\\right)$ and has index 6.\n\nsage: rho = E.galois_representation();\n\nsage: [rho.image_type(p) for p in rho.non_surjective()]\n\nmagma: [GaloisRepresentation(E,p): p in PrimesUpTo(20)];\n\nThe mod $$p$$ Galois representation has maximal image $$\\GL(2,\\F_p)$$ for all primes $$p$$ except those listed.\n\nprime Image of Galois representation\n$$2$$ B\n$$3$$ B\n\n## $p$-adic data\n\n### $p$-adic regulators\n\nsage: [E.padic_regulator(p) for p in primes(3,20) if E.conductor().valuation(p)<2]\n\n$$p$$-adic regulators are not yet computed for curves that are not $$\\Gamma_0$$-optimal.\n\n## Iwasawa invariants\n\n $p$ Reduction type $\\lambda$-invariant(s) $\\mu$-invariant(s) 2 3 5 7 11 13 17 19 23 29 31 37 41 43 47 add ordinary ss add ordinary ordinary split ordinary ss ss ordinary ordinary ordinary ordinary ss - 7 1,1 - 1 1 2 1 1,1 1,1 1 1 1 1 1,1 - 0 0,0 - 0 0 0 0 0,0 0,0 0 0 0 0 0,0\n\nAn entry - indicates that the invariants are not computed because the reduction is additive.\n\n## Isogenies\n\nThis curve has non-trivial cyclic isogenies of degree $$d$$ for $$d=$$ 2, 3 and 6.\nIts isogeny class 53312.k consists of 4 curves linked by isogenies of degrees dividing 6.\n\n## Growth of torsion in number fields\n\nThe number fields $K$ of degree up to 7 such that $E(K)_{\\rm tors}$ is strictly larger than $E(\\Q)_{\\rm tors}$ $\\cong \\Z/{2}\\Z$ are as follows:\n\n$[K:\\Q]$ $K$ $E(K)_{\\rm tors}$ Base change curve\n$2$ $$\\Q(\\sqrt{2})$$ $$\\Z/2\\Z \\times \\Z/2\\Z$$ Not in database\n$2$ $$\\Q(\\sqrt{42})$$ $$\\Z/6\\Z$$ Not in database\n$4$ $$\\Q(\\sqrt{2}, \\sqrt{21})$$ $$\\Z/2\\Z \\times \\Z/6\\Z$$ Not in database\n$4$ 4.0.453152.3 $$\\Z/4\\Z$$ Not in database\n$6$ 6.0.512096256.14 $$\\Z/6\\Z$$ Not in database\n\nWe only show fields where the torsion growth is primitive. For each field $K$ we either show its label, or a defining polynomial when $K$ is not in the database."
] | [
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https://www.classace.io/learn/math/3rdgrade/estimating-differences | [
"Estimating Differences",
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"Start Practice",
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"## How to Estimate Differences\n\nIn the last lesson, you learned how to use rounding to estimate sums.\n\nDo you know that you can also use rounding to estimate differences?",
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"",
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"You can estimate a difference by first rounding the minuend and subtrahend.\n\nThen subtract the rounded numbers to get a difference that is close to the exact difference.\n\n### Rounding Rules\n\nLet's review.",
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"If the digit one place to the right of the target digit is less than 5, you round down. 👇\n\nOtherwise, you round up.\n\n### Estimating a Difference, Example 1\n\nEstimate 923 - 486.\n\nTo estimate the difference, we first round each number.\n\nTip: Unless otherwise stated, always round each number to its highest place value.\n\nWhat's 923 rounded to the nearest hundred?\n\nThat's right, 900.\n\nWhat's 486 rounded to the nearest hundred?\n\n500.\n\nLet's subtract those rounded values.",
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"",
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"So, the difference between 923 and 486 is about 400. ✅\n\n### Example 2\n\nEstimate 726 - 48.\n\nWhat's 726 rounded to the nearest hundred?\n\n700.\n\nWhat's 48 rounded to the nearest ten?\n\nYes, 50.\n\nLet's subtract the rounded values to get an estimate.",
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"",
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"So, 726 - 48 is about 650.\n\nYou can also use the approximate symbol, ≈:\n\n726 - 48 ≈ 650\n\nGreat job learning. Now, complete the practice. You'll understand more and remember for longer.",
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"AI teaching assistants\nTrusted by over 100,000 students, parents and teachers.\n\"Class Ace is the favorite part of my students' day.\" Paola, Teacher\nStart Free Trial",
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https://www.colorhexa.com/0f5374 | [
"# #0f5374 Color Information\n\nIn a RGB color space, hex #0f5374 is composed of 5.9% red, 32.5% green and 45.5% blue. Whereas in a CMYK color space, it is composed of 87.1% cyan, 28.4% magenta, 0% yellow and 54.5% black. It has a hue angle of 199.6 degrees, a saturation of 77.1% and a lightness of 25.7%. #0f5374 color hex could be obtained by blending #1ea6e8 with #000000. Closest websafe color is: #006666.\n\n• R 6\n• G 33\n• B 45\nRGB color chart\n• C 87\n• M 28\n• Y 0\n• K 55\nCMYK color chart\n\n#0f5374 color description : Dark blue.\n\n# #0f5374 Color Conversion\n\nThe hexadecimal color #0f5374 has RGB values of R:15, G:83, B:116 and CMYK values of C:0.87, M:0.28, Y:0, K:0.55. Its decimal value is 1004404.\n\nHex triplet RGB Decimal 0f5374 `#0f5374` 15, 83, 116 `rgb(15,83,116)` 5.9, 32.5, 45.5 `rgb(5.9%,32.5%,45.5%)` 87, 28, 0, 55 199.6°, 77.1, 25.7 `hsl(199.6,77.1%,25.7%)` 199.6°, 87.1, 45.5 006666 `#006666`\nCIE-LAB 33.024, -7.453, -24.504 6.442, 7.548, 17.64 0.204, 0.239, 7.548 33.024, 25.612, 253.082 33.024, -20.838, -32.071 27.474, -6.228, -18.834 00001111, 01010011, 01110100\n\n# Color Schemes with #0f5374\n\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #74300f\n``#74300f` `rgb(116,48,15)``\nComplementary Color\n• #0f7463\n``#0f7463` `rgb(15,116,99)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #0f2174\n``#0f2174` `rgb(15,33,116)``\nAnalogous Color\n• #74630f\n``#74630f` `rgb(116,99,15)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #740f21\n``#740f21` `rgb(116,15,33)``\nSplit Complementary Color\n• #53740f\n``#53740f` `rgb(83,116,15)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #740f53\n``#740f53` `rgb(116,15,83)``\nTriadic Color\n• #0f7430\n``#0f7430` `rgb(15,116,48)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #740f53\n``#740f53` `rgb(116,15,83)``\n• #74300f\n``#74300f` `rgb(116,48,15)``\nTetradic Color\n• #062330\n``#062330` `rgb(6,35,48)``\n• #093347\n``#093347` `rgb(9,51,71)``\n• #0c435d\n``#0c435d` `rgb(12,67,93)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #12638b\n``#12638b` `rgb(18,99,139)``\n• #1573a1\n``#1573a1` `rgb(21,115,161)``\n• #1883b8\n``#1883b8` `rgb(24,131,184)``\nMonochromatic Color\n\n# Alternatives to #0f5374\n\nBelow, you can see some colors close to #0f5374. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #0f6c74\n``#0f6c74` `rgb(15,108,116)``\n• #0f6474\n``#0f6474` `rgb(15,100,116)``\n• #0f5b74\n``#0f5b74` `rgb(15,91,116)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #0f4b74\n``#0f4b74` `rgb(15,75,116)``\n• #0f4274\n``#0f4274` `rgb(15,66,116)``\n• #0f3a74\n``#0f3a74` `rgb(15,58,116)``\nSimilar Colors\n\n# #0f5374 Preview\n\nText with hexadecimal color #0f5374\n\nThis text has a font color of #0f5374.\n\n``<span style=\"color:#0f5374;\">Text here</span>``\n#0f5374 background color\n\nThis paragraph has a background color of #0f5374.\n\n``<p style=\"background-color:#0f5374;\">Content here</p>``\n#0f5374 border color\n\nThis element has a border color of #0f5374.\n\n``<div style=\"border:1px solid #0f5374;\">Content here</div>``\nCSS codes\n``.text {color:#0f5374;}``\n``.background {background-color:#0f5374;}``\n``.border {border:1px solid #0f5374;}``\n\n# Shades and Tints of #0f5374\n\nA shade is achieved by adding black to any pure hue, while a tint is created by mixing white to any pure color. In this example, #02080c is the darkest color, while #f9fdfe is the lightest one.\n\n• #02080c\n``#02080c` `rgb(2,8,12)``\n• #04151d\n``#04151d` `rgb(4,21,29)``\n• #06212f\n``#06212f` `rgb(6,33,47)``\n• #082e40\n``#082e40` `rgb(8,46,64)``\n• #0b3a51\n``#0b3a51` `rgb(11,58,81)``\n• #0d4763\n``#0d4763` `rgb(13,71,99)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #115f85\n``#115f85` `rgb(17,95,133)``\n• #136c97\n``#136c97` `rgb(19,108,151)``\n• #1678a8\n``#1678a8` `rgb(22,120,168)``\n• #1885b9\n``#1885b9` `rgb(24,133,185)``\n• #1a91cb\n``#1a91cb` `rgb(26,145,203)``\n• #1c9edc\n``#1c9edc` `rgb(28,158,220)``\nShade Color Variation\n• #29a6e3\n``#29a6e3` `rgb(41,166,227)``\n• #3aaee6\n``#3aaee6` `rgb(58,174,230)``\n• #4cb5e8\n``#4cb5e8` `rgb(76,181,232)``\n• #5dbcea\n``#5dbcea` `rgb(93,188,234)``\n• #6ec3ec\n``#6ec3ec` `rgb(110,195,236)``\n• #80caef\n``#80caef` `rgb(128,202,239)``\n• #91d2f1\n``#91d2f1` `rgb(145,210,241)``\n• #a3d9f3\n``#a3d9f3` `rgb(163,217,243)``\n• #b4e0f5\n``#b4e0f5` `rgb(180,224,245)``\n• #c5e7f8\n``#c5e7f8` `rgb(197,231,248)``\n• #d7eefa\n``#d7eefa` `rgb(215,238,250)``\n• #e8f6fc\n``#e8f6fc` `rgb(232,246,252)``\n• #f9fdfe\n``#f9fdfe` `rgb(249,253,254)``\nTint Color Variation\n\n# Tones of #0f5374\n\nA tone is produced by adding gray to any pure hue. In this case, #414242 is the less saturated color, while #05567e is the most saturated one.\n\n• #414242\n``#414242` `rgb(65,66,66)``\n• #3c4347\n``#3c4347` `rgb(60,67,71)``\n• #37454c\n``#37454c` `rgb(55,69,76)``\n• #324751\n``#324751` `rgb(50,71,81)``\n• #2d4956\n``#2d4956` `rgb(45,73,86)``\n• #284a5b\n``#284a5b` `rgb(40,74,91)``\n• #234c60\n``#234c60` `rgb(35,76,96)``\n• #1e4e65\n``#1e4e65` `rgb(30,78,101)``\n• #19506a\n``#19506a` `rgb(25,80,106)``\n• #14516f\n``#14516f` `rgb(20,81,111)``\n• #0f5374\n``#0f5374` `rgb(15,83,116)``\n• #0a5579\n``#0a5579` `rgb(10,85,121)``\n• #05567e\n``#05567e` `rgb(5,86,126)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #0f5374 is perceived by people affected by a color vision deficiency. This can be useful if you need to ensure your color combinations are accessible to color-blind users.\n\nMonochromacy\n• Achromatopsia 0.005% of the population\n• Atypical Achromatopsia 0.001% of the population\nDichromacy\n• Protanopia 1% of men\n• Deuteranopia 1% of men\n• Tritanopia 0.001% of the population\nTrichromacy\n• Protanomaly 1% of men, 0.01% of women\n• Deuteranomaly 6% of men, 0.4% of women\n• Tritanomaly 0.01% of the population"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5256237,"math_prob":0.7041097,"size":3680,"snap":"2021-21-2021-25","text_gpt3_token_len":1684,"char_repetition_ratio":0.12595212,"word_repetition_ratio":0.011111111,"special_character_ratio":0.5679348,"punctuation_ratio":0.23809524,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9875235,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-06-20T14:04:56Z\",\"WARC-Record-ID\":\"<urn:uuid:10e84556-5065-4158-a1b8-825039cde302>\",\"Content-Length\":\"36255\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:50e4b0ff-fa75-438f-8b9f-c2b51f75197d>\",\"WARC-Concurrent-To\":\"<urn:uuid:9b431150-7aad-4d37-bd63-521991e0d44c>\",\"WARC-IP-Address\":\"178.32.117.56\",\"WARC-Target-URI\":\"https://www.colorhexa.com/0f5374\",\"WARC-Payload-Digest\":\"sha1:42DXONODCOIU3IZIZZH4HFONCISQ7N24\",\"WARC-Block-Digest\":\"sha1:4VVMLLD7E7IEGYWIQGU3Q7TAC5YT4TAA\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-25/CC-MAIN-2021-25_segments_1623487662882.61_warc_CC-MAIN-20210620114611-20210620144611-00075.warc.gz\"}"} |
https://www.analyzemath.com/convert/convert_velocity.html | [
"",
null,
"# Convert Units of Velocity\n\nQuestions, with answers, on how to convert from one unit of velocity (speed) to another. For the lengths, both metric and imperial units are used.\n\nBoth time and length conversions are needed in order to convert velocity or speed units. The time conversion is shown below and the length conversion is in a table in this site.\n\nTime Conversion.\n1 hour = 60 minutes\n1 minute = 60 seconds\n1 hour = 3600 seconds\n1 minute = 1/60 hours\n1 second = 1/3600 hours\n1 second = 1/60 minutes\n1 millisecond (ms) = 1/1000 seconds = 10-3 seconds\n1 microsecond = 1/1000000 seconds = 10-6 seconds\n1 nanosecond = 1/1000000000 seconds = 10-9 seconds\n\n### Question 1\n\nConvert 1 km / hr into inches / second.\nSolution:\nWe first use the\ntable of conversion of lengths to convert 1 km into inches\n1 km = 39370.07 inches.\nWe next convert hours into seconds: 1 hour = 3600 seconds and we write\n1 km/hr = 39370.07 inches / 3600 sec\n= 10.9361 inches / sec\n\n### Question 2\n\nConvert 12.34 miles / hour into centimeters / minute.\nSolution:\nThe\ntable of conversion of lengths gives 1 mile = 160934.4 cm. Also 1 hour = 60 minutes. Hence\n12.34 miles / hour = 12.34 �� (160934.4 cm) / (60 mn)\n= 3.30988 �� 10\n4 cm / mn\n\n### Question 3\n\nIf someone is driving at 60 miles / hour, what is it in meters / second?\nSolution:\nThe\ntable of conversion of lengthsgives 1 mile = 1609.344 meters. Also 1 hour = 3600 seconds. Hence\n60 miles / hour = 60 �� 1609.344 m / 3600 sec\n= 26.8223 m / sec\n\n### Question 4\n\nThe speed of light is approximately 3 �� 108 m / sec. What is the speed of light in km / hour?\nSolution:\n1 m = 0.001 km and 1 second = 1 / 3600 hour. Hence\n3 �� 10\n8 m / sec = 0.001 �� 3 �� 108 / (1 / 3600)\n= 1.08 �� 10\n9 km/hour\n\n### Question 5\n\nConvert 235 feet / seconds into meters / minute.\nSolution:\n1 foot = 0.3048 m and 1 second = (1/60) minutes. Hence\n235 feet / seconds = 235 �� 0.3048 / (1/60)\n= 4297.68 meters / minute\nMore math problems with detailed solutions in this site."
] | [
null,
"https://ezoic-top-images.s3.amazonaws.com/vmw7e1f3lelt6ssmutokvcxe1kxxha.jpg",
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https://percentage-calculator.net/x-is-y-percent-of-what-number/120-is-20-percent-of-what-number.php | [
"# 120 is 20 percent of what number?\n\nAnswer: 120 is 20 percent of 600\n\n## Fastest method for calculating 120 is 20 percent of what number\n\nAssume the unknown value is 'Y'\n\n120 = 20% x Y\n\n120 = 20 / 100 x Y\n\nMultiplying both sides by 100 and dividing both sides of the equation by 20 we will arrive at:\n\nY = 3 x 100 / 20\n\nY = 600%\n\nAnswer: 120 is 20 percent of 600\n\nIf you want to use a calculator, simply enter 120x100÷20 and you will get your answer which is 600\n\nYou may also be interested in:\n\nHere is a calculator to solve percentage calculations such as 120 is 20 percent of what number. You can solve this type of calculation with your own values by entering them into the calculator's fields, and click 'Calculate' to get the result and explanation.\n\nis\npercent of?\n\n## Have time and want to learn the details?\n\nLet's solve the equation for Y by first rewriting it as: 100% / Y = 20% / 120\n\nDrop the percentage marks to simplify your calculations: 100 / Y = 20 / 120\n\nMultiply both sides by Y to move Y on the right side of the equation: 100 = ( 20 / 120 ) Y\n\nSimplifying the right side, we get: 100 = 20 Y\n\nDividing both sides of the equation by 20, we will arrive at: 600 = Y\n\nThis leaves us with our final answer: 120 is 20 percent of 600"
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9254271,"math_prob":0.9983977,"size":1062,"snap":"2020-24-2020-29","text_gpt3_token_len":303,"char_repetition_ratio":0.13327032,"word_repetition_ratio":0.059907835,"special_character_ratio":0.34274954,"punctuation_ratio":0.072072074,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9997662,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-04T20:59:04Z\",\"WARC-Record-ID\":\"<urn:uuid:c98679ad-b77f-41ad-91ed-fdb88eed85f1>\",\"Content-Length\":\"58933\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:7e144805-da6f-4732-9103-21af4e7aa186>\",\"WARC-Concurrent-To\":\"<urn:uuid:c7217d8e-404a-4f7f-a06a-324d0e1c9665>\",\"WARC-IP-Address\":\"68.66.224.6\",\"WARC-Target-URI\":\"https://percentage-calculator.net/x-is-y-percent-of-what-number/120-is-20-percent-of-what-number.php\",\"WARC-Payload-Digest\":\"sha1:ZIX4GYQ53GBZ7O4XGET3DMTUOE2HC5WH\",\"WARC-Block-Digest\":\"sha1:JBJOCYLLSWYCHKH7LTR57MG5LZPAGC35\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590347458095.68_warc_CC-MAIN-20200604192256-20200604222256-00108.warc.gz\"}"} |
https://matplotlib.org/_modules/dateutil/rrule.html | [
"# Source code for dateutil.rrule\n\n# -*- coding: utf-8 -*-\n\"\"\"\nThe rrule module offers a small, complete, and very fast, implementation of\nthe recurrence rules documented in the\niCalendar RFC <https://tools.ietf.org/html/rfc5545>_,\nincluding support for caching of results.\n\"\"\"\nimport itertools\nimport datetime\nimport calendar\nimport re\nimport sys\n\ntry:\nfrom math import gcd\nexcept ImportError:\nfrom fractions import gcd\n\nimport heapq\n\nfrom ._common import weekday as weekdaybase\n\n# For warning about deprecation of until and count\nfrom warnings import warn\n\n__all__ = [\"rrule\", \"rruleset\", \"rrulestr\",\n\"YEARLY\", \"MONTHLY\", \"WEEKLY\", \"DAILY\",\n\"HOURLY\", \"MINUTELY\", \"SECONDLY\",\n\"MO\", \"TU\", \"WE\", \"TH\", \"FR\", \"SA\", \"SU\"]\n\n# Every mask is 7 days longer to handle cross-year weekly periods.\n*31+*31+*30+*31+*30+*31+*7)\nM29, M30, M31 = list(range(1, 30)), list(range(1, 31)), list(range(1, 32))\nM29, M30, M31 = list(range(-29, 0)), list(range(-30, 0)), list(range(-31, 0))\nM366RANGE = (0, 31, 60, 91, 121, 152, 182, 213, 244, 274, 305, 335, 366)\nM365RANGE = (0, 31, 59, 90, 120, 151, 181, 212, 243, 273, 304, 334, 365)\nWDAYMASK = [0, 1, 2, 3, 4, 5, 6]*55\n\nFREQNAMES = ['YEARLY', 'MONTHLY', 'WEEKLY', 'DAILY', 'HOURLY', 'MINUTELY', 'SECONDLY']\n\n(YEARLY,\nMONTHLY,\nWEEKLY,\nDAILY,\nHOURLY,\nMINUTELY,\nSECONDLY) = list(range(7))\n\n# Imported on demand.\neaster = None\nparser = None\n\nclass weekday(weekdaybase):\n\"\"\"\nThis version of weekday does not allow n = 0.\n\"\"\"\ndef __init__(self, wkday, n=None):\nif n == 0:\nraise ValueError(\"Can't create weekday with n==0\")\n\nsuper(weekday, self).__init__(wkday, n)\n\nMO, TU, WE, TH, FR, SA, SU = weekdays = tuple(weekday(x) for x in range(7))\n\ndef _invalidates_cache(f):\n\"\"\"\nDecorator for rruleset methods which may invalidate the\ncached length.\n\"\"\"\ndef inner_func(self, *args, **kwargs):\nrv = f(self, *args, **kwargs)\nself._invalidate_cache()\nreturn rv\n\nreturn inner_func\n\nclass rrulebase(object):\ndef __init__(self, cache=False):\nif cache:\nself._cache = []\nself._invalidate_cache()\nelse:\nself._cache = None\nself._cache_complete = False\nself._len = None\n\ndef __iter__(self):\nif self._cache_complete:\nreturn iter(self._cache)\nelif self._cache is None:\nreturn self._iter()\nelse:\nreturn self._iter_cached()\n\ndef _invalidate_cache(self):\nif self._cache is not None:\nself._cache = []\nself._cache_complete = False\nself._cache_gen = self._iter()\n\nif self._cache_lock.locked():\nself._cache_lock.release()\n\nself._len = None\n\ndef _iter_cached(self):\ni = 0\ngen = self._cache_gen\ncache = self._cache\nacquire = self._cache_lock.acquire\nrelease = self._cache_lock.release\nwhile gen:\nif i == len(cache):\nacquire()\nif self._cache_complete:\nbreak\ntry:\nfor j in range(10):\nexcept StopIteration:\nself._cache_gen = gen = None\nself._cache_complete = True\nbreak\nrelease()\nyield cache[i]\ni += 1\nwhile i < self._len:\nyield cache[i]\ni += 1\n\ndef __getitem__(self, item):\nif self._cache_complete:\nreturn self._cache[item]\nelif isinstance(item, slice):\nif item.step and item.step < 0:\nreturn list(iter(self))[item]\nelse:\nreturn list(itertools.islice(self,\nitem.start or 0,\nitem.stop or sys.maxsize,\nitem.step or 1))\nelif item >= 0:\ngen = iter(self)\ntry:\nfor i in range(item+1):\nexcept StopIteration:\nraise IndexError\nreturn res\nelse:\nreturn list(iter(self))[item]\n\ndef __contains__(self, item):\nif self._cache_complete:\nreturn item in self._cache\nelse:\nfor i in self:\nif i == item:\nreturn True\nelif i > item:\nreturn False\nreturn False\n\n# __len__() introduces a large performance penalty.\ndef count(self):\n\"\"\" Returns the number of recurrences in this set. It will have go\ntrough the whole recurrence, if this hasn't been done before. \"\"\"\nif self._len is None:\nfor x in self:\npass\nreturn self._len\n\ndef before(self, dt, inc=False):\n\"\"\" Returns the last recurrence before the given datetime instance. The\ninc keyword defines what happens if dt is an occurrence. With\ninc=True, if dt itself is an occurrence, it will be returned. \"\"\"\nif self._cache_complete:\ngen = self._cache\nelse:\ngen = self\nlast = None\nif inc:\nfor i in gen:\nif i > dt:\nbreak\nlast = i\nelse:\nfor i in gen:\nif i >= dt:\nbreak\nlast = i\nreturn last\n\ndef after(self, dt, inc=False):\n\"\"\" Returns the first recurrence after the given datetime instance. The\ninc keyword defines what happens if dt is an occurrence. With\ninc=True, if dt itself is an occurrence, it will be returned. \"\"\"\nif self._cache_complete:\ngen = self._cache\nelse:\ngen = self\nif inc:\nfor i in gen:\nif i >= dt:\nreturn i\nelse:\nfor i in gen:\nif i > dt:\nreturn i\nreturn None\n\ndef xafter(self, dt, count=None, inc=False):\n\"\"\"\nGenerator which yields up to count recurrences after the given\ndatetime instance, equivalent to after.\n\n:param dt:\nThe datetime at which to start generating recurrences.\n\n:param count:\nThe maximum number of recurrences to generate. If None (default),\ndates are generated until the recurrence rule is exhausted.\n\n:param inc:\nIf dt is an instance of the rule and inc is True, it is\nincluded in the output.\n\n:yields: Yields a sequence of datetime objects.\n\"\"\"\n\nif self._cache_complete:\ngen = self._cache\nelse:\ngen = self\n\n# Select the comparison function\nif inc:\ncomp = lambda dc, dtc: dc >= dtc\nelse:\ncomp = lambda dc, dtc: dc > dtc\n\n# Generate dates\nn = 0\nfor d in gen:\nif comp(d, dt):\nif count is not None:\nn += 1\nif n > count:\nbreak\n\nyield d\n\ndef between(self, after, before, inc=False, count=1):\n\"\"\" Returns all the occurrences of the rrule between after and before.\nThe inc keyword defines what happens if after and/or before are\nthemselves occurrences. With inc=True, they will be included in the\nlist, if they are found in the recurrence set. \"\"\"\nif self._cache_complete:\ngen = self._cache\nelse:\ngen = self\nstarted = False\nl = []\nif inc:\nfor i in gen:\nif i > before:\nbreak\nelif not started:\nif i >= after:\nstarted = True\nl.append(i)\nelse:\nl.append(i)\nelse:\nfor i in gen:\nif i >= before:\nbreak\nelif not started:\nif i > after:\nstarted = True\nl.append(i)\nelse:\nl.append(i)\nreturn l\n\n[docs]class rrule(rrulebase):\n\"\"\"\nThat's the base of the rrule operation. It accepts all the keywords\ndefined in the RFC as its constructor parameters (except byday,\nwhich was renamed to byweekday) and more. The constructor prototype is::\n\nrrule(freq)\n\nWhere freq must be one of YEARLY, MONTHLY, WEEKLY, DAILY, HOURLY, MINUTELY,\nor SECONDLY.\n\n.. note::\nPer RFC section 3.3.10, recurrence instances falling on invalid dates\nand times are ignored rather than coerced:\n\nRecurrence rules may generate recurrence instances with an invalid\ndate (e.g., February 30) or nonexistent local time (e.g., 1:30 AM\non a day where the local time is moved forward by an hour at 1:00\nAM). Such recurrence instances MUST be ignored and MUST NOT be\ncounted as part of the recurrence set.\n\nThis can lead to possibly surprising behavior when, for example, the\nstart date occurs at the end of the month:\n\n>>> from dateutil.rrule import rrule, MONTHLY\n>>> from datetime import datetime\n>>> start_date = datetime(2014, 12, 31)\n>>> list(rrule(freq=MONTHLY, count=4, dtstart=start_date))\n... # doctest: +NORMALIZE_WHITESPACE\n[datetime.datetime(2014, 12, 31, 0, 0),\ndatetime.datetime(2015, 1, 31, 0, 0),\ndatetime.datetime(2015, 3, 31, 0, 0),\ndatetime.datetime(2015, 5, 31, 0, 0)]\n\nAdditionally, it supports the following keyword arguments:\n\n:param dtstart:\nThe recurrence start. Besides being the base for the recurrence,\nmissing parameters in the final recurrence instances will also be\nextracted from this date. If not given, datetime.now() will be used\n:param interval:\nThe interval between each freq iteration. For example, when using\nYEARLY, an interval of 2 means once every two years, but with HOURLY,\nit means once every two hours. The default interval is 1.\n:param wkst:\nThe week start day. Must be one of the MO, TU, WE constants, or an\ninteger, specifying the first day of the week. This will affect\nrecurrences based on weekly periods. The default week start is got\nfrom calendar.firstweekday(), and may be modified by\ncalendar.setfirstweekday().\n:param count:\nIf given, this determines how many occurrences will be generated.\n\n.. note::\nAs of version 2.5.0, the use of the keyword until in conjunction\nwith count is deprecated, to make sure dateutil is fully\ncompliant with RFC-5545 Sec. 3.3.10 <https://tools.ietf.org/\nhtml/rfc5545#section-3.3.10>_. Therefore, until and count\n**must not** occur in the same call to rrule.\n:param until:\nIf given, this must be a datetime instance specifying the upper-bound\nlimit of the recurrence. The last recurrence in the rule is the greatest\ndatetime that is less than or equal to the value specified in the\nuntil parameter.\n\n.. note::\nAs of version 2.5.0, the use of the keyword until in conjunction\nwith count is deprecated, to make sure dateutil is fully\ncompliant with RFC-5545 Sec. 3.3.10 <https://tools.ietf.org/\nhtml/rfc5545#section-3.3.10>_. Therefore, until and count\n**must not** occur in the same call to rrule.\n:param bysetpos:\nIf given, it must be either an integer, or a sequence of integers,\npositive or negative. Each given integer will specify an occurrence\nnumber, corresponding to the nth occurrence of the rule inside the\nfrequency period. For example, a bysetpos of -1 if combined with a\nMONTHLY frequency, and a byweekday of (MO, TU, WE, TH, FR), will\nresult in the last work day of every month.\n:param bymonth:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the months to apply the recurrence to.\n:param bymonthday:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the month days to apply the recurrence to.\n:param byyearday:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the year days to apply the recurrence to.\n:param byeaster:\nIf given, it must be either an integer, or a sequence of integers,\npositive or negative. Each integer will define an offset from the\nEaster Sunday. Passing the offset 0 to byeaster will yield the Easter\nSunday itself. This is an extension to the RFC specification.\n:param byweekno:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the week numbers to apply the recurrence to. Week numbers\nhave the meaning described in ISO8601, that is, the first week of\nthe year is that containing at least four days of the new year.\n:param byweekday:\nIf given, it must be either an integer (0 == MO), a sequence of\nintegers, one of the weekday constants (MO, TU, etc), or a sequence\nof these constants. When given, these variables will define the\nweekdays where the recurrence will be applied. It's also possible to\nuse an argument n for the weekday instances, which will mean the nth\noccurrence of this weekday in the period. For example, with MONTHLY,\nor with YEARLY and BYMONTH, using FR(+1) in byweekday will specify the\nfirst friday of the month where the recurrence happens. Notice that in\nthe RFC documentation, this is specified as BYDAY, but was renamed to\navoid the ambiguity of that keyword.\n:param byhour:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the hours to apply the recurrence to.\n:param byminute:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the minutes to apply the recurrence to.\n:param bysecond:\nIf given, it must be either an integer, or a sequence of integers,\nmeaning the seconds to apply the recurrence to.\n:param cache:\nIf given, it must be a boolean value specifying to enable or disable\ncaching of results. If you will use the same rrule instance multiple\ntimes, enabling caching will improve the performance considerably.\n\"\"\"\ndef __init__(self, freq, dtstart=None,\ninterval=1, wkst=None, count=None, until=None, bysetpos=None,\nbymonth=None, bymonthday=None, byyearday=None, byeaster=None,\nbyweekno=None, byweekday=None,\nbyhour=None, byminute=None, bysecond=None,\ncache=False):\nsuper(rrule, self).__init__(cache)\nglobal easter\nif not dtstart:\nif until and until.tzinfo:\ndtstart = datetime.datetime.now(tz=until.tzinfo).replace(microsecond=0)\nelse:\ndtstart = datetime.datetime.now().replace(microsecond=0)\nelif not isinstance(dtstart, datetime.datetime):\ndtstart = datetime.datetime.fromordinal(dtstart.toordinal())\nelse:\ndtstart = dtstart.replace(microsecond=0)\nself._dtstart = dtstart\nself._tzinfo = dtstart.tzinfo\nself._freq = freq\nself._interval = interval\nself._count = count\n\n# Cache the original byxxx rules, if they are provided, as the _byxxx\n# attributes do not necessarily map to the inputs, and this can be\n# a problem in generating the strings. Only store things if they've\n# been supplied (the string retrieval will just use .get())\nself._original_rule = {}\n\nif until and not isinstance(until, datetime.datetime):\nuntil = datetime.datetime.fromordinal(until.toordinal())\nself._until = until\n\nif self._dtstart and self._until:\nif (self._dtstart.tzinfo is not None) != (self._until.tzinfo is not None):\n# According to RFC5545 Section 3.3.10:\n# https://tools.ietf.org/html/rfc5545#section-3.3.10\n#\n# > If the \"DTSTART\" property is specified as a date with UTC\n# > time or a date with local time and time zone reference,\n# > then the UNTIL rule part MUST be specified as a date with\n# > UTC time.\nraise ValueError(\n'RRULE UNTIL values must be specified in UTC when DTSTART '\n'is timezone-aware'\n)\n\nif count is not None and until:\nwarn(\"Using both 'count' and 'until' is inconsistent with RFC 5545\"\n\" and has been deprecated in dateutil. Future versions will \"\n\"raise an error.\", DeprecationWarning)\n\nif wkst is None:\nself._wkst = calendar.firstweekday()\nelif isinstance(wkst, integer_types):\nself._wkst = wkst\nelse:\nself._wkst = wkst.weekday\n\nif bysetpos is None:\nself._bysetpos = None\nelif isinstance(bysetpos, integer_types):\nif bysetpos == 0 or not (-366 <= bysetpos <= 366):\nraise ValueError(\"bysetpos must be between 1 and 366, \"\n\"or between -366 and -1\")\nself._bysetpos = (bysetpos,)\nelse:\nself._bysetpos = tuple(bysetpos)\nfor pos in self._bysetpos:\nif pos == 0 or not (-366 <= pos <= 366):\nraise ValueError(\"bysetpos must be between 1 and 366, \"\n\"or between -366 and -1\")\n\nif self._bysetpos:\nself._original_rule['bysetpos'] = self._bysetpos\n\nif (byweekno is None and byyearday is None and bymonthday is None and\nbyweekday is None and byeaster is None):\nif freq == YEARLY:\nif bymonth is None:\nbymonth = dtstart.month\nself._original_rule['bymonth'] = None\nbymonthday = dtstart.day\nself._original_rule['bymonthday'] = None\nelif freq == MONTHLY:\nbymonthday = dtstart.day\nself._original_rule['bymonthday'] = None\nelif freq == WEEKLY:\nbyweekday = dtstart.weekday()\nself._original_rule['byweekday'] = None\n\n# bymonth\nif bymonth is None:\nself._bymonth = None\nelse:\nif isinstance(bymonth, integer_types):\nbymonth = (bymonth,)\n\nself._bymonth = tuple(sorted(set(bymonth)))\n\nif 'bymonth' not in self._original_rule:\nself._original_rule['bymonth'] = self._bymonth\n\n# byyearday\nif byyearday is None:\nself._byyearday = None\nelse:\nif isinstance(byyearday, integer_types):\nbyyearday = (byyearday,)\n\nself._byyearday = tuple(sorted(set(byyearday)))\nself._original_rule['byyearday'] = self._byyearday\n\n# byeaster\nif byeaster is not None:\nif not easter:\nfrom dateutil import easter\nif isinstance(byeaster, integer_types):\nself._byeaster = (byeaster,)\nelse:\nself._byeaster = tuple(sorted(byeaster))\n\nself._original_rule['byeaster'] = self._byeaster\nelse:\nself._byeaster = None\n\n# bymonthday\nif bymonthday is None:\nself._bymonthday = ()\nself._bynmonthday = ()\nelse:\nif isinstance(bymonthday, integer_types):\nbymonthday = (bymonthday,)\n\nbymonthday = set(bymonthday) # Ensure it's unique\n\nself._bymonthday = tuple(sorted(x for x in bymonthday if x > 0))\nself._bynmonthday = tuple(sorted(x for x in bymonthday if x < 0))\n\n# Storing positive numbers first, then negative numbers\nif 'bymonthday' not in self._original_rule:\nself._original_rule['bymonthday'] = tuple(\nitertools.chain(self._bymonthday, self._bynmonthday))\n\n# byweekno\nif byweekno is None:\nself._byweekno = None\nelse:\nif isinstance(byweekno, integer_types):\nbyweekno = (byweekno,)\n\nself._byweekno = tuple(sorted(set(byweekno)))\n\nself._original_rule['byweekno'] = self._byweekno\n\n# byweekday / bynweekday\nif byweekday is None:\nself._byweekday = None\nself._bynweekday = None\nelse:\n# If it's one of the valid non-sequence types, convert to a\n# single-element sequence before the iterator that builds the\n# byweekday set.\nif isinstance(byweekday, integer_types) or hasattr(byweekday, \"n\"):\nbyweekday = (byweekday,)\n\nself._byweekday = set()\nself._bynweekday = set()\nfor wday in byweekday:\nif isinstance(wday, integer_types):\nelif not wday.n or freq > MONTHLY:\nelse:\n\nif not self._byweekday:\nself._byweekday = None\nelif not self._bynweekday:\nself._bynweekday = None\n\nif self._byweekday is not None:\nself._byweekday = tuple(sorted(self._byweekday))\norig_byweekday = [weekday(x) for x in self._byweekday]\nelse:\norig_byweekday = ()\n\nif self._bynweekday is not None:\nself._bynweekday = tuple(sorted(self._bynweekday))\norig_bynweekday = [weekday(*x) for x in self._bynweekday]\nelse:\norig_bynweekday = ()\n\nif 'byweekday' not in self._original_rule:\nself._original_rule['byweekday'] = tuple(itertools.chain(\norig_byweekday, orig_bynweekday))\n\n# byhour\nif byhour is None:\nif freq < HOURLY:\nself._byhour = {dtstart.hour}\nelse:\nself._byhour = None\nelse:\nif isinstance(byhour, integer_types):\nbyhour = (byhour,)\n\nif freq == HOURLY:\nself._byhour = self.__construct_byset(start=dtstart.hour,\nbyxxx=byhour,\nbase=24)\nelse:\nself._byhour = set(byhour)\n\nself._byhour = tuple(sorted(self._byhour))\nself._original_rule['byhour'] = self._byhour\n\n# byminute\nif byminute is None:\nif freq < MINUTELY:\nself._byminute = {dtstart.minute}\nelse:\nself._byminute = None\nelse:\nif isinstance(byminute, integer_types):\nbyminute = (byminute,)\n\nif freq == MINUTELY:\nself._byminute = self.__construct_byset(start=dtstart.minute,\nbyxxx=byminute,\nbase=60)\nelse:\nself._byminute = set(byminute)\n\nself._byminute = tuple(sorted(self._byminute))\nself._original_rule['byminute'] = self._byminute\n\n# bysecond\nif bysecond is None:\nif freq < SECONDLY:\nself._bysecond = ((dtstart.second,))\nelse:\nself._bysecond = None\nelse:\nif isinstance(bysecond, integer_types):\nbysecond = (bysecond,)\n\nself._bysecond = set(bysecond)\n\nif freq == SECONDLY:\nself._bysecond = self.__construct_byset(start=dtstart.second,\nbyxxx=bysecond,\nbase=60)\nelse:\nself._bysecond = set(bysecond)\n\nself._bysecond = tuple(sorted(self._bysecond))\nself._original_rule['bysecond'] = self._bysecond\n\nif self._freq >= HOURLY:\nself._timeset = None\nelse:\nself._timeset = []\nfor hour in self._byhour:\nfor minute in self._byminute:\nfor second in self._bysecond:\nself._timeset.append(\ndatetime.time(hour, minute, second,\ntzinfo=self._tzinfo))\nself._timeset.sort()\nself._timeset = tuple(self._timeset)\n\ndef __str__(self):\n\"\"\"\nOutput a string that would generate this RRULE if passed to rrulestr.\nThis is mostly compatible with RFC5545, except for the\ndateutil-specific extension BYEASTER.\n\"\"\"\n\noutput = []\nh, m, s = [None] * 3\nif self._dtstart:\noutput.append(self._dtstart.strftime('DTSTART:%Y%m%dT%H%M%S'))\nh, m, s = self._dtstart.timetuple()[3:6]\n\nparts = ['FREQ=' + FREQNAMES[self._freq]]\nif self._interval != 1:\nparts.append('INTERVAL=' + str(self._interval))\n\nif self._wkst:\nparts.append('WKST=' + repr(weekday(self._wkst))[0:2])\n\nif self._count is not None:\nparts.append('COUNT=' + str(self._count))\n\nif self._until:\nparts.append(self._until.strftime('UNTIL=%Y%m%dT%H%M%S'))\n\nif self._original_rule.get('byweekday') is not None:\n# The str() method on weekday objects doesn't generate\n# RFC5545-compliant strings, so we should modify that.\noriginal_rule = dict(self._original_rule)\nwday_strings = []\nfor wday in original_rule['byweekday']:\nif wday.n:\nwday_strings.append('{n:+d}{wday}'.format(\nn=wday.n,\nwday=repr(wday)[0:2]))\nelse:\nwday_strings.append(repr(wday))\n\noriginal_rule['byweekday'] = wday_strings\nelse:\noriginal_rule = self._original_rule\n\npartfmt = '{name}={vals}'\nfor name, key in [('BYSETPOS', 'bysetpos'),\n('BYMONTH', 'bymonth'),\n('BYMONTHDAY', 'bymonthday'),\n('BYYEARDAY', 'byyearday'),\n('BYWEEKNO', 'byweekno'),\n('BYDAY', 'byweekday'),\n('BYHOUR', 'byhour'),\n('BYMINUTE', 'byminute'),\n('BYSECOND', 'bysecond'),\n('BYEASTER', 'byeaster')]:\nvalue = original_rule.get(key)\nif value:\nparts.append(partfmt.format(name=name, vals=(','.join(str(v)\nfor v in value))))\n\noutput.append('RRULE:' + ';'.join(parts))\nreturn '\\n'.join(output)\n\n[docs] def replace(self, **kwargs):\n\"\"\"Return new rrule with same attributes except for those attributes given new\nvalues by whichever keyword arguments are specified.\"\"\"\nnew_kwargs = {\"interval\": self._interval,\n\"count\": self._count,\n\"dtstart\": self._dtstart,\n\"freq\": self._freq,\n\"until\": self._until,\n\"wkst\": self._wkst,\n\"cache\": False if self._cache is None else True }\nnew_kwargs.update(self._original_rule)\nnew_kwargs.update(kwargs)\nreturn rrule(**new_kwargs)\n\ndef _iter(self):\nyear, month, day, hour, minute, second, weekday, yearday, _ = \\\nself._dtstart.timetuple()\n\n# Some local variables to speed things up a bit\nfreq = self._freq\ninterval = self._interval\nwkst = self._wkst\nuntil = self._until\nbymonth = self._bymonth\nbyweekno = self._byweekno\nbyyearday = self._byyearday\nbyweekday = self._byweekday\nbyeaster = self._byeaster\nbymonthday = self._bymonthday\nbynmonthday = self._bynmonthday\nbysetpos = self._bysetpos\nbyhour = self._byhour\nbyminute = self._byminute\nbysecond = self._bysecond\n\nii = _iterinfo(self)\nii.rebuild(year, month)\n\ngetdayset = {YEARLY: ii.ydayset,\nMONTHLY: ii.mdayset,\nWEEKLY: ii.wdayset,\nDAILY: ii.ddayset,\nHOURLY: ii.ddayset,\nMINUTELY: ii.ddayset,\nSECONDLY: ii.ddayset}[freq]\n\nif freq < HOURLY:\ntimeset = self._timeset\nelse:\ngettimeset = {HOURLY: ii.htimeset,\nMINUTELY: ii.mtimeset,\nSECONDLY: ii.stimeset}[freq]\nif ((freq >= HOURLY and\nself._byhour and hour not in self._byhour) or\n(freq >= MINUTELY and\nself._byminute and minute not in self._byminute) or\n(freq >= SECONDLY and\nself._bysecond and second not in self._bysecond)):\ntimeset = ()\nelse:\ntimeset = gettimeset(hour, minute, second)\n\ntotal = 0\ncount = self._count\nwhile True:\n# Get dayset with the right frequency\ndayset, start, end = getdayset(year, month, day)\n\n# Do the \"hard\" work ;-)\nfiltered = False\nfor i in dayset[start:end]:\nif ((bymonth and ii.mmask[i] not in bymonth) or\n(byweekday and ii.wdaymask[i] not in byweekday) or\n((bymonthday or bynmonthday) and\n(byyearday and\n((i < ii.yearlen and i+1 not in byyearday and\n-ii.yearlen+i not in byyearday) or\n(i >= ii.yearlen and i+1-ii.yearlen not in byyearday and\n-ii.nextyearlen+i-ii.yearlen not in byyearday)))):\ndayset[i] = None\nfiltered = True\n\n# Output results\nif bysetpos and timeset:\nposlist = []\nfor pos in bysetpos:\nif pos < 0:\ndaypos, timepos = divmod(pos, len(timeset))\nelse:\ndaypos, timepos = divmod(pos-1, len(timeset))\ntry:\ni = [x for x in dayset[start:end]\nif x is not None][daypos]\ntime = timeset[timepos]\nexcept IndexError:\npass\nelse:\ndate = datetime.date.fromordinal(ii.yearordinal+i)\nres = datetime.datetime.combine(date, time)\nif res not in poslist:\nposlist.append(res)\nposlist.sort()\nfor res in poslist:\nif until and res > until:\nself._len = total\nreturn\nelif res >= self._dtstart:\nif count is not None:\ncount -= 1\nif count < 0:\nself._len = total\nreturn\ntotal += 1\nyield res\nelse:\nfor i in dayset[start:end]:\nif i is not None:\ndate = datetime.date.fromordinal(ii.yearordinal + i)\nfor time in timeset:\nres = datetime.datetime.combine(date, time)\nif until and res > until:\nself._len = total\nreturn\nelif res >= self._dtstart:\nif count is not None:\ncount -= 1\nif count < 0:\nself._len = total\nreturn\n\ntotal += 1\nyield res\n\n# Handle frequency and interval\nfixday = False\nif freq == YEARLY:\nyear += interval\nif year > datetime.MAXYEAR:\nself._len = total\nreturn\nii.rebuild(year, month)\nelif freq == MONTHLY:\nmonth += interval\nif month > 12:\ndiv, mod = divmod(month, 12)\nmonth = mod\nyear += div\nif month == 0:\nmonth = 12\nyear -= 1\nif year > datetime.MAXYEAR:\nself._len = total\nreturn\nii.rebuild(year, month)\nelif freq == WEEKLY:\nif wkst > weekday:\nday += -(weekday+1+(6-wkst))+self._interval*7\nelse:\nday += -(weekday-wkst)+self._interval*7\nweekday = wkst\nfixday = True\nelif freq == DAILY:\nday += interval\nfixday = True\nelif freq == HOURLY:\nif filtered:\nhour += ((23-hour)//interval)*interval\n\nif byhour:\nndays, hour = self.__mod_distance(value=hour,\nbyxxx=self._byhour,\nbase=24)\nelse:\nndays, hour = divmod(hour+interval, 24)\n\nif ndays:\nday += ndays\nfixday = True\n\ntimeset = gettimeset(hour, minute, second)\nelif freq == MINUTELY:\nif filtered:\nminute += ((1439-(hour*60+minute))//interval)*interval\n\nvalid = False\nrep_rate = (24*60)\nfor j in range(rep_rate // gcd(interval, rep_rate)):\nif byminute:\nnhours, minute = \\\nself.__mod_distance(value=minute,\nbyxxx=self._byminute,\nbase=60)\nelse:\nnhours, minute = divmod(minute+interval, 60)\n\ndiv, hour = divmod(hour+nhours, 24)\nif div:\nday += div\nfixday = True\nfiltered = False\n\nif not byhour or hour in byhour:\nvalid = True\nbreak\n\nif not valid:\nraise ValueError('Invalid combination of interval and ' +\n'byhour resulting in empty rule.')\n\ntimeset = gettimeset(hour, minute, second)\nelif freq == SECONDLY:\nif filtered:\nsecond += (((86399 - (hour * 3600 + minute * 60 + second))\n// interval) * interval)\n\nrep_rate = (24 * 3600)\nvalid = False\nfor j in range(0, rep_rate // gcd(interval, rep_rate)):\nif bysecond:\nnminutes, second = \\\nself.__mod_distance(value=second,\nbyxxx=self._bysecond,\nbase=60)\nelse:\nnminutes, second = divmod(second+interval, 60)\n\ndiv, minute = divmod(minute+nminutes, 60)\nif div:\nhour += div\ndiv, hour = divmod(hour, 24)\nif div:\nday += div\nfixday = True\n\nif ((not byhour or hour in byhour) and\n(not byminute or minute in byminute) and\n(not bysecond or second in bysecond)):\nvalid = True\nbreak\n\nif not valid:\nraise ValueError('Invalid combination of interval, ' +\n'byhour and byminute resulting in empty' +\n' rule.')\n\ntimeset = gettimeset(hour, minute, second)\n\nif fixday and day > 28:\ndaysinmonth = calendar.monthrange(year, month)\nif day > daysinmonth:\nwhile day > daysinmonth:\nday -= daysinmonth\nmonth += 1\nif month == 13:\nmonth = 1\nyear += 1\nif year > datetime.MAXYEAR:\nself._len = total\nreturn\ndaysinmonth = calendar.monthrange(year, month)\nii.rebuild(year, month)\n\ndef __construct_byset(self, start, byxxx, base):\n\"\"\"\nIf a BYXXX sequence is passed to the constructor at the same level as\nFREQ (e.g. FREQ=HOURLY,BYHOUR={2,4,7},INTERVAL=3), there are some\nspecifications which cannot be reached given some starting conditions.\n\nThis occurs whenever the interval is not coprime with the base of a\ngiven unit and the difference between the starting position and the\nending position is not coprime with the greatest common denominator\nbetween the interval and the base. For example, with a FREQ of hourly\nstarting at 17:00 and an interval of 4, the only valid values for\nBYHOUR would be {21, 1, 5, 9, 13, 17}, because 4 and 24 are not\ncoprime.\n\n:param start:\nSpecifies the starting position.\n:param byxxx:\nAn iterable containing the list of allowed values.\n:param base:\nThe largest allowable value for the specified frequency (e.g.\n24 hours, 60 minutes).\n\nThis does not preserve the type of the iterable, returning a set, since\nthe values should be unique and the order is irrelevant, this will\nspeed up later lookups.\n\nIn the event of an empty set, raises a :exception:ValueError, as this\nresults in an empty rrule.\n\"\"\"\n\ncset = set()\n\n# Support a single byxxx value.\nif isinstance(byxxx, integer_types):\nbyxxx = (byxxx, )\n\nfor num in byxxx:\ni_gcd = gcd(self._interval, base)\n# Use divmod rather than % because we need to wrap negative nums.\nif i_gcd == 1 or divmod(num - start, i_gcd) == 0:\n\nif len(cset) == 0:\nraise ValueError(\"Invalid rrule byxxx generates an empty set.\")\n\nreturn cset\n\ndef __mod_distance(self, value, byxxx, base):\n\"\"\"\nCalculates the next value in a sequence where the FREQ parameter is\nspecified along with a BYXXX parameter at the same \"level\"\n(e.g. HOURLY specified with BYHOUR).\n\n:param value:\nThe old value of the component.\n:param byxxx:\nThe BYXXX set, which should have been generated by\nrrule._construct_byset, or something else which checks that a\nvalid rule is present.\n:param base:\nThe largest allowable value for the specified frequency (e.g.\n24 hours, 60 minutes).\n\nIf a valid value is not found after base iterations (the maximum\nnumber before the sequence would start to repeat), this raises a\n:exception:ValueError, as no valid values were found.\n\nThis returns a tuple of divmod(n*interval, base), where n is the\nsmallest number of interval repetitions until the next specified\nvalue in byxxx is found.\n\"\"\"\naccumulator = 0\nfor ii in range(1, base + 1):\n# Using divmod() over % to account for negative intervals\ndiv, value = divmod(value + self._interval, base)\naccumulator += div\nif value in byxxx:\nreturn (accumulator, value)\n\nclass _iterinfo(object):\n__slots__ = [\"rrule\", \"lastyear\", \"lastmonth\",\n\"yearlen\", \"nextyearlen\", \"yearordinal\", \"yearweekday\",\n\ndef __init__(self, rrule):\nfor attr in self.__slots__:\nsetattr(self, attr, None)\nself.rrule = rrule\n\ndef rebuild(self, year, month):\n# Every mask is 7 days longer to handle cross-year weekly periods.\nrr = self.rrule\nif year != self.lastyear:\nself.yearlen = 365 + calendar.isleap(year)\nself.nextyearlen = 365 + calendar.isleap(year + 1)\nfirstyday = datetime.date(year, 1, 1)\nself.yearordinal = firstyday.toordinal()\nself.yearweekday = firstyday.weekday()\n\nwday = datetime.date(year, 1, 1).weekday()\nif self.yearlen == 365:\nself.mrange = M365RANGE\nelse:\nself.mrange = M366RANGE\n\nif not rr._byweekno:\nelse:\n# no1wkst = firstwkst = self.wdaymask.index(rr._wkst)\nno1wkst = firstwkst = (7-self.yearweekday+rr._wkst) % 7\nif no1wkst >= 4:\nno1wkst = 0\n# Number of days in the year, plus the days we got\n# from last year.\nwyearlen = self.yearlen+(self.yearweekday-rr._wkst) % 7\nelse:\n# Number of days in the year, minus the days we\n# left in last year.\nwyearlen = self.yearlen-no1wkst\ndiv, mod = divmod(wyearlen, 7)\nnumweeks = div+mod//4\nfor n in rr._byweekno:\nif n < 0:\nn += numweeks+1\nif not (0 < n <= numweeks):\ncontinue\nif n > 1:\ni = no1wkst+(n-1)*7\nif no1wkst != firstwkst:\ni -= 7-firstwkst\nelse:\ni = no1wkst\nfor j in range(7):\ni += 1\nbreak\nif 1 in rr._byweekno:\n# Check week number 1 of next year as well\n# TODO: Check -numweeks for next year.\ni = no1wkst+numweeks*7\nif no1wkst != firstwkst:\ni -= 7-firstwkst\nif i < self.yearlen:\n# If week starts in next year, we\nfor j in range(7):\ni += 1\nbreak\nif no1wkst:\n# Check last week number of last year as\n# well. If no1wkst is 0, either the year\n# started on week start, or week number 1\n# got days from last year, so there are no\n# days from last year's last week number in\n# this year.\nif -1 not in rr._byweekno:\nlyearweekday = datetime.date(year-1, 1, 1).weekday()\nlno1wkst = (7-lyearweekday+rr._wkst) % 7\nlyearlen = 365+calendar.isleap(year-1)\nif lno1wkst >= 4:\nlno1wkst = 0\nlnumweeks = 52+(lyearlen +\n(lyearweekday-rr._wkst) % 7) % 7//4\nelse:\nlnumweeks = 52+(self.yearlen-no1wkst) % 7//4\nelse:\nlnumweeks = -1\nif lnumweeks in rr._byweekno:\nfor i in range(no1wkst):\n\nif (rr._bynweekday and (month != self.lastmonth or\nyear != self.lastyear)):\nranges = []\nif rr._freq == YEARLY:\nif rr._bymonth:\nfor month in rr._bymonth:\nranges.append(self.mrange[month-1:month+1])\nelse:\nranges = [(0, self.yearlen)]\nelif rr._freq == MONTHLY:\nranges = [self.mrange[month-1:month+1]]\nif ranges:\n# Weekly frequency won't get here, so we may not\n# care about cross-year weekly periods.\nfor first, last in ranges:\nlast -= 1\nfor wday, n in rr._bynweekday:\nif n < 0:\ni = last+(n+1)*7\nelse:\ni = first+(n-1)*7\nif first <= i <= last:\n\nif rr._byeaster:\neyday = easter.easter(year).toordinal()-self.yearordinal\nfor offset in rr._byeaster:\n\nself.lastyear = year\nself.lastmonth = month\n\ndef ydayset(self, year, month, day):\nreturn list(range(self.yearlen)), 0, self.yearlen\n\ndef mdayset(self, year, month, day):\ndset = [None]*self.yearlen\nstart, end = self.mrange[month-1:month+1]\nfor i in range(start, end):\ndset[i] = i\nreturn dset, start, end\n\ndef wdayset(self, year, month, day):\n# We need to handle cross-year weeks here.\ndset = [None]*(self.yearlen+7)\ni = datetime.date(year, month, day).toordinal()-self.yearordinal\nstart = i\nfor j in range(7):\ndset[i] = i\ni += 1\n# if (not (0 <= i < self.yearlen) or\n# This will cross the year boundary, if necessary.\nbreak\nreturn dset, start, i\n\ndef ddayset(self, year, month, day):\ndset = [None] * self.yearlen\ni = datetime.date(year, month, day).toordinal() - self.yearordinal\ndset[i] = i\nreturn dset, i, i + 1\n\ndef htimeset(self, hour, minute, second):\ntset = []\nrr = self.rrule\nfor minute in rr._byminute:\nfor second in rr._bysecond:\ntset.append(datetime.time(hour, minute, second,\ntzinfo=rr._tzinfo))\ntset.sort()\nreturn tset\n\ndef mtimeset(self, hour, minute, second):\ntset = []\nrr = self.rrule\nfor second in rr._bysecond:\ntset.append(datetime.time(hour, minute, second, tzinfo=rr._tzinfo))\ntset.sort()\nreturn tset\n\ndef stimeset(self, hour, minute, second):\nreturn (datetime.time(hour, minute, second,\ntzinfo=self.rrule._tzinfo),)\n\nclass rruleset(rrulebase):\n\"\"\" The rruleset type allows more complex recurrence setups, mixing\nmultiple rules, dates, exclusion rules, and exclusion dates. The type\nconstructor takes the following keyword arguments:\n\n:param cache: If True, caching of results will be enabled, improving\nperformance of multiple queries considerably. \"\"\"\n\nclass _genitem(object):\ndef __init__(self, genlist, gen):\ntry:\ngenlist.append(self)\nexcept StopIteration:\npass\nself.genlist = genlist\nself.gen = gen\n\ndef __next__(self):\ntry:\nexcept StopIteration:\nif self.genlist is self:\nheapq.heappop(self.genlist)\nelse:\nself.genlist.remove(self)\nheapq.heapify(self.genlist)\n\nnext = __next__\n\ndef __lt__(self, other):\nreturn self.dt < other.dt\n\ndef __gt__(self, other):\nreturn self.dt > other.dt\n\ndef __eq__(self, other):\nreturn self.dt == other.dt\n\ndef __ne__(self, other):\nreturn self.dt != other.dt\n\ndef __init__(self, cache=False):\nsuper(rruleset, self).__init__(cache)\nself._rrule = []\nself._rdate = []\nself._exrule = []\nself._exdate = []\n\n@_invalidates_cache\ndef rrule(self, rrule):\n\"\"\" Include the given :py:class:rrule instance in the recurrence set\ngeneration. \"\"\"\nself._rrule.append(rrule)\n\n@_invalidates_cache\ndef rdate(self, rdate):\n\"\"\" Include the given :py:class:datetime instance in the recurrence\nset generation. \"\"\"\nself._rdate.append(rdate)\n\n@_invalidates_cache\ndef exrule(self, exrule):\n\"\"\" Include the given rrule instance in the recurrence set exclusion\nlist. Dates which are part of the given recurrence rules will not\nbe generated, even if some inclusive rrule or rdate matches them.\n\"\"\"\nself._exrule.append(exrule)\n\n@_invalidates_cache\ndef exdate(self, exdate):\n\"\"\" Include the given datetime instance in the recurrence set\nexclusion list. Dates included that way will not be generated,\neven if some inclusive rrule or rdate matches them. \"\"\"\nself._exdate.append(exdate)\n\ndef _iter(self):\nrlist = []\nself._rdate.sort()\nself._genitem(rlist, iter(self._rdate))\nfor gen in [iter(x) for x in self._rrule]:\nself._genitem(rlist, gen)\nexlist = []\nself._exdate.sort()\nself._genitem(exlist, iter(self._exdate))\nfor gen in [iter(x) for x in self._exrule]:\nself._genitem(exlist, gen)\nlastdt = None\ntotal = 0\nheapq.heapify(rlist)\nheapq.heapify(exlist)\nwhile rlist:\nritem = rlist\nif not lastdt or lastdt != ritem.dt:\nwhile exlist and exlist < ritem:\nexitem = exlist\nif exlist and exlist is exitem:\nheapq.heapreplace(exlist, exitem)\nif not exlist or ritem != exlist:\ntotal += 1\nyield ritem.dt\nlastdt = ritem.dt\nif rlist and rlist is ritem:\nheapq.heapreplace(rlist, ritem)\nself._len = total\n\nclass _rrulestr(object):\n\"\"\" Parses a string representation of a recurrence rule or set of\nrecurrence rules.\n\n:param s:\nRequired, a string defining one or more recurrence rules.\n\n:param dtstart:\nIf given, used as the default recurrence start if not specified in the\nrule string.\n\n:param cache:\nIf set True caching of results will be enabled, improving\nperformance of multiple queries considerably.\n\n:param unfold:\nIf set True indicates that a rule string is split over more\nthan one line and should be joined before processing.\n\n:param forceset:\nIf set True forces a :class:dateutil.rrule.rruleset to\nbe returned.\n\n:param compatible:\nIf set True forces unfold and forceset to be True.\n\n:param ignoretz:\nIf set True, time zones in parsed strings are ignored and a naive\n:class:datetime.datetime object is returned.\n\n:param tzids:\nIf given, a callable or mapping used to retrieve a\n:class:datetime.tzinfo from a string representation.\nDefaults to :func:dateutil.tz.gettz.\n\n:param tzinfos:\nAdditional time zone names / aliases which may be present in a string\nrepresentation. See :func:dateutil.parser.parse for more\ninformation.\n\n:return:\nReturns a :class:dateutil.rrule.rruleset or\n:class:dateutil.rrule.rrule\n\"\"\"\n\n_freq_map = {\"YEARLY\": YEARLY,\n\"MONTHLY\": MONTHLY,\n\"WEEKLY\": WEEKLY,\n\"DAILY\": DAILY,\n\"HOURLY\": HOURLY,\n\"MINUTELY\": MINUTELY,\n\"SECONDLY\": SECONDLY}\n\n_weekday_map = {\"MO\": 0, \"TU\": 1, \"WE\": 2, \"TH\": 3,\n\"FR\": 4, \"SA\": 5, \"SU\": 6}\n\ndef _handle_int(self, rrkwargs, name, value, **kwargs):\nrrkwargs[name.lower()] = int(value)\n\ndef _handle_int_list(self, rrkwargs, name, value, **kwargs):\nrrkwargs[name.lower()] = [int(x) for x in value.split(',')]\n\n_handle_INTERVAL = _handle_int\n_handle_COUNT = _handle_int\n_handle_BYSETPOS = _handle_int_list\n_handle_BYMONTH = _handle_int_list\n_handle_BYMONTHDAY = _handle_int_list\n_handle_BYYEARDAY = _handle_int_list\n_handle_BYEASTER = _handle_int_list\n_handle_BYWEEKNO = _handle_int_list\n_handle_BYHOUR = _handle_int_list\n_handle_BYMINUTE = _handle_int_list\n_handle_BYSECOND = _handle_int_list\n\ndef _handle_FREQ(self, rrkwargs, name, value, **kwargs):\nrrkwargs[\"freq\"] = self._freq_map[value]\n\ndef _handle_UNTIL(self, rrkwargs, name, value, **kwargs):\nglobal parser\nif not parser:\nfrom dateutil import parser\ntry:\nrrkwargs[\"until\"] = parser.parse(value,\nignoretz=kwargs.get(\"ignoretz\"),\ntzinfos=kwargs.get(\"tzinfos\"))\nexcept ValueError:\nraise ValueError(\"invalid until date\")\n\ndef _handle_WKST(self, rrkwargs, name, value, **kwargs):\nrrkwargs[\"wkst\"] = self._weekday_map[value]\n\ndef _handle_BYWEEKDAY(self, rrkwargs, name, value, **kwargs):\n\"\"\"\nTwo ways to specify this: +1MO or MO(+1)\n\"\"\"\nl = []\nfor wday in value.split(','):\nif '(' in wday:\n# If it's of the form TH(+1), etc.\nsplt = wday.split('(')\nw = splt\nn = int(splt[:-1])\nelif len(wday):\n# If it's of the form +1MO\nfor i in range(len(wday)):\nif wday[i] not in '+-0123456789':\nbreak\nn = wday[:i] or None\nw = wday[i:]\nif n:\nn = int(n)\nelse:\nraise ValueError(\"Invalid (empty) BYDAY specification.\")\n\nl.append(weekdays[self._weekday_map[w]](n))\nrrkwargs[\"byweekday\"] = l\n\n_handle_BYDAY = _handle_BYWEEKDAY\n\ndef _parse_rfc_rrule(self, line,\ndtstart=None,\ncache=False,\nignoretz=False,\ntzinfos=None):\nif line.find(':') != -1:\nname, value = line.split(':')\nif name != \"RRULE\":\nraise ValueError(\"unknown parameter name\")\nelse:\nvalue = line\nrrkwargs = {}\nfor pair in value.split(';'):\nname, value = pair.split('=')\nname = name.upper()\nvalue = value.upper()\ntry:\ngetattr(self, \"_handle_\"+name)(rrkwargs, name, value,\nignoretz=ignoretz,\ntzinfos=tzinfos)\nexcept AttributeError:\nraise ValueError(\"unknown parameter '%s'\" % name)\nexcept (KeyError, ValueError):\nraise ValueError(\"invalid '%s': %s\" % (name, value))\nreturn rrule(dtstart=dtstart, cache=cache, **rrkwargs)\n\ndef _parse_date_value(self, date_value, parms, rule_tzids,\nignoretz, tzids, tzinfos):\nglobal parser\nif not parser:\nfrom dateutil import parser\n\ndatevals = []\nvalue_found = False\nTZID = None\n\nfor parm in parms:\nif parm.startswith(\"TZID=\"):\ntry:\ntzkey = rule_tzids[parm.split('TZID=')[-1]]\nexcept KeyError:\ncontinue\nif tzids is None:\nfrom . import tz\ntzlookup = tz.gettz\nelif callable(tzids):\ntzlookup = tzids\nelse:\ntzlookup = getattr(tzids, 'get', None)\nif tzlookup is None:\nmsg = ('tzids must be a callable, mapping, or None, '\n'not %s' % tzids)\nraise ValueError(msg)\n\nTZID = tzlookup(tzkey)\ncontinue\n\n# RFC 5445 3.8.2.4: The VALUE parameter is optional, but may be found\n# only once.\nif parm not in {\"VALUE=DATE-TIME\", \"VALUE=DATE\"}:\nraise ValueError(\"unsupported parm: \" + parm)\nelse:\nif value_found:\nmsg = (\"Duplicate value parameter found in: \" + parm)\nraise ValueError(msg)\nvalue_found = True\n\nfor datestr in date_value.split(','):\ndate = parser.parse(datestr, ignoretz=ignoretz, tzinfos=tzinfos)\nif TZID is not None:\nif date.tzinfo is None:\ndate = date.replace(tzinfo=TZID)\nelse:\nraise ValueError('DTSTART/EXDATE specifies multiple timezone')\ndatevals.append(date)\n\nreturn datevals\n\ndef _parse_rfc(self, s,\ndtstart=None,\ncache=False,\nunfold=False,\nforceset=False,\ncompatible=False,\nignoretz=False,\ntzids=None,\ntzinfos=None):\nglobal parser\nif compatible:\nforceset = True\nunfold = True\n\nTZID_NAMES = dict(map(\nlambda x: (x.upper(), x),\nre.findall('TZID=(?P<name>[^:]+):', s)\n))\ns = s.upper()\nif not s.strip():\nraise ValueError(\"empty string\")\nif unfold:\nlines = s.splitlines()\ni = 0\nwhile i < len(lines):\nline = lines[i].rstrip()\nif not line:\ndel lines[i]\nelif i > 0 and line == \" \":\nlines[i-1] += line[1:]\ndel lines[i]\nelse:\ni += 1\nelse:\nlines = s.split()\nif (not forceset and len(lines) == 1 and (s.find(':') == -1 or\ns.startswith('RRULE:'))):\nreturn self._parse_rfc_rrule(lines, cache=cache,\ndtstart=dtstart, ignoretz=ignoretz,\ntzinfos=tzinfos)\nelse:\nrrulevals = []\nrdatevals = []\nexrulevals = []\nexdatevals = []\nfor line in lines:\nif not line:\ncontinue\nif line.find(':') == -1:\nname = \"RRULE\"\nvalue = line\nelse:\nname, value = line.split(':', 1)\nparms = name.split(';')\nif not parms:\nraise ValueError(\"empty property name\")\nname = parms\nparms = parms[1:]\nif name == \"RRULE\":\nfor parm in parms:\nraise ValueError(\"unsupported RRULE parm: \"+parm)\nrrulevals.append(value)\nelif name == \"RDATE\":\nfor parm in parms:\nif parm != \"VALUE=DATE-TIME\":\nraise ValueError(\"unsupported RDATE parm: \"+parm)\nrdatevals.append(value)\nelif name == \"EXRULE\":\nfor parm in parms:\nraise ValueError(\"unsupported EXRULE parm: \"+parm)\nexrulevals.append(value)\nelif name == \"EXDATE\":\nexdatevals.extend(\nself._parse_date_value(value, parms,\nTZID_NAMES, ignoretz,\ntzids, tzinfos)\n)\nelif name == \"DTSTART\":\ndtvals = self._parse_date_value(value, parms, TZID_NAMES,\nignoretz, tzids, tzinfos)\nif len(dtvals) != 1:\nraise ValueError(\"Multiple DTSTART values specified:\" +\nvalue)\ndtstart = dtvals\nelse:\nraise ValueError(\"unsupported property: \"+name)\nif (forceset or len(rrulevals) > 1 or rdatevals\nor exrulevals or exdatevals):\nif not parser and (rdatevals or exdatevals):\nfrom dateutil import parser\nrset = rruleset(cache=cache)\nfor value in rrulevals:\nrset.rrule(self._parse_rfc_rrule(value, dtstart=dtstart,\nignoretz=ignoretz,\ntzinfos=tzinfos))\nfor value in rdatevals:\nfor datestr in value.split(','):\nrset.rdate(parser.parse(datestr,\nignoretz=ignoretz,\ntzinfos=tzinfos))\nfor value in exrulevals:\nrset.exrule(self._parse_rfc_rrule(value, dtstart=dtstart,\nignoretz=ignoretz,\ntzinfos=tzinfos))\nfor value in exdatevals:\nrset.exdate(value)\nif compatible and dtstart:\nrset.rdate(dtstart)\nreturn rset\nelse:\nreturn self._parse_rfc_rrule(rrulevals,\ndtstart=dtstart,\ncache=cache,\nignoretz=ignoretz,\ntzinfos=tzinfos)\n\ndef __call__(self, s, **kwargs):\nreturn self._parse_rfc(s, **kwargs)\n\nrrulestr = _rrulestr()\n\n# vim:ts=4:sw=4:et"
] | [
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https://laceshawl.savingadvice.com/2008/08/ | [
"User Real IP - 34.204.193.85\n```Array\n(\n => Array\n(\n => 182.68.68.92\n)\n\n => Array\n(\n => 101.0.41.201\n)\n\n => Array\n(\n => 43.225.98.123\n)\n\n => Array\n(\n => 2.58.194.139\n)\n\n => Array\n(\n => 46.119.197.104\n)\n\n => Array\n(\n => 45.249.8.93\n)\n\n => Array\n(\n => 103.12.135.72\n)\n\n => Array\n(\n => 157.35.243.216\n)\n\n => Array\n(\n => 209.107.214.176\n)\n\n => Array\n(\n => 5.181.233.166\n)\n\n => Array\n(\n => 106.201.10.100\n)\n\n => Array\n(\n => 36.90.55.39\n)\n\n => Array\n(\n => 119.154.138.47\n)\n\n => Array\n(\n => 51.91.31.157\n)\n\n => Array\n(\n => 182.182.65.216\n)\n\n => Array\n(\n => 157.35.252.63\n)\n\n => Array\n(\n => 14.142.34.163\n)\n\n => Array\n(\n => 178.62.43.135\n)\n\n => Array\n(\n => 43.248.152.148\n)\n\n => Array\n(\n => 222.252.104.114\n)\n\n => Array\n(\n => 209.107.214.168\n)\n\n => Array\n(\n => 103.99.199.250\n)\n\n => Array\n(\n => 178.62.72.160\n)\n\n => Array\n(\n => 27.6.1.170\n)\n\n => Array\n(\n => 182.69.249.219\n)\n\n => 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119.153.40.69\n)\n\n => Array\n(\n => 49.36.133.64\n)\n\n => Array\n(\n => 103.255.4.249\n)\n\n => Array\n(\n => 198.144.154.15\n)\n\n => Array\n(\n => 1.22.46.172\n)\n\n => Array\n(\n => 103.255.5.46\n)\n\n => Array\n(\n => 27.56.195.188\n)\n\n => Array\n(\n => 203.101.167.53\n)\n\n => Array\n(\n => 117.230.62.195\n)\n\n => Array\n(\n => 103.240.194.186\n)\n\n => Array\n(\n => 107.170.166.118\n)\n\n => Array\n(\n => 101.53.245.80\n)\n\n => Array\n(\n => 157.43.13.208\n)\n\n => Array\n(\n => 137.97.100.77\n)\n\n => Array\n(\n => 47.31.150.208\n)\n\n => Array\n(\n => 137.59.222.65\n)\n\n => Array\n(\n => 103.85.127.250\n)\n\n => Array\n(\n => 103.214.119.32\n)\n\n => Array\n(\n => 182.255.49.52\n)\n\n => Array\n(\n => 103.75.247.72\n)\n\n => Array\n(\n => 103.85.125.250\n)\n\n => Array\n(\n => 183.83.253.167\n)\n\n => Array\n(\n => 1.39.222.111\n)\n\n => Array\n(\n => 111.119.185.9\n)\n\n => Array\n(\n => 111.119.187.10\n)\n\n => Array\n(\n => 39.37.147.144\n)\n\n => Array\n(\n => 103.200.198.183\n)\n\n => Array\n(\n => 1.39.222.18\n)\n\n => Array\n(\n => 198.8.80.103\n)\n\n => Array\n(\n => 42.108.1.243\n)\n\n => Array\n(\n => 111.119.187.16\n)\n\n => Array\n(\n => 39.40.241.8\n)\n\n => Array\n(\n => 122.169.150.158\n)\n\n => Array\n(\n => 39.40.215.119\n)\n\n => Array\n(\n => 103.255.5.77\n)\n\n => Array\n(\n => 157.38.108.196\n)\n\n => Array\n(\n => 103.255.4.67\n)\n\n => Array\n(\n => 5.62.60.62\n)\n\n => Array\n(\n => 39.37.146.202\n)\n\n => Array\n(\n => 110.138.6.221\n)\n\n => Array\n(\n => 49.36.143.88\n)\n\n => Array\n(\n => 37.1.215.39\n)\n\n => Array\n(\n => 27.106.59.190\n)\n\n => Array\n(\n => 139.167.139.41\n)\n\n => Array\n(\n => 114.142.166.179\n)\n\n => Array\n(\n => 223.225.240.112\n)\n\n => Array\n(\n => 103.255.5.36\n)\n\n => Array\n(\n => 175.136.1.48\n)\n\n => Array\n(\n => 103.82.80.166\n)\n\n => Array\n(\n => 182.185.196.126\n)\n\n => Array\n(\n => 157.43.45.76\n)\n\n => Array\n(\n => 119.152.132.49\n)\n\n => Array\n(\n => 5.62.62.162\n)\n\n => Array\n(\n => 103.255.4.39\n)\n\n => Array\n(\n => 202.5.144.153\n)\n\n => Array\n(\n => 1.39.223.210\n)\n\n => Array\n(\n => 92.38.176.154\n)\n\n => Array\n(\n => 117.230.186.142\n)\n\n => Array\n(\n => 183.83.39.123\n)\n\n => Array\n(\n => 182.185.156.76\n)\n\n => Array\n(\n => 104.236.74.212\n)\n\n => Array\n(\n => 107.170.145.187\n)\n\n => Array\n(\n => 117.102.7.98\n)\n\n => Array\n(\n => 137.59.220.0\n)\n\n => Array\n(\n => 157.47.222.14\n)\n\n => Array\n(\n => 47.15.206.82\n)\n\n => Array\n(\n => 117.230.159.99\n)\n\n => Array\n(\n => 117.230.175.151\n)\n\n => Array\n(\n => 157.50.97.18\n)\n\n => Array\n(\n => 117.230.47.164\n)\n\n => Array\n(\n => 77.111.244.34\n)\n\n => Array\n(\n => 139.167.189.131\n)\n\n => Array\n(\n => 1.39.204.103\n)\n\n => Array\n(\n => 117.230.58.0\n)\n\n => Array\n(\n => 182.185.226.66\n)\n\n => Array\n(\n => 115.42.70.119\n)\n\n => Array\n(\n => 171.48.114.134\n)\n\n => Array\n(\n => 144.34.218.75\n)\n\n => Array\n(\n => 199.58.164.135\n)\n\n => Array\n(\n => 101.53.228.151\n)\n\n => Array\n(\n => 117.230.50.57\n)\n\n => Array\n(\n => 223.225.138.84\n)\n\n => Array\n(\n => 110.225.67.65\n)\n\n => Array\n(\n => 47.15.200.39\n)\n\n => Array\n(\n => 39.42.20.127\n)\n\n => Array\n(\n => 117.97.241.81\n)\n\n => Array\n(\n => 111.119.185.11\n)\n\n => Array\n(\n => 103.100.5.94\n)\n\n => Array\n(\n => 103.25.137.69\n)\n\n => Array\n(\n => 47.15.197.159\n)\n\n => Array\n(\n => 223.188.176.122\n)\n\n => Array\n(\n => 27.4.175.80\n)\n\n => Array\n(\n => 181.215.43.82\n)\n\n => Array\n(\n => 27.56.228.157\n)\n\n => Array\n(\n => 117.230.19.19\n)\n\n => Array\n(\n => 47.15.208.71\n)\n\n => Array\n(\n => 119.155.21.176\n)\n\n => Array\n(\n => 47.15.234.202\n)\n\n => Array\n(\n => 117.230.144.135\n)\n\n => Array\n(\n => 112.79.139.199\n)\n\n => Array\n(\n => 116.75.246.41\n)\n\n => Array\n(\n => 117.230.177.126\n)\n\n => Array\n(\n => 212.103.48.134\n)\n\n => Array\n(\n => 102.69.228.78\n)\n\n => Array\n(\n => 117.230.37.118\n)\n\n => Array\n(\n => 175.143.61.75\n)\n\n => Array\n(\n => 139.167.56.138\n)\n\n => Array\n(\n => 58.145.189.250\n)\n\n => Array\n(\n => 103.255.5.65\n)\n\n => Array\n(\n => 39.37.153.182\n)\n\n => Array\n(\n => 157.43.85.106\n)\n\n => Array\n(\n => 185.209.178.77\n)\n\n => Array\n(\n => 1.39.212.45\n)\n\n => Array\n(\n => 103.72.7.16\n)\n\n => Array\n(\n => 117.97.185.244\n)\n\n => Array\n(\n => 117.230.59.106\n)\n\n => Array\n(\n => 137.97.121.103\n)\n\n => Array\n(\n => 103.82.123.215\n)\n\n => Array\n(\n => 103.68.217.248\n)\n\n => Array\n(\n => 157.39.27.175\n)\n\n => Array\n(\n => 47.31.100.249\n)\n\n => Array\n(\n => 14.171.232.139\n)\n\n => Array\n(\n => 103.31.93.208\n)\n\n => Array\n(\n => 117.230.56.77\n)\n\n => Array\n(\n => 124.182.25.124\n)\n\n => Array\n(\n => 106.66.191.242\n)\n\n => Array\n(\n => 175.107.237.25\n)\n\n => Array\n(\n => 119.155.1.27\n)\n\n => Array\n(\n => 72.255.6.24\n)\n\n => Array\n(\n => 192.140.152.223\n)\n\n => Array\n(\n => 212.103.48.136\n)\n\n => Array\n(\n => 39.45.134.56\n)\n\n => Array\n(\n => 139.167.173.30\n)\n\n => Array\n(\n => 117.230.63.87\n)\n\n => Array\n(\n => 182.189.95.203\n)\n\n => Array\n(\n => 49.204.183.248\n)\n\n => Array\n(\n => 47.31.125.188\n)\n\n => Array\n(\n => 103.252.171.13\n)\n\n => Array\n(\n => 112.198.74.36\n)\n\n => Array\n(\n => 27.109.113.152\n)\n\n => Array\n(\n => 42.112.233.44\n)\n\n => Array\n(\n => 47.31.68.193\n)\n\n => Array\n(\n => 103.252.171.134\n)\n\n => Array\n(\n => 77.123.32.114\n)\n\n => Array\n(\n => 1.38.189.66\n)\n\n => Array\n(\n => 39.37.181.108\n)\n\n => Array\n(\n => 42.106.44.61\n)\n\n => Array\n(\n => 157.36.8.39\n)\n\n => Array\n(\n => 223.238.41.53\n)\n\n => Array\n(\n => 202.89.77.10\n)\n\n => Array\n(\n => 117.230.150.68\n)\n\n => Array\n(\n => 175.176.87.60\n)\n\n => Array\n(\n => 137.97.117.87\n)\n\n => Array\n(\n => 132.154.123.11\n)\n\n => Array\n(\n => 45.113.124.141\n)\n\n => Array\n(\n => 103.87.56.203\n)\n\n => Array\n(\n => 159.89.171.156\n)\n\n => Array\n(\n => 119.155.53.88\n)\n\n => Array\n(\n => 222.252.107.215\n)\n\n => Array\n(\n => 132.154.75.238\n)\n\n => Array\n(\n => 122.183.41.168\n)\n\n => Array\n(\n => 42.106.254.158\n)\n\n => Array\n(\n => 103.252.171.37\n)\n\n => Array\n(\n => 202.59.13.180\n)\n\n => Array\n(\n => 37.111.139.137\n)\n\n => Array\n(\n => 39.42.93.25\n)\n\n => Array\n(\n => 118.70.177.156\n)\n\n => Array\n(\n => 117.230.148.64\n)\n\n => Array\n(\n => 39.42.15.194\n)\n\n => Array\n(\n => 137.97.176.86\n)\n\n => Array\n(\n => 106.210.102.113\n)\n\n => Array\n(\n => 39.59.84.236\n)\n\n => Array\n(\n => 49.206.187.177\n)\n\n => Array\n(\n => 117.230.133.11\n)\n\n => Array\n(\n => 42.106.253.173\n)\n\n => Array\n(\n => 178.62.102.23\n)\n\n => Array\n(\n => 111.92.76.175\n)\n\n => Array\n(\n => 132.154.86.45\n)\n\n => Array\n(\n => 117.230.128.39\n)\n\n => Array\n(\n => 117.230.53.165\n)\n\n => Array\n(\n => 49.37.200.171\n)\n\n => Array\n(\n => 104.236.213.230\n)\n\n => Array\n(\n => 103.140.30.81\n)\n\n => Array\n(\n => 59.103.104.117\n)\n\n => Array\n(\n => 65.49.126.79\n)\n\n => Array\n(\n => 202.59.12.251\n)\n\n => Array\n(\n => 37.111.136.17\n)\n\n => Array\n(\n => 163.53.85.67\n)\n\n => Array\n(\n => 123.16.240.73\n)\n\n => Array\n(\n => 103.211.14.183\n)\n\n => Array\n(\n => 103.248.93.211\n)\n\n => Array\n(\n => 116.74.59.127\n)\n\n => Array\n(\n => 137.97.169.254\n)\n\n => Array\n(\n => 113.177.79.100\n)\n\n => Array\n(\n => 74.82.60.187\n)\n\n => Array\n(\n => 117.230.157.66\n)\n\n => Array\n(\n => 169.149.194.241\n)\n\n => Array\n(\n => 117.230.156.11\n)\n\n => Array\n(\n => 202.59.12.157\n)\n\n => Array\n(\n => 42.106.181.25\n)\n\n => Array\n(\n => 202.59.13.78\n)\n\n => Array\n(\n => 39.37.153.32\n)\n\n => Array\n(\n => 177.188.216.175\n)\n\n => Array\n(\n => 222.252.53.165\n)\n\n => Array\n(\n => 37.139.23.89\n)\n\n => Array\n(\n => 117.230.139.150\n)\n\n => Array\n(\n => 104.131.176.234\n)\n\n => Array\n(\n => 42.106.181.117\n)\n\n => Array\n(\n => 117.230.180.94\n)\n\n => Array\n(\n => 180.190.171.5\n)\n\n => Array\n(\n => 150.129.165.185\n)\n\n => Array\n(\n => 51.15.0.150\n)\n\n => Array\n(\n => 42.111.4.84\n)\n\n => Array\n(\n => 74.82.60.116\n)\n\n => Array\n(\n => 137.97.121.165\n)\n\n => Array\n(\n => 64.62.187.194\n)\n\n => Array\n(\n => 137.97.106.162\n)\n\n => Array\n(\n => 137.97.92.46\n)\n\n => Array\n(\n => 137.97.170.25\n)\n\n => Array\n(\n => 103.104.192.100\n)\n\n => Array\n(\n => 185.246.211.34\n)\n\n => Array\n(\n => 119.160.96.78\n)\n\n => Array\n(\n => 212.103.48.152\n)\n\n => Array\n(\n => 183.83.153.90\n)\n\n => Array\n(\n => 117.248.150.41\n)\n\n => Array\n(\n => 185.240.246.180\n)\n\n => Array\n(\n => 162.253.131.125\n)\n\n => Array\n(\n => 117.230.153.217\n)\n\n => Array\n(\n => 117.230.169.1\n)\n\n => Array\n(\n => 49.15.138.247\n)\n\n => Array\n(\n => 117.230.37.110\n)\n\n => Array\n(\n => 14.167.188.75\n)\n\n => Array\n(\n => 169.149.239.93\n)\n\n => Array\n(\n => 103.216.176.91\n)\n\n => Array\n(\n => 117.230.12.126\n)\n\n => Array\n(\n => 184.75.209.110\n)\n\n => Array\n(\n => 117.230.6.60\n)\n\n => Array\n(\n => 117.230.135.132\n)\n\n => Array\n(\n => 31.179.29.109\n)\n\n => Array\n(\n => 74.121.188.186\n)\n\n => Array\n(\n => 117.230.35.5\n)\n\n => Array\n(\n => 111.92.74.239\n)\n\n => Array\n(\n => 104.245.144.236\n)\n\n => Array\n(\n => 39.50.22.100\n)\n\n => Array\n(\n => 47.31.190.23\n)\n\n => Array\n(\n => 157.44.73.187\n)\n\n => Array\n(\n => 117.230.8.91\n)\n\n => Array\n(\n => 157.32.18.2\n)\n\n => Array\n(\n => 111.119.187.43\n)\n\n => Array\n(\n => 203.101.185.246\n)\n\n => Array\n(\n => 5.62.34.22\n)\n\n)\n```\nArchive for August, 2008: Laceshawl's Personal Finance Blog\n << Back to all Blogs Login or Create your own free blog Layout: Blue and Brown (Default) Author's Creation\nHome > Archive: August, 2008",
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"",
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"",
null,
"# Archive for August, 2008\n\n## Pumpkin\n\nAugust 22nd, 2008 at 11:40 pm\n\nUnfortunately I have been unwell again and have had to quit my job. At least I have managed to save up enough to put me in a good financial position for the next few months, and hopefully I will get back to work in the New Year. In the meantime I am being veeerrry careful with the cash - no more buying coffees as I'm always tempted to buy a nice little ginger slice or sandwich or other goodie to go with it. The coffee alone costs nz\\$3. But I did buy a whole crown pumpkin for \\$1. Funny thing, I would never eat it when I was little, but now I know why nana served it so often. I have plenty of rice in the pantry as well, so I may get a little sick of pumpkin risotto. I have nz\\$4.20 in my pocket and no plans to buy anything other than milk until Wednesday."
] | [
null,
"https://www.savingadvice.com/blogs/images/search/top_left.php",
null,
"https://www.savingadvice.com/blogs/images/search/top_right.php",
null,
"https://www.savingadvice.com/blogs/images/search/bottom_left.php",
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9872989,"math_prob":0.99925894,"size":799,"snap":"2020-24-2020-29","text_gpt3_token_len":202,"char_repetition_ratio":0.09685534,"word_repetition_ratio":0.0,"special_character_ratio":0.24530663,"punctuation_ratio":0.083333336,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9996493,"pos_list":[0,1,2,3,4,5,6],"im_url_duplicate_count":[null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-01T05:43:26Z\",\"WARC-Record-ID\":\"<urn:uuid:e6bb910d-de34-4a7e-a5f3-4b54b8ac4047>\",\"Content-Length\":\"103810\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:1ab47566-59f0-4a95-b4fc-8e877250b9ef>\",\"WARC-Concurrent-To\":\"<urn:uuid:b29d4a2f-c8d2-42d3-be6c-6f1ae8dbd0fc>\",\"WARC-IP-Address\":\"173.231.200.26\",\"WARC-Target-URI\":\"https://laceshawl.savingadvice.com/2008/08/\",\"WARC-Payload-Digest\":\"sha1:QN2AJGKI5RV5L37F24TTUXPDVEGHDTOP\",\"WARC-Block-Digest\":\"sha1:WACT3U3PALBQKRJ3BO3FLDOVEDDRSUKI\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590347414057.54_warc_CC-MAIN-20200601040052-20200601070052-00532.warc.gz\"}"} |
https://www.physics.leidenuniv.nl/vanhecke/research/jamming-in-sand | [
"",
null,
"# Jamming in Sand\n\nWe all know that if you tilt a bucket filled with sand, the sand will only start to flow when the tilt reaches a certain angle. The sand immediately flows fast. If you want the sand to flow slowly, you should gently vibrate the bucket (as you do with breakfast cereal). In the lab we have a setup that allows us to do controlled flow experiments on weakly vibrated sand. We have a disk in the sand that is connected to a rheometer (see inset of the Figure (copied from our PRL (2011)). We measure how much torque (T) it takes to rotate the disk at a certain rotation rate (Ω) for different vibration amplitudes (Γ), where we keep the acceleration below 1g. The result is shown in the Figure.",
null,
"In the absence of vibrations (Γ=0), this curve has a large regime with a negative slope dT/dΩ < 0, this suggests that if you want the disk to rotate faster, you have to impose less torque! This is exactly the instability that causes the observation that you cannot let sand flow slowly out of a bucket. For Γ=0.5, there still is a small regime with a negative slope, but for low Ω, slow flow is possible. For Γ=1, the flow curve is monotonic as it would be for a Newtonian fluid such as water – the vibration liquefied the sand. The behavior of this system is very rich which means we can study many different properties of the system. A first example is that we are trying to characterize the phase transitions from no flow and slow flow to fast flow. Addionally, as recently reported in PRE (2014), we have found that if the grains are weakly vibrated, the system can no longer be described by concidering it purely from a frictional point of view."
] | [
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"https://www.physics.leidenuniv.nl/templates/lion/images/rsz_11matthijsvanspronsen-lionimageaward.png",
null,
"https://www.physics.leidenuniv.nl/images/project_mvh_vibrheo.png",
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.95632756,"math_prob":0.90807843,"size":1658,"snap":"2019-35-2019-39","text_gpt3_token_len":388,"char_repetition_ratio":0.11487304,"word_repetition_ratio":0.0,"special_character_ratio":0.22436671,"punctuation_ratio":0.08259587,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9518372,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,3,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-09-20T01:36:30Z\",\"WARC-Record-ID\":\"<urn:uuid:e740a943-0b36-4d11-aed1-73940adaf098>\",\"Content-Length\":\"17627\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:b623014f-e419-4018-825f-70f5566298e2>\",\"WARC-Concurrent-To\":\"<urn:uuid:f5d89adc-4efb-427d-8bc8-482572e1d9c2>\",\"WARC-IP-Address\":\"132.229.216.66\",\"WARC-Target-URI\":\"https://www.physics.leidenuniv.nl/vanhecke/research/jamming-in-sand\",\"WARC-Payload-Digest\":\"sha1:5Z5SQHFFQKO66UBUW6RN7SQKEOEEZKKN\",\"WARC-Block-Digest\":\"sha1:KJKNKPZ4AUUVKUI6M55YXLZJD245PJUJ\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-39/CC-MAIN-2019-39_segments_1568514573801.14_warc_CC-MAIN-20190920005656-20190920031656-00484.warc.gz\"}"} |
https://www.numbers.education/13121.html | [
"Is 13121 a prime number? What are the divisors of 13121?\n\n## Parity of 13 121\n\n13 121 is an odd number, because it is not evenly divisible by 2.\n\nFind out more:\n\n## Is 13 121 a perfect square number?\n\nA number is a perfect square (or a square number) if its square root is an integer; that is to say, it is the product of an integer with itself. Here, the square root of 13 121 is about 114.547.\n\nThus, the square root of 13 121 is not an integer, and therefore 13 121 is not a square number.\n\nAnyway, 13 121 is a prime number, and a prime number cannot be a perfect square.\n\n## What is the square number of 13 121?\n\nThe square of a number (here 13 121) is the result of the product of this number (13 121) by itself (i.e., 13 121 × 13 121); the square of 13 121 is sometimes called \"raising 13 121 to the power 2\", or \"13 121 squared\".\n\nThe square of 13 121 is 172 160 641 because 13 121 × 13 121 = 13 1212 = 172 160 641.\n\nAs a consequence, 13 121 is the square root of 172 160 641.\n\n## Number of digits of 13 121\n\n13 121 is a number with 5 digits.\n\n## What are the multiples of 13 121?\n\nThe multiples of 13 121 are all integers evenly divisible by 13 121, that is all numbers such that the remainder of the division by 13 121 is zero. There are infinitely many multiples of 13 121. The smallest multiples of 13 121 are:\n\n## Numbers near 13 121\n\n### Nearest numbers from 13 121\n\nFind out whether some integer is a prime number"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.8885059,"math_prob":0.9993371,"size":848,"snap":"2021-31-2021-39","text_gpt3_token_len":219,"char_repetition_ratio":0.19075829,"word_repetition_ratio":0.025641026,"special_character_ratio":0.2936321,"punctuation_ratio":0.12432432,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99880034,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-09-27T16:59:25Z\",\"WARC-Record-ID\":\"<urn:uuid:52e12b96-0b70-4748-a1ad-77d3aa3cf714>\",\"Content-Length\":\"18622\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:dc2678e7-a5c7-400e-a64c-cf3522dbffc2>\",\"WARC-Concurrent-To\":\"<urn:uuid:c5c14c31-b802-42d5-8ccc-66efc65b7de5>\",\"WARC-IP-Address\":\"213.186.33.19\",\"WARC-Target-URI\":\"https://www.numbers.education/13121.html\",\"WARC-Payload-Digest\":\"sha1:GOPAHVHEVJXPIJV2CI4RHXTTAXLZS52T\",\"WARC-Block-Digest\":\"sha1:7KFMJM4EARCAH6NHN5FBZ2CDHWPOKYYT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-39/CC-MAIN-2021-39_segments_1631780058456.86_warc_CC-MAIN-20210927151238-20210927181238-00605.warc.gz\"}"} |
https://tex.stackexchange.com/questions/445519/tikz-matrix-of-objects-in-latex | [
"# TikZ matrix of objects in LaTeX\n\nI want to make a TikZ matrix of objects, and then draw some vertical and horizontal lines. For instance, I would like to put the elements of the Polygon division example inside a tabular environment. So far, I checked more than 20 similar questions and none of them could really help me.\n\nI created the following minimal working example of what I want. The idea is to create all the possible simple networks of 3 vertices, and draw them in big rows according to their edge numbers (m), and grouped in columns depending on the degrees of the vertices of the top (k's). In every row, I put at the top the cases where the horizontal thicker edge exist and at the bottom where it doesn't. Every big column is defined by the degree of the vertex at the top left, and every smaller individual subcolumn has the degree pair of the top left and top right vertices, respectively.\n\n\\documentclass{minimal}\n\n\\usepackage{tikz}\n\\usetikzlibrary{matrix}\n\n\\begin{document}\n\n\\def\\side{0.5} % Define the size of the triangle's side\n\n\\newcommand{\\slice}{% Inverted triangle network\n\\filldraw (-\\side/2, {sqrt(3)*\\side/2}) circle (1pt) (\\side/2, {sqrt(3)*\\side/2}) circle (1pt) (0, 0) circle (1pt);\n\\filldraw \\foreach \\x/\\y in {#1} {(\\x) -- (\\y)};\n}\n\n\\begin{tikzpicture}\n% Define the inverted triangle coordinates\n\\coordinate (A) at (-\\side/2, {sqrt(3)*\\side/2});\n\\coordinate (B) at (\\side/2, {sqrt(3)*\\side/2});\n\\coordinate (C) at (0, 0);\n\n% Start the matrix\n\\matrix (M) [matrix of nodes, nodes={text width=7mm}, row sep=\\side*0.3cm]\n{\n{} & 0 & {} & {} & 1 & {} & {} & 2 & $k_i$ \\\\\n{} & $[0,0]$ & $[0,1]$ & $[1,0]$ & $[1,1]$ & $[1,2]$ & $[2,1]$ & $[2,2]$ & $[k_i,k_j]$ \\\\\n0 & \\slice{} & {} & {} & {} & {} & {} & {} & {} \\\\\n{} & {} & {} & {} & \\slice{A/B} \\draw[ultra thick] (A) -- (B); & {} & {} & {} & {} \\\\\n1 & {} & \\slice{B/C} & \\slice{A/C} & {} & {} & {} & {} & {} \\\\\n{} & {} & {} & {} & {} & \\slice{A/B, B/C} \\draw[ultra thick] (A) -- (B); & \\slice{A/B, A/C} \\draw[ultra thick] (A) -- (B); & {} & {} & {} \\\\\n2 & {} & {} & {} & \\slice{A/C, B/C} & {} & {} & {} & {} \\\\\n3 & {} & {} & {} & {} & {} & {} & \\slice{A/B, A/C, B/C} \\draw[ultra thick] (A) -- (B); & {} \\\\\n{} & {} & {} & {} & {} & {} & {} & {} & {} \\\\\n$m$ & {} & {} & {} & {} & {} & {} & {} & {} \\\\\n};\n% vertical lines\n\\foreach \\i in {2,...,9}{\n\\draw (M-2-\\i.north west) -- (M-9-\\i.south west);\n}\n\\draw[ultra thick]\n(M-1-2.north west) -- (M-9-2.south west)\n(M-1-4.north west) -- (M-9-4.south west)\n(M-1-7.north west) -- (M-9-7.south west)\n(M-1-9.north west) -- (M-9-9.south west)\n;\n% horizontal lines\n\\draw\n(M-2-2.south west) -- (M-2-8.south east)\n(M-3-1.south west) -- (M-3-8.south east)\n(M-5-1.south west) -- (M-5-8.south east)\n(M-7-1.south west) -- (M-7-8.south east)\n(M-9-1.south west) -- (M-9-8.south east)\n;\n\\end{tikzpicture}\n\n\\end{document}\n\n\nThe problems I faced are:\n\n1. When drawing the vertical and horizontal lines, I was forced to add extra rows or columns, because other way I received an error like\n\nPackage pgf Error: No shape named M-i-j is known...\n\nwhere of course i-j represents the location of my object (triangular network). A good example of this is the penultimate row that I added. As soon as there is no object in the matrix node, even if there is an empty element like {}, everything is OK.\n\n1. I don't know what is the best way to center the row or columns numbers. Is even hard to do it for the degree pairs inside the brackets, so I did it manually playing with the command\n\ntext width,\n\nand for the network objects I had to manually adjust their coordinate positions.\n\n1. I don't quite understand why the thicker vertical lines are not of the same size. In general, I would like to easily control and draw the lines. Any suggestion to make it similar to a tabular environment will be highly appreciated.\n2. The reason why I left m and the k's in their actual position is because what I explained in 1., so if somebody could help me to put them nicely in the top left corner of the matrix it will be awesome.\n\nJorge\n\n• Welcome to TeX.SE! I do not yet fully understand your code and problems, but it seems to me that you are nesting tikzpictures. That is, you have a matrix of nodes and then use \\filldraw inside the node contents. You may get rid of many issues by using path pictures instead. – user121799 Aug 10 '18 at 15:55\n• Thanks for your welcoming message :) I googled path picture examples and couldn't find anything useful yet, unfortunately. Could you provide an specific example maybe? – Jorge Aug 10 '18 at 16:09\n\n1. The shape unknown errors come because you did not tell TikZ that you want nodes in empty cells.\n2. One of the issues of your approach is that you are nesting tikzpictures. It is sort of intuitive that text width clashes with nested tikzpictures. You can use minimum size and align=center.\n3. I do not understand your 3rd question but in the answer below the lines have the width they got assigned.\n4. I do not understand the 4th question either, but perhaps you could just tell me where the (which?) k should be.\n\nHere is the updated code. Please note also that, in order to have the lines between the cells, one also has to draw them between, not south east or so of a given cell. This won't work because there are gaps between the cells. And this is the reason why I use all the ($(...)!0.5!(...)$) syntax, which just computes the average of two coordinates. I also made an effort in adding explanations in the code.\n\n\\documentclass[border=3.14mm]{standalone}\n\\usepackage{tikz}\n\\usetikzlibrary{matrix,calc,fit}\n\\newcounter{slicenum}\n\n\\begin{document}\n\n\\def\\side{0.5} % Define the size of the triangle's side\n\n% in order to avoid nesting nodes, we draw the triangles as path pictures\n% another option would be to store the triangles in \\savebox es and use those\n% for the nodes. But this approach is more flexible.\n% Also, in order to avoid confusion, I introduced a counter to discriminate\n% the nodes. Of course, this is not strictly necessary, and one may make this\n% slightly more elegant by using prefixes, but for the moment this will do.\n\\tikzset{slice/.style={path picture={\n\\stepcounter{slicenum}\n% \\draw (path picture bounding box.south west) rectangle\n% (path picture bounding box.north east);\n\\coordinate (O-\\theslicenum) at ($(path picture bounding box.south west)!0.5!(path picture bounding box.north east)$);\n\\pgfmathsetmacro{\\myshift}{2*(1-sqrt(3)/2)*\\side}\n\\coordinate (A-\\theslicenum) at\n($(O-\\theslicenum)+(150:\\side)+(0,{\\myshift})$);\n\\coordinate (B-\\theslicenum) at ($(O-\\theslicenum)+(30:\\side)+(0,{\\myshift})$);\n\\coordinate (C-\\theslicenum) at ($(O-\\theslicenum)+(-90:\\side)+(0,{\\myshift})$);\n\\filldraw (A-\\theslicenum) circle (1pt) (B-\\theslicenum) circle (1pt) (C-\\theslicenum) circle (1pt);\n\\foreach \\x/\\y/\\z in {#1} {\\draw[\\z] (\\x-\\theslicenum) -- (\\y-\\theslicenum);}\n}}}\n\n\\begin{tikzpicture}\n\n% Start the matrix\n\\matrix (M) [matrix of nodes,nodes in empty cells,nodes={\nminimum width=2.4*\\side*1cm,minimum height=2*\\side*1cm,align=center}]\n{\n& & & & & & & & \\\\\n\\makebox[0.8cm][r]{$[k_i,k_j]$} & $[0,0]$ & $[0,1]$ & $[1,0]$ & $[1,1]$ & $[1,2]$ & $[2,1]$ & $[2,2]$ &\n\\\\\n& |[slice=]| & & & & & & & \\\\\n& & & & |[slice={A/B/ultra thick}]| & & & & \\\\\n& & |[slice={B/C/}]| & |[slice={A/C/}]| & & & & & \\\\\n& & & & & |[slice={A/B/ultra thick, B/C/}]| & |[slice={A/B/ultra thick, A/C/}]|\n& & & \\\\\n& & & & |[slice={A/C/, B/C/}]| & & & & \\\\\n& & & & & & & |[slice={A/B/ultra thick, A/C/, B/C/}]| & \\\\\n& & & & & & & & \\\\\n& & & & & & & & \\\\\n};\n\\path (M-1-2) -- (M-1-3) node[midway]{0} (M-1-4) -- (M-1-6) node[midway]{1}\n(M-1-7) -- (M-1-8) node[midway]{2} (M-1-1) node[right]{$k_i$};\n\\path (M-3-1) node(0){$0$} (M-4-1)-- (M-5-1) node[midway](1){$1$}\n(M-6-1)-- (M-7-1) node[midway](2){$2$} (M-8-1)-- (M-9-1) node[midway](3){$3$} ;\n% horizontal lines\n\\path (0) -- (3) node[midway,left=6mm] (m) {$m$};\n\\foreach \\X in {0,...,3}\n{\\draw[-latex] (m) to[out=90-\\X*60,in=180] (\\X);}\n\\newcommand{\\DrawHorizontalLineInMatrix}[]{\n\\xdef\\Lst{(M-#2-2)}\n\\foreach \\XX in {3,...,8}\n{\\xdef\\Lst{\\Lst (M-#2-\\XX)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#2) {};\n\\xdef\\Lst{(M-#3-2)}\n\\foreach \\XX in {3,...,8}\n{\\xdef\\Lst{\\Lst (M-#3-\\XX)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#3) {};\n\\draw[#1] ($(fit-#2.south west)!0.5!(fit-#3.north west)$)\n-- ($(fit-#2.south east)!0.5!(fit-#3.north east)$);\n}\n\\foreach \\X[evaluate=\\X as \\Y using {int(\\X-1)}] in {2,4,...,10}\n{\n\\DrawHorizontalLineInMatrix[]{\\Y}{\\X}\n}\n% vertical lines\n\\newcommand{\\DrawVerticalLineInMatrix}[]{\n\\xdef\\Lst{(M-1-#2)}\n\\foreach \\XX in {2,...,9}\n{\\xdef\\Lst{\\Lst (M-\\XX-#2)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#2) {};\n\\xdef\\Lst{(M-1-#3)}\n\\foreach \\XX in {2,...,9}\n{\\xdef\\Lst{\\Lst (M-\\XX-#3)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#3) {};\n\\draw[#1] ($(fit-#2.north east)!0.5!(fit-#3.north west)$)\n-- ($(fit-#2.south east)!0.5!(fit-#3.south west)$);\n}\n\\DrawVerticalLineInMatrix{1}{2}\n\\foreach \\X[evaluate=\\X as \\Y using {int(\\X-1)}] in {2,4,7,9}\n{\n\\DrawVerticalLineInMatrix[ultra thick]{\\Y}{\\X}\n}\n\\end{tikzpicture}\n\\end{document}",
null,
"• Hi @marmot and thanks a lot. I read your fist answer and now the updated version. Regarding my 3rd question, in the code I wrote, the vertical lines are clearly of different size, is not important now with your solution. About the 4th question, $k_i$ represents the first element in the bracket, and this means your third and fourth vertical lines (from left to right) are misplaced, but is fixed easily changing {2,4,6,8} to {2,4,7,9} in one if the last lines of your code. I think the k's should be at the left and not at the right of the expressions. The same for m, it should be up and not down. – Jorge Aug 10 '18 at 21:40\n• I guess the most appealing way to see a matrix like this is similar to a joint probability table, see for instance math.stackexchange.com/questions/2634751/… so instead of X and Y, we have k_i, [k_i,k_j] for X, and m for Y. But is just an idea, maybe in LaTeX there is something better or simpler. – Jorge Aug 10 '18 at 22:27\n• @Jorge Either way but let's just remove all obsolete comments... – user121799 Aug 10 '18 at 23:24\n\nAn option using scope to locate a definition drawing inside respective matrix node center.\n\nMWE:\n\n\\documentclass[tikz,border=14pt]{standalone}\n\\usepackage{tikz}\n\\usetikzlibrary{matrix,arrows.meta, positioning,fit,shapes}\n\n\\begin{document}\n\\begin{tikzpicture}[\n%Environment config\n>={Stealth[inset=0pt,length=6pt]},\n%Environment Styles\nMyMatrix/.style={\nmatrix of nodes,\nfont=\\scriptsize,\nline width=0.75pt,\ncolumn sep=-0.5pt,\nrow sep=-0.5pt,\ntext height=18pt,\ntext width =24pt,\ntext depth =12pt,\nalign=center,\nnodes={draw=none},\nnodes in empty cells\n}\n]\n\n% Start Drawing the thing\n\\matrix[\nMyMatrix,\ncolumn 1/.style={nodes={draw=none},text width =12pt},\nrow 1/.style={text height =9pt,text depth =6pt},\nrow 2/.style={text height =9pt,text depth =4pt}\n] at (0,0) (M1){%Matrix contents\n&&&&&&&&\\\\\n&$[0,0]$&$[0,1]$&$[1,0]$&$[1,1]$&$[1,2]$&$[2,1]$&$[2,2]$&$[k_i,k_j]$\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n};\n%Draw thick vertical lines\n\\foreach \\x in {1,3,5,7,9}{\n\\draw[line width=2pt](M1-1-\\x.north east) -- (M1-10-\\x.south east);\n}\n%Draw horizontal lines\n\\foreach \\x in {1,2,...,10}{\n\\draw[line width=0.5pt](M1-\\x-1.south east) -- (M1-\\x-9.south east);\n}\n%Label row1\n\\foreach \\x [count=\\k from 1, evaluate=\\k as \\m using {int(\\k*2)}] in {0,1,2,$k_i$}{\n\\node at (M1-1-\\m.0){\\x};\n}\n%Label col1\n\\foreach \\x [count=\\k from 1, evaluate=\\k as \\m using {int(1+\\k*2)}] in {0,1,2,3}{\n\\node at (M1-\\m-1.center){\\x};\n}\n\n\\def\\slice(#1)[#2][#3][#4]{\n\\begin{scope}[shift={(#1)}]\n\\node[circle,fill,inner sep=1pt](c1) at (30:10pt){};\n\\node[circle,fill,inner sep=1pt](c2) at (150:10pt){};\n\\node[circle,fill,inner sep=1pt](c3) at (270:10pt){};\n\\path[#2](c1.center)--(c2.center);\n\\path[#3](c2.center)--(c3.center);\n\\path[#4](c3.center)--(c1.center);\n\\end{scope}\n}\n\n\\slice(M1-3-2.center)[][][]\n\\slice(M1-5-3.center)[][][draw]\n\\slice(M1-5-4.center)[][draw][]\n\\slice(M1-4-5.center)[draw,very thick][][]\n\\slice(M1-6-6.center)[draw,very thick][][draw]\n\\slice(M1-6-7.center)[draw,very thick][draw][]\n\\slice(M1-7-5.center)[][draw][draw]\n\\slice(M1-9-8.center)[draw,very thick][draw][draw]\n\n\\end{tikzpicture}\n\\end{document}\n\n• Hola @J Leon V. y muchas gracias por tu respuesta. I modified part of your code to achieve my requirements. It seems that I can't reply directly here with my new version of your code. Basically, I deleted many horizontal lines, added all the normal vertical lines, and corrected the misplaced third and fourth vertical lines (from left to right), as I previously explained to @marmot in the previous reply. I had to manually add the labels though. Should I write a new reply to my post to include this new version of your code? Thanks again! – Jorge Aug 10 '18 at 23:17\n• Que bien, Español !!!, Well, sometimes the OP brings some picture or hand drawing photo to explain what they need, and then the attempt code to scape from the \"do it for me\" situation to \"helpme to achieve this\", that help us to obtain the desired result, that I did was to propose a solution to draw inside matrix nodes and not more; and feel free to use or modify the code, but its polite to refer the author to recognize his / her dedicated time to answer. – J Leon V. Aug 11 '18 at 0:11\n\nMy version of J Leon V.'s code is\n\n\\documentclass[tikz,border=14pt]{standalone}\n\\usepackage{tikz}\n\\usetikzlibrary{matrix,arrows.meta, positioning,fit,shapes}\n\n\\begin{document}\n\\begin{tikzpicture}[\n%Environment config\n>={Stealth[inset=0pt,length=6pt]},\n%Environment Styles\nMyMatrix/.style={\nmatrix of nodes,\nfont=\\scriptsize,\nline width=0.75pt,\ncolumn sep=-0.5pt,\nrow sep=-0.5pt,\ntext height=18pt,\ntext width =24pt,\ntext depth =12pt,\nalign=center,\nnodes={draw=none},\nnodes in empty cells\n}\n]\n\n% Start Drawing the thing\n\\matrix[\nMyMatrix,\ncolumn 1/.style={nodes={draw=none},text width =12pt},\nrow 1/.style={text height =9pt,text depth =6pt},\nrow 2/.style={text height =9pt,text depth =4pt}\n] at (0,0) (M1){%Matrix contents\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n&&&&&&&&\\\\\n};\n%Draw thick vertical lines\n\\foreach \\x in {1,3,6,8}{\n\\draw[line width=2pt](M1-1-\\x.north east) -- (M1-8-\\x.south east);\n}\n%Draw vertical lines\n\\foreach \\x in {1,2,...,8}{\n\\draw[line width=0.5pt](M1-2-\\x.north east) -- (M1-8-\\x.south east);\n}\n%Draw horizontal lines\n\\foreach \\x in {2,3,5,7,8}{\n\\draw[line width=0.5pt](M1-\\x-1.south east) -- (M1-\\x-8.south east);\n}\n%Label row1\n\\node at (M1-1-2.0){0};\n\\node at (M1-1-5.center){1};\n\\node at (M1-1-7.0){2};\n\\node at (M1-1-9.center){$k_i$};\n\\node at (M1-2-2.center){$[0,0]$};\n\\node at (M1-2-3.center){$[0,1]$};\n\\node at (M1-2-4.center){$[1,0]$};\n\\node at (M1-2-5.center){$[1,1]$};\n\\node at (M1-2-6.center){$[1,2]$};\n\\node at (M1-2-7.center){$[2,1]$};\n\\node at (M1-2-8.center){$[2,2]$};\n\\node at (M1-2-9.center){$[k_i,k_j]$};\n%Label col1\n\\node at (M1-3-1.center){0};\n\\node at (M1-5-1.north){1};\n\\node at (M1-7-1.north){2};\n\\node at (M1-8-1.center){3};\n\\node at (M1-9-1.center){$m$};\n\n\\def\\slice(#1)[#2][#3][#4]{\n\\begin{scope}[shift={(#1)}]\n\\node[circle,fill,inner sep=1pt](c1) at (30:10pt){};\n\\node[circle,fill,inner sep=1pt](c2) at (150:10pt){};\n\\node[circle,fill,inner sep=1pt](c3) at (270:10pt){};\n\\path[#2](c1.center)--(c2.center);\n\\path[#3](c2.center)--(c3.center);\n\\path[#4](c3.center)--(c1.center);\n\\end{scope}\n}\n\n\\slice(M1-3-2.center)[][][]\n\\slice(M1-5-3.center)[][][draw]\n\\slice(M1-5-4.center)[][draw][]\n\\slice(M1-4-5.center)[draw,very thick][][]\n\\slice(M1-6-6.center)[draw,very thick][][draw]\n\\slice(M1-6-7.center)[draw,very thick][draw][]\n\\slice(M1-7-5.center)[][draw][draw]\n\\slice(M1-8-8.center)[draw,very thick][draw][draw]\n\n\\end{tikzpicture}\n\\end{document}\n\n\nAnd the result is",
null,
"My version of @marmot code is\n\n\\documentclass[border=3.14mm]{standalone}\n\\usepackage{tikz}\n\\usetikzlibrary{matrix,calc,fit}\n\\newcounter{slicenum}\n\n\\begin{document}\n\n\\def\\side{0.5} % Define the size of the triangle's side\n\n\\tikzset{slice/.style={path picture={\n\\stepcounter{slicenum}\n\\coordinate (O-\\theslicenum) at ($(path picture bounding box.south west)!0.5!(path picture bounding box.north east)$);\n\\pgfmathsetmacro{\\myshift}{2*(1-sqrt(3)/2)*\\side}\n\\coordinate (A-\\theslicenum) at\n($(O-\\theslicenum)+(150:\\side)+(0,{\\myshift})$);\n\\coordinate (B-\\theslicenum) at ($(O-\\theslicenum)+(30:\\side)+(0,{\\myshift})$);\n\\coordinate (C-\\theslicenum) at ($(O-\\theslicenum)+(-90:\\side)+(0,{\\myshift})$);\n\\filldraw (A-\\theslicenum) circle (1pt) (B-\\theslicenum) circle (1pt) (C-\\theslicenum) circle (1pt);\n\\foreach \\x/\\y/\\z in {#1} {\\draw[\\z] (\\x-\\theslicenum) -- (\\y-\\theslicenum);}\n}}}\n\n\\begin{tikzpicture}\n% Start the matrix\n\\matrix (M) [matrix of nodes, nodes in empty cells, nodes={minimum width=2.4*\\side*1cm, minimum height=2*\\side*1cm, align=center}]\n{\n& & & & & & & & \\\\\n& $[0,0]$ & $[0,1]$ & $[1,0]$ & $[1,1]$ & $[1,2]$ & $[2,1]$ & $[2,2]$ & \\\\\n& |[slice=]| & & & & & & & \\\\\n& & & & |[slice={A/B/ultra thick}]| & & & & \\\\\n& & |[slice={B/C/}]| & |[slice={A/C/}]| & & & & & \\\\\n& & & & & |[slice={A/B/ultra thick, B/C/}]| & |[slice={A/B/ultra thick, A/C/}]|\n& & & \\\\\n& & & & |[slice={A/C/, B/C/}]| & & & & \\\\\n& & & & & & & |[slice={A/B/ultra thick, A/C/, B/C/}]| & \\\\\n& & & & & & & & \\\\\n};\n\\path (M-1-2) -- (M-1-3) node[midway]{0} (M-1-4) -- (M-1-6) node[midway]{1} (M-1-7) -- (M-1-8) node[midway]{2} (M-1-1) node[right]{$k_i$};\n\\path (M-2-1) node[]{$[k_i,k_j]$};\n\\path (M-3-1) node(0){$0$} (M-4-1) -- (M-5-1) node[midway](1){$1$} (M-6-1) -- (M-7-1) node[midway](2){$2$} (M-8-1) node(3){$3$} ;\n% horizontal lines\n\\path (0) -- (3) node[midway,left=6mm] (m) {$m$};\n\\foreach \\X in {0,...,3}\n{\\draw[-latex] (m) to[out=90-\\X*60,in=180] (\\X);}\n\\newcommand{\\DrawHorizontalLineInMatrix}[]{\n\\xdef\\Lst{(M-#2-2)}\n\\foreach \\XX in {3,...,8}\n{\\xdef\\Lst{\\Lst (M-#2-\\XX)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#2) {};\n\\xdef\\Lst{(M-#3-2)}\n\\foreach \\XX in {3,...,8}\n{\\xdef\\Lst{\\Lst (M-#3-\\XX)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#3) {};\n\\draw[#1] ($(fit-#2.south west)!0.5!(fit-#3.north west)$)\n-- ($(fit-#2.south east)!0.5!(fit-#3.north east)$);\n}\n\\foreach \\X[evaluate=\\X as \\Y using {int(\\X-1)}] in {3,4,6,8,9}\n{\n\\DrawHorizontalLineInMatrix[]{\\Y}{\\X}\n}\n% thick vertical lines\n\\newcommand{\\DrawThickVerticalLineInMatrix}[]{\n\\xdef\\Lst{(M-1-#2)}\n\\foreach \\XX in {2,...,8}\n{\\xdef\\Lst{\\Lst (M-\\XX-#2)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#2) {};\n\\xdef\\Lst{(M-1-#3)}\n\\foreach \\XX in {2,...,8}\n{\\xdef\\Lst{\\Lst (M-\\XX-#3)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#3) {};\n\\draw[#1] ($(fit-#2.north east)!0.5!(fit-#3.north west)$)\n-- ($(fit-#2.south east)!0.5!(fit-#3.south west)$);\n}\n\\DrawThickVerticalLineInMatrix{1}{2}\n\\foreach \\X[evaluate=\\X as \\Y using {int(\\X-1)}] in {2,4,7,9}\n{\n\\DrawThickVerticalLineInMatrix[ultra thick]{\\Y}{\\X}\n}\n% vertical lines\n\\newcommand{\\DrawVerticalLineInMatrix}[]{\n\\xdef\\Lst{(M-2-#2)}\n\\foreach \\XX in {2,...,8}\n{\\xdef\\Lst{\\Lst (M-\\XX-#2)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#2) {};\n\\xdef\\Lst{(M-2-#3)}\n\\foreach \\XX in {2,...,8}\n{\\xdef\\Lst{\\Lst (M-\\XX-#3)}}\n\\node [fit=\\Lst,inner sep=0pt] (fit-#3) {};\n\\draw[#1] ($(fit-#2.north east)!0.5!(fit-#3.north west)$)\n-- ($(fit-#2.south east)!0.5!(fit-#3.south west)$);\n}\n\\foreach \\X[evaluate=\\X as \\Y using {int(\\X-1)}] in {3,5,6,8}\n{\n\\DrawVerticalLineInMatrix[]{\\Y}{\\X}\n}\n\\end{tikzpicture}\n\\end{document}\n\n\nAnd the result is",
null,
""
] | [
null,
"https://i.stack.imgur.com/0u47M.png",
null,
"https://i.stack.imgur.com/2GSl8.png",
null,
"https://i.stack.imgur.com/kUtWh.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.78593916,"math_prob":0.99232876,"size":4186,"snap":"2020-10-2020-16","text_gpt3_token_len":1334,"char_repetition_ratio":0.17886178,"word_repetition_ratio":0.14507772,"special_character_ratio":0.38294315,"punctuation_ratio":0.12742719,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98678434,"pos_list":[0,1,2,3,4,5,6],"im_url_duplicate_count":[null,4,null,4,null,4,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-02-17T22:24:48Z\",\"WARC-Record-ID\":\"<urn:uuid:65e90781-5e1d-4528-aa3f-d020acd542ae>\",\"Content-Length\":\"180776\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ef9a0143-7838-4b01-86ea-23e380445128>\",\"WARC-Concurrent-To\":\"<urn:uuid:2d4a6570-ee28-4abc-bd97-b2c3b73efcfc>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://tex.stackexchange.com/questions/445519/tikz-matrix-of-objects-in-latex\",\"WARC-Payload-Digest\":\"sha1:3ZYECUJDVKMN5FIM6HRIJ7QNVM5IOJLS\",\"WARC-Block-Digest\":\"sha1:2HERZZFNN6KJ3EYJAQZ2IHQV5HDK3MKT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-10/CC-MAIN-2020-10_segments_1581875143373.18_warc_CC-MAIN-20200217205657-20200217235657-00329.warc.gz\"}"} |
http://hostelbuisto.net/qspevdu_d001008003 | [
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null,
"常德路沿石价格_如何选购合格的路沿石\n\n品牌:金河,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n宽城金河建材构件必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:水泥管,市政砖,井盖,路沿石,路面砖\n\n•",
null,
"昌平盲点砖供应-优良盲点砖优选宽城金河建材\n\n品牌:金河,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n宽城金河建材构件必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:水泥管,市政砖,井盖,路沿石,路面砖\n\n•",
null,
"挡车器批发_专业的挡车器承德哪里有售\n\n品牌:承德翔飞,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n承德翔飞建筑装饰工程必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:环氧地坪,交通设施,装饰装修,地下车库金刚砂超耐磨地坪,交通设施工程\n\n•",
null,
"河北反光道钉-承德哪里有好用的反光道钉供应\n\n品牌:承德翔飞,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n承德翔飞建筑装饰工程必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:环氧地坪,交通设施,装饰装修,地下车库金刚砂超耐磨地坪,交通设施工程\n\n•",
null,
"粉状活性炭必威体育手机版推荐_河北有口皆碑的黄金活性炭\n\n品牌:华禹,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n承德华禹活性炭制造必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:活性炭,椰壳活性炭,粉状活性炭,椰壳黄金炭,果壳活性炭\n\n•",
null,
"承德快速卷帘门多少钱_承德快速卷帘门知名厂商\n\n品牌:承德翔飞,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n承德翔飞建筑装饰工程必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:环氧地坪,交通设施,装饰装修,地下车库金刚砂超耐磨地坪,交通设施工程\n\n•",
null,
"河北地坪漆必威体育手机版|买PVC地坪认准承德翔飞建筑公司\n\n品牌:承德翔飞,,\n\n出厂地:罗城仡佬族自治县(东门镇)\n\n报价:面议\n\n承德翔飞建筑装饰工程必威app安卓版\n\n黄金会员:",
null,
"经营模式:生产型\n\n主营:环氧地坪,交通设施,装饰装修,地下车库金刚砂超耐磨地坪,交通设施工程\n\n•",
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null,
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"经营模式:生产型\n\n主营:活性炭,椰壳活性炭,粉状活性炭,椰壳黄金炭,果壳活性炭\n\n• 没有找到合适的承德市供应商?您可以发布采购信息\n\n没有找到满足要求的承德市供应商?您可以搜索 批发 公司\n\n### 最新入驻必威体育手机版\n\n相关产品:\n常德路沿石价格 昌平盲点砖供应 挡车器批发 河北反光道钉 粉状活性炭必威体育手机版推荐 承德快速卷帘门多少钱 河北地坪漆必威体育手机版 脱色活性炭必威体育手机版 代理活性炭 活性炭必威体育手机版直销"
] | [
null,
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null,
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https://formatessays.com/we-have-an-urn-with-red-and-green-balls-with-an-x-or-y-on-them/ | [
"# We have an urn with red and green balls with an X or Y on them\n\nSuppose that we have an urn with red and green balls with an X or Y on them (i.e. four different kinds of balls, namely, Red – X , Red – Y , Green – X , Green – Y ). Suppose that we know the following:\n\nWe have an urn with red and green balls with an X or Y on them\n8.) Suppose that we have an urn with red and green balls with an X or Y on them (i.e. four different kinds of balls, namely, Red – X , Red – Y , Green – X , Green – Y ). Suppose that we know the following:\nP ( Red ) = .2, P ( Red and X ) = .1, and P ( X ) = .3\n\nFind:\nA.) P ( Green )\n\nB.) P ( Red or X )\n\nC.) P ( Red|X )\n\nD.) P ( X|Red )\n\nE.) Are events Red and X independent?\n\nF.) Why or why not? If they are not independent, change one of the probabilities given to make them independent.\n\n10.) Suppose the probability of being farsighted is .1. Suppose also that the probability of a farsighted person being dyslexic is .05 and the probability of a person who is not farsighted being dyslexic is .025 (1/2 as likely). What is the probability that a person with dyslexia is farsighted?\n\n11.) In baseball, suppose we are told that the probability of scoring a run on a double is .54. That is, given a play has generated a double, 54% of the time at least one run will score. However, we want to know how often when a run scores, it was generated by a double. This is not the same question. Do we see the difference? We are told that the probability of runs scoring on plays that are not doubles is .11 and the probability of hitting a double is 18%.\n\n13.) One cab company in our city is named “Blue Cab Co.”\nAnd they have had some complaints about the driving behavior of their employees. But we know that all cab companies have some drivers who are a bit reckless.\n\nWe know that the probability of getting a reckless driver if we are in a Blue Cab car is .25, but what we want to know is if we have a reckless driver, how likely is it a Blue Cab that we are in? Do we see the difference? We know the probability of getting a reckless driver if we are not in a Blue Cab car is .15, and we know the probability of getting a Blue Cab car is .4. So, what is the probability of being in a Blue Cab car if we have a reckless driver?\n\n3.) For each of the following situations, specify the null and alternative hypotheses:\n\nA.) The average respiration rate per minute is 8. Do smokers have an average rate different from 8?\n\nB.) The average score on the Beck Depression Inventory is 12. Does the average depression score of mothers with young children deviate from the population mean?\n\nC.) The average miles per gallon (mpg) of cars used in the United States is 20. Is the observed mpg of a sample of cars used in Japan different?\n\n4.) When conducting an inferential test, when should we use the t distribution?\n\n5.) `What if a researcher conducting a project using a single‐sample design has access to both the population and the sample standard deviation, which test should they use?\n\n7.) What type of error corresponds to a “false positive?”\n8.) What type of error corresponds to a “false negative?”\n\n11.) For which type of error can we set the precise risk rate, and which one can we only increase or decrease the chance of making?\n\n16.) Among trained typists, suppose it is known that the average typing speed using a standard keyboard is 60 words per minute (wpm), with a standard deviation of 5 wpm. The manufacturer of an ergonomically designed keyboard claims their device will improve typing speed. A random sample of 50 typists is tested on the ergonomically designed keyboard, and the sample mean wpm is 65. Test the hypothesis that using the new device affects typing speed. Set alpha at .05.\n\nA.)Should we use the z distribution or t distribution? Why?\n\nB.) State H 0 and H 1 .\n\nC.) What are the critical values?\n\nD.) What is the obtained statistic?\n\nE.) Reject the null hypothesis?\n\nF.) What type of decision error might have been made?\n\nG.) Is there sufficient evidence to support the manufacturer’s claim?\n\nH.) If so, what is the effect size?\n17.) On one standardized measure of IQ, μ = 100 and σ = 15. Imagine we want to test the hypothesis that children of parents with college degrees have an average IQ that is greater than the national average. A sample of 100 students who have college‐educated parents is randomly selected, and the mean is 110 with a standard deviation of 12. Conduct a test of the null hypothesis and set alpha at .05.\n\nA.) Should we use the z distribution or t distribution? Why?\n\nB.) State H 0 and H 1 .\n\nC.) What are the critical values?\n\nD.) What is the obtained statistic?\n\nE.)Reject the null hypothesis?\n\nF.) What type of decision error might have been made?\n\nG.) Interpret the finding.\n\nH.) If the null is rejected, what is the effect size?\n\n20.) An industrial/organizational psychologist believes that people who work at home experience greater job satisfaction. Imagine that a job satisfaction rating scale exists. The publishers of this scale claim the population is normally distributed with a mean of 50. The psychologist samples 20 people who work at home finding M = 63 and s = 17.\n\nA.) Should we use the z distribution or t distribution? Why?\nB.) State H 0 and H 1 .\n\nC.) What are the critical values?\n\nD.) What is the obtained statistic?\n\nE.) Reject the null hypothesis?\n\nF.) What type of decision error might have been made?\n\nG.) Interpret the finding.\n\nH.) If the null is rejected, what is the effect size?\n\n23.) anthropologist hypothesizes that physical stress in childhood increases height (Landauer & Whiting, 1964 ). The researchers locate a tribe of people in which physical stress is a by‐product of frequent tribal rituals (e.g. piercing and molding body parts, exposure to extreme temperatures, etc.). The mean height of the people in the region who do not use physically stressful rituals with their young is used as the population mean. The following raw data are for adult biological males and women of the tribe in question. Conduct a t test for men and a t test for women. The population mean height for men is 65 and 59 in. for women.\n\nMen Women\n67 59\n69 63\n72 65\n\n1. 60\n2. 59\n72 62\n64 61\n70 66\nA.) What is t obt for men?\nB.) What is t obt for women?\nC.) What are the critical values for each test ( α = .05)?\nD.) Compare each t obt with its respective critical values and interpret the findings; present the findings in a professionally appropriate manner.\n\n28.) health psychologist is interested in educating high school students about the negative effects of smoking. Fifty students who smoke are randomly selected to participate in the program. To measure the success of the program, the average number of cigarettes smoked per day among the participants is obtained 10 weeks after the end of the program.\n\nAssume that previous research had shown that, among all smoking students, the average number of cigarettes smoked in a day was 17. Set alpha at .05, and conduct a t test on the following data. Interpret the findings.\n\nAverage number of cigarettes consumed per day among participants\n12 11 7 0 0 6 2 23 45\n0 0 1 2 0 3 16 8 22 17 9\n12 10 6 5 9 11 0 33 24 5\n11 10 0 0 0 22 4 22 21 0\n10 11 0 6 7 11 3 42 38 0\n\n29.) An insurance company states that it takes them an average of 15 days to process an auto accident claim. A random sample of 40 claims is draw n from process claims over the past six months. Based on the following data, is there any evidence that the mean number of days to pay claims is not 15? Set α = .05.\n\nNumber of days to process a claim\n22 11 7 9 9 8 7 23 45 9\n23 21 8 8 5 16 9 22 17 6\n12 29 6 5 9 23 7 33 24 5\n15 14 9 7 3 17 8 19 15 8\n\n## Calculate the price of your order\n\n550 words\nWe'll send you the first draft for approval by September 11, 2018 at 10:52 AM\nTotal price:\n\\$26\nThe price is based on these factors:\nNumber of pages\nUrgency\nBasic features\n• Free title page and bibliography\n• Unlimited revisions\n• Plagiarism-free guarantee\n• Money-back guarantee\nOn-demand options\n• Writer’s samples\n• Part-by-part delivery\n• Overnight delivery\n• Copies of used sources\nPaper format\n• 275 words per page\n• 12 pt Arial/Times New Roman\n• Double line spacing\n• Any citation style (APA, MLA, Chicago/Turabian, Harvard)\n\n# Our Guarantees\n\n### Money-back Guarantee\n\nYou have to be 100% sure of the quality of your product to give a money-back guarantee. This describes us perfectly. Make sure that this guarantee is totally transparent.\n\n### Zero-plagiarism Guarantee\n\nEach paper is composed from scratch, according to your instructions. It is then checked by our plagiarism-detection software. There is no gap where plagiarism could squeeze in.\n\n### Free-revision Policy\n\nThanks to our free revisions, there is no way for you to be unsatisfied. We will work on your paper until you are completely happy with the result."
] | [
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9265996,"math_prob":0.9114886,"size":8109,"snap":"2021-43-2021-49","text_gpt3_token_len":1978,"char_repetition_ratio":0.10869833,"word_repetition_ratio":0.18955512,"special_character_ratio":0.26550746,"punctuation_ratio":0.12742858,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95772976,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-11-29T20:13:43Z\",\"WARC-Record-ID\":\"<urn:uuid:be1bc9bd-f309-42f3-9c32-f6cb2a30579a>\",\"Content-Length\":\"94134\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:770ccc9e-a939-4683-b5c8-00f234ceec29>\",\"WARC-Concurrent-To\":\"<urn:uuid:480323f3-bbb4-4d8f-a678-2f2bf630acee>\",\"WARC-IP-Address\":\"162.0.229.88\",\"WARC-Target-URI\":\"https://formatessays.com/we-have-an-urn-with-red-and-green-balls-with-an-x-or-y-on-them/\",\"WARC-Payload-Digest\":\"sha1:ROZMQ5QV5AF4T7MKIXEGSYEJ77DPUWM7\",\"WARC-Block-Digest\":\"sha1:4TB6LETRA4IBNQ26P5ANZFSMNJJQE6HJ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-49/CC-MAIN-2021-49_segments_1637964358842.4_warc_CC-MAIN-20211129194957-20211129224957-00432.warc.gz\"}"} |
https://www.mathvids.com/lesson_series/140/lessons/1413-trig-functions-special-angles-2 | [
"# Trig functions special angles 2\n\nTaught by YourMathGal\n• Currently 4.0/5 Stars.\n4701 views | 1 rating\nPart of video series\nMeets NCTM Standards:\nLesson Summary:\n\nIn this lesson, the teacher shows an easy way to find the trig functions of special angles and angles at multiples of 90 degrees. By using a right triangle and labeling the sides, the teacher demonstrates how to find the sine, cosine, tangent, cotangent, csc, and sec of each angle. Through seven examples, the teacher explains how to use this method, emphasizing that it is just one way of doing it and can be a helpful tool in finding exact trig function values.\n\nLesson Description:\n\nEasy way to use right triangle and label sides to find sin, cos, tan, cot, csc, and sec of the special angles, and of angles at multiples of 90 degrees. Part 2.\n\nMore free YouTube videos by Julie Harland are organized at http://yourmathgal.com\n\n• What are the special angles in trigonometry?\n• What is an easy way to find trig functions of special angles?\n• How can you use special triangles from geometry to easily find trig values on the unit circle?\n• What do sec, csc, and cot mean and how do you find their values?\n• How do you find cos 300 degrees?\n• How do you find cot 180 degrees?\n• How do you find sin 1305 degrees?\n• How do you find sec -210 degrees?\n• How do you find csc 750 degrees?\n• How do you find cos 270 degrees?\n• How do you find sin -420 degrees?\n•",
null,
"#### Staff Review\n\n• Currently 4.0/5 Stars.\nThis lesson continues from where the previous lesson left off but includes the trig functions secant (sec), cosecant (csc), and cotangent (cot). The 30, 60, 90 and 45, 45, 90 special triangles are used to easily find the values of trig functions at common angle measures. The answer to the final problem should be -(square root 3)/2, NOT -1/2."
] | [
null,
"https://www.mathvids.com/assets/testimonial/artist-testimonial-avatar-01-c96ee2a66f1e941fb1528708979edbcecf5383e31bcadfe00817b03e5645bd16.jpg",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.82084054,"math_prob":0.86552966,"size":707,"snap":"2023-14-2023-23","text_gpt3_token_len":158,"char_repetition_ratio":0.11806543,"word_repetition_ratio":0.032786883,"special_character_ratio":0.21782178,"punctuation_ratio":0.14666666,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98174864,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-05-30T10:07:50Z\",\"WARC-Record-ID\":\"<urn:uuid:c156558b-ce8a-425b-bafb-6f61c36caf64>\",\"Content-Length\":\"23516\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c43fa524-88c0-43d2-92f9-c8f3a3e0cc80>\",\"WARC-Concurrent-To\":\"<urn:uuid:d4e17a57-0731-4b12-969f-316be2644883>\",\"WARC-IP-Address\":\"104.16.244.78\",\"WARC-Target-URI\":\"https://www.mathvids.com/lesson_series/140/lessons/1413-trig-functions-special-angles-2\",\"WARC-Payload-Digest\":\"sha1:WD7XL4NKFNDVVLC7RRFDDEYSAOS3N2U6\",\"WARC-Block-Digest\":\"sha1:3GMZBHLUK7D7EBB3SKAKDP7Y4O7LETGL\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-23/CC-MAIN-2023-23_segments_1685224645595.10_warc_CC-MAIN-20230530095645-20230530125645-00262.warc.gz\"}"} |
https://crypto.stackexchange.com/questions/72083/how-to-encrypt-a-small-number-of-identities-which-are-related-to-each-other | [
"# How to encrypt a small number of identities (which are related to each other)? / Which algorithm has the smallest bit-length?\n\nI'm looking for an encryption with as small numbers as possible.\n\nGiven a small group of identities ($$G$$) (e.g. numbers from $$1$$ to $$N$$). Given one entry (or a small number) $$e_i$$ allows to compute another entry (like existence of a known generator/function). With this all group elements can get generated (which should take very long) or a constant fraction of it (which are a low amount ($$<100, <) of disjoint sets). All elements generated this way should lay in this initial group ($$G$$) or there need to exist a function $$f$$ which generates a unique element out of this initial group ($$f(e_i) \\in G$$). That means $$e_i$$ don't need to be in $$G$$ iff all elements we can generate $$E=\\{e_i, \\forall i \\in [1..|G|]\\}$$ and $$\\{f(e_i), \\forall i \\in [1..|G|]\\} = \\{G\\}$$\n\nNow given two random entries it should be hard to derive how one could be computed out of the other. Hard means it should take at least one year of computation for a current consumer PC for most cases (longer would be much better). There should be a way to generate each (or nearly) entry without the knowledge of any other or inner structure. E.g. for the example above were the identities are the numbers from $$1$$ to $$N$$ that could be just a random number. For an elliptic curves it would be some function which finds an element out of a random number.\n\nIn use case it will run at user PC. That means an attacker has access to the whole source code. Each user gets a random entry.\n\nToy example:\n\nprime $$P=13$$\n\nelements: $$1,..,12$$\n\ngenerator: prime root $$g=7$$\n\n$$e \\equiv g^a \\mod P$$ for $$a=1,..12$$ generates all elements\n\nGiven one random number $$r \\in [1..12]$$ as entry each other element can get generated out of it:\n\n$$\\{r \\cdot g^a \\mod P\\} = \\{g^a \\mod P\\}$$\n\nNow given another random $$r'$$ it is hard to compute $$a$$ for :\n\n$$r' \\equiv r \\cdot g^a \\mod P$$\n\n(at least for big numbers, discrecte logarithm).\n\nIf not a prime root for $$g$$ is picked, e.g. $$g=4$$ then each given random $$r'$$ can only produce one of two disjoint sets which would also be OK for use case.\n\nNow the toy example only works for large $$P$$ and with this a large number of group of identities. Now I'm looking for a way to do this with as small as possible groups. I'm also thankful for ideas which might work. Has this kind of encryption a special name?\n\nIdentity group size is less than 64-bit. As far as I know toy example or elliptic curves aren't safe for those small numbers.\n\n• Format preserving encryption is the right keyword. It's a symmetric cipher mode – Natanael Jul 21 at 21:29"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.8962359,"math_prob":0.9996836,"size":2406,"snap":"2019-43-2019-47","text_gpt3_token_len":640,"char_repetition_ratio":0.11781848,"word_repetition_ratio":0.0,"special_character_ratio":0.2788861,"punctuation_ratio":0.09803922,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99991846,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-11-18T14:14:24Z\",\"WARC-Record-ID\":\"<urn:uuid:2606f0b0-bd14-4c17-b148-b65ede663ff3>\",\"Content-Length\":\"136041\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ee9b432c-9ce8-44e1-80b1-0acdae660da4>\",\"WARC-Concurrent-To\":\"<urn:uuid:cad1d3c1-c88d-4ce2-b830-429db051568c>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://crypto.stackexchange.com/questions/72083/how-to-encrypt-a-small-number-of-identities-which-are-related-to-each-other\",\"WARC-Payload-Digest\":\"sha1:SS5Q6RNTQ2ZW2POFXDBJ2Z4OQUWPFZUY\",\"WARC-Block-Digest\":\"sha1:EZNM53VO4SLI4WTJYWVUOF6RPKYH4O4Z\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-47/CC-MAIN-2019-47_segments_1573496669795.59_warc_CC-MAIN-20191118131311-20191118155311-00412.warc.gz\"}"} |
https://zh.cppreference.com/w/cpp/language/copy_assignment | [
"# 复制赋值运算符\n\n< cpp | language\n\nC++\n 语言 标准库头文件 自立与有宿主实现 具名要求 语言支持库 概念库 (C++20) 诊断库 工具库 字符串库 容器库 迭代器库 范围库 (C++20) 算法库 数值库 输入/输出库 本地化库 正则表达式库 (C++11) 原子操作库 (C++11) 线程支持库 (C++11) 文件系统库 (C++17) 技术规范\n\n 概述 综述 class/struct 类型 union 类型 注入类名 成员 数据成员 静态成员 this 指针 嵌套类 成员模板 位域 using 声明 成员函数 成员访问指定符 构造函数与成员初始化器列表 默认成员初始化器(C++11) friend 指定符 explicit 指定符 转换构造函数 特殊成员函数 默认构造函数 复制构造函数 移动构造函数(C++11) 复制赋值运算符 移动赋值运算符(C++11) 析构函数 继承 基与派生类 空基类优化 虚成员函数 纯虚函数与抽象类 override(C++11) final(C++11)\n\nT 的复制赋值运算符是名为 operator= 的非模板非静态成员函数,它接收恰好一个 TT&const T&volatile T&const volatile T& 类型的形参。对于可复制赋值 (CopyAssignable) 类型,它必须有公开的复制赋值运算符。\n\n## 目录\n\n### [编辑]语法\n\n 类名 & 类名 :: operator= ( class_name ) (1) 类名 & 类名 :: operator= ( const class_name & ) (2) 类名 & 类名 :: operator= ( const 类名 & ) = default; (3) (C++11 起) 类名 & 类名 :: operator= ( const 类名 & ) = delete; (4) (C++11 起)\n\n### [编辑]解释\n\n1. 当可以使用复制并交换手法时,复制赋值运算符的典型声明。\n2. 当不能使用复制并交换手法时(不可交换类型或有性能退化),复制赋值运算符的典型声明。\n3. 强制编译器生成复制赋值运算符。\n4. 避免隐式复制赋值。\n\n### [编辑]隐式声明的复制赋值运算符\n\n• T 的每个直接基类 B 均拥有复制赋值运算符,其形参是 Bconst B&const volatile B&\n• T 的每个类类型或类数组类型的非静态数据成员 M 均拥有复制赋值运算符,其形参是 Mconst M&const volatile M&\n\n### [编辑]弃置的隐式声明的复制赋值运算符\n\n• T 拥有用户声明的移动构造函数;\n• T 拥有用户声明的移动赋值运算符。\n\n• T 拥有非类类型(或其数组)的 const 限定的非静态数据成员;\n• T 拥有引用类型的非静态数据成员;\n• T 拥有无法复制赋值的非静态数据成员,或直接或虚基类(对复制赋值的重载决议失败,或选择弃置或不可访问的函数);\n• T联合体式的类,且拥有对应复制赋值运算符非平凡的变体成员。\n\n### [编辑]平凡复制赋值运算符\n\n• 它不是用户提供的(即它是隐式定义或预置的),且若它被预置,则其签名与隐式定义的相同 (C++14 前)\n• T 没有虚成员函数;\n• T 没有虚基类;\n• T 的每个直接基类选择的复制赋值运算符都是平凡的;\n• T 的每个类类型(或类类型的数组)的非静态数据成员选择的复制赋值运算符都是平凡的;\n T 没有 volatile 限定类型的非静态数据成员。 (C++14 起)\n\n### [编辑]隐式定义的复制赋值运算符\n\nT 拥有用户定义的析构函数或用户定义的复制赋值运算符时,隐式定义的复制赋值运算符的生成被弃用。(C++11 起)\n\n### [编辑]示例\n\n#include <iostream>\n#include <memory>\n#include <string>\n#include <algorithm>\n\nstruct A\n{\nint n;\nstd::string s1;\n// 用户定义的复制赋值,复制并交换形式\nA& operator=(A other)\n{\nstd::cout << \"copy assignment of A\\n\";\nstd::swap(n, other.n);\nstd::swap(s1, other.s1);\nreturn *this;\n}\n};\n\nstruct B : A\n{\nstd::string s2;\n// 隐式定义的复制赋值\n};\n\nstruct C\n{\nstd::unique_ptr<int[]> data;\nstd::size_t size;\n// 非复制并交换的赋值\nC& operator=(const C& other)\n{\n// 检查自赋值\nif(&other == this)\nreturn *this;\n// 可能时复用存储\nif(size != other.size)\n{\ndata.reset(new int[other.size]);\nsize = other.size;\n}\nstd::copy(&other.data, &other.data + size, &data);\nreturn *this;\n}\n// 注意:复制并交换始终导致重分配\n};\n\nint main()\n{\nA a1, a2;\nstd::cout << \"a1 = a2 calls \";\na1 = a2; // 用户定义的复制赋值\n\nB b1, b2;\nb2.s1 = \"foo\";\nb2.s2 = \"bar\";\nstd::cout << \"b1 = b2 calls \";\nb1 = b2; // 隐式定义的复制赋值\nstd::cout << \"b1.s1 = \" << b1.s1 << \" b1.s2 = \" << b1.s2 << '\\n';\n}\n\na1 = a2 calls copy assignment of A\nb1 = b2 calls copy assignment of A\nb1.s1 = foo b1.s2 = bar\n\n### [编辑]缺陷报告\n\nDR 应用于 出版时的行为 正确行为\nCWG 2171 C++14 operator=(X&) = default 非平凡 令它平凡"
] | [
null
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https://kr.mathworks.com/matlabcentral/cody/problems/1116-calculate-the-height-of-an-object-dropped-from-the-sky | [
"Cody\n\n# Problem 1116. Calculate the height of an object dropped from the sky\n\nAssume that an object is dropped from 1000 meters above the surface of the earth at time t=0. The object is dropped such that the initial velocity and acceleration are both zero.\n\nWrite a function to determine the height, h, of the object at any time, t, where h=0 is the surface of the earth. Assume the acceleration due to gravity is constant 9.8 m/s^2. Also, assume that before the object is dropped (negative t) it is being held at a constant height of 1000 meters. Finally, assume that after the object hits the ground it remains at h=0.\n\n### Solution Stats\n\n50.43% Correct | 49.57% Incorrect\nLast Solution submitted on Nov 07, 2019"
] | [
null
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https://tnboardsolutions.com/samacheer-kalvi-11th-maths-guide-chapter-3-ex-3-11/ | [
"Tamilnadu State Board New Syllabus Samacheer Kalvi 11th Maths Guide Pdf Chapter 3 Trigonometry Ex 3.11 Text Book Back Questions and Answers, Notes.\n\n## Tamilnadu Samacheer Kalvi 11th Maths Solutions Chapter 3 Trigonometry Ex 3.11\n\nQuestion 1.\nFind the principal value of\n(i) sin-1 \n(ii) Cos-1 \n(iii) cosec-1 (- 1)\n(iv) sec-1 (- √2)\n(v) tan-1 (√3)\n(i) sin-1 $$\\frac{1}{\\sqrt{2}}$$",
null,
"",
null,
"",
null,
"(ii) Cos-1 $$\\frac{\\sqrt{3}}{2}$$",
null,
"(iii) cosec-1 (- 1)",
null,
"",
null,
"(iv) sec-1 (- √2)",
null,
"(v) tan-1 (√3)",
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"",
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"Question 2.\nA man standing directly opposite to one side of a road of width x meter views a circular shaped traffic green signal of diameter ‘a’ meter on the other side of the road. The bottom of the green signal Is ‘b’ meter height from the horizontal level of viewer’s eye. If ‘a’ denotes the angle subtended by the diameter of the green signal at the viewer’s eye, then prove that",
null,
"",
null,
"",
null,
""
] | [
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-1.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-2.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/01/SamacheerKalvi.Guide_.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-3.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-4.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/01/SamacheerKalvi.Guide_.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-5.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-6.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/01/SamacheerKalvi.Guide_.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-7.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-8.png",
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"https://tnboardsolutions.com/wp-content/uploads/2020/12/Samacheer-Kalvi-11th-Maths-Guide-Chapter-3-Trigonometry-Ex-3.11-9.png",
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https://www.jpost.com/features/bnei-menashe-rejoin-the-tribe | [
"(function (a, d, o, r, i, c, u, p, w, m) { m = d.getElementsByTagName(o), a[c] = a[c] || {}, a[c].trigger = a[c].trigger || function () { (a[c].trigger.arg = a[c].trigger.arg || []).push(arguments)}, a[c].on = a[c].on || function () {(a[c].on.arg = a[c].on.arg || []).push(arguments)}, a[c].off = a[c].off || function () {(a[c].off.arg = a[c].off.arg || []).push(arguments) }, w = d.createElement(o), w.id = i, w.src = r, w.async = 1, w.setAttribute(p, u), m.parentNode.insertBefore(w, m), w = null} )(window, document, \"script\", \"https://95662602.adoric-om.com/adoric.js\", \"Adoric_Script\", \"adoric\",\"9cc40a7455aa779b8031bd738f77ccf1\", \"data-key\");\nvar domain=window.location.hostname; var params_totm = \"\"; (new URLSearchParams(window.location.search)).forEach(function(value, key) {if (key.startsWith('totm')) { params_totm = params_totm +\"&\"+key.replace('totm','')+\"=\"+value}}); var rand=Math.floor(10*Math.random()); var script=document.createElement(\"script\"); script.src=`https://stag-core.tfla.xyz/pre_onetag?pub_id=34&domain=\\${domain}&rand=\\${rand}&min_ugl=0\\${params_totm}`; document.head.append(script);",
null,
""
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null,
"https://images.jpost.com/image/upload/f_auto,fl_lossy/t_JD_ArticleMainImage/37610",
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https://www.physicsoverflow.org/34146/spontaneously-broken-charge-operator-create-exactly-goldstone | [
"#",
null,
"Why does a spontaneously broken charge operator create exactly a one-Goldstone state?\n\n+ 3 like - 0 dislike\n217 views\n\nIt is commonly claimed that, if $j^0$ is a charge (density) that generates a spontaneously broken symmetry transformation, then\n\n$$j^0|\\text{VAC}\\rangle=|\\text{1-Goldstone}\\rangle\\cdots(1).$$\n\nIt can be shown (cf. Weinberg Vol2, chap 19, equation (19.2.34)), that $j^0|\\text{VAC}\\rangle$ has nonzero overlaps with 1-Goldstone states , but how can I see it's not, e.g., a supeposition 1-Goldstone and 2-Goldstone states? Or is equation (1) meant to be taken as a defining formula for 1-Goldstone state? In any case, there seems to be another paradox: it can also be shown (cf. Weinberg Vol2, chap 19, equation (19.2.35)), that $\\phi|VAC\\rangle$ has nonzero overlaps with 1-Goldstone states, where $\\phi$ is the scalar field that acquires VEV in the model. However, by Noether's theorem, $j^0$ is a quadratic function of $\\phi$ and $\\pi$ ($\\pi$ being the canonical conjugate of $\\phi$), and if $\\phi$ has a mode expansion at all, wouldn't $j^0$ have to contain a term that creates two particles?\n\nFurthermore, in demonstrating the non-existence of parity doubling of hadronic spectrum, it is claimed $$j^0|h\\rangle=|h, \\text{1-Goldstone}\\rangle\\cdots(2),$$\n\nwhere $|h\\rangle$ is a 1-hadron state. Even if I take for granted that $j^0$ creats a 1-Goldstone when acting on vacuum, it's still not clear to me why it does not do anything to the hadron at all.\n\n But note in Weinberg's proof, nowhere did he explicitly defined what a 1-Goldstone state is. He only loosely defined 1-particle state as a state of which momentum is the only continuous index, and 1-Goldstone as a massless 1-particle state with nonzero overlap with both $j^\\mu|\\text{VAC}\\rangle$ and $\\phi|\\text{VAC}\\rangle$.\n\n For example, M. Schwartz, Quantum field theory and standard model",
null,
"Also, Weinberg Vol 2, when talking about nonexistence of hadronic parity doubling:",
null,
"edited Nov 5, 2015\n\nThis is difficult to answer as the fields make sense only as interactive fields, about very little is known when one asks too precise questions. Where is (1) claimed?\n\nBy the way, it should be \"cf.\" and \"e.g.,\", not \"c.f.\" and \"e.g,\"\n\nTo your note : Weinberg defines after (19.2.8) what a Goldstone boson is - a pole in the effective action corresponding to a massless mode of the second derivative of the potential. Corresponding to each such pole is an asymptotic particle (Peskin-Schroeder, end of Section 11.5) that participates in the S-matrix and defines a Hilbert space of asymptotic 1-boson states. Being massless, these states cannot decay, hence this 1-particle space is preserved by translations, hence agrees with the space of nonasymptotic 1-boson states.\n\n@ArnoldNeumaier, I just added two references for equation (1) (and corrected c.f and e.g, of course :D)\n\nabout footnot , in his second proof of Goldstone theorem (the non-effective-potential, current-algebra-like approach), he writes down single Goldstone states such as $|B\\rangle$, but without writing its full relation with field operators, except some partial information such as (19.2.34) and (19.2.35).\n\n Please use answers only to (at least partly) answer questions. To comment, discuss, or ask for clarification, leave a comment instead. To mask links under text, please type your text, highlight it, and click the \"link\" button. You can then enter your link URL. Please consult the FAQ for as to how to format your post. This is the answer box; if you want to write a comment instead, please use the 'add comment' button. Live preview (may slow down editor) Preview Your name to display (optional): Email me at this address if my answer is selected or commented on: Privacy: Your email address will only be used for sending these notifications. Anti-spam verification: If you are a human please identify the position of the character covered by the symbol $\\varnothing$ in the following word:p$\\varnothing$ysicsOverflowThen drag the red bullet below over the corresponding character of our banner. When you drop it there, the bullet changes to green (on slow internet connections after a few seconds). To avoid this verification in future, please log in or register."
] | [
null,
"https://www.physicsoverflow.org/qa-plugin/po-printer-friendly/print_on.png",
null,
"https://www.physicsoverflow.org/34146/",
null,
"https://www.physicsoverflow.org/34146/",
null
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https://it.mathworks.com/help/curvefit/types-of-splines-ppform-and-b-form.html | [
"## Types of Splines: ppform and B-form\n\n### Polynomials vs. Splines\n\nPolynomials are the approximating functions of choice when a smooth function is to be approximated locally. For example, the truncated Taylor series\n\n`$\\sum _{i=0}^{n}{\\left(x-a\\right)}^{i}{D}^{i}f\\left(a\\right)/i!$`\n\nprovides a satisfactory approximation for f(x) if f is sufficiently smooth and x is sufficiently close to a. But if a function is to be approximated on a larger interval, the degree, n, of the approximating polynomial may have to be chosen unacceptably large. The alternative is to subdivide the interval [a..b] of approximation into sufficiently small intervals [ξj..ξj+1], with a = ξ1<··· <ξl+1 = b, so that, on each such interval, a polynomial pj of relatively low degree can provide a good approximation to f. This can even be done in such a way that the polynomial pieces blend smoothly, i.e., so that the resulting patched or composite function s(x) that equals pj(x) for x∊[ξj ξj+1], all j, has several continuous derivatives. Any such smooth piecewise polynomial function is called a spline. I.J. Schoenberg coined this term because a twice continuously differentiable cubic spline with sufficiently small first derivative approximates the shape of a draftsman's spline.\n\nThere are two commonly used ways to represent a polynomial spline, the ppform and the B-form. In this toolbox, a spline in ppform is often referred to as a piecewise polynomial, while a piecewise polynomial in B-form is often referred to as a spline. This reflects the fact that piecewise polynomials and (polynomial) splines are just two different views of the same thing.\n\n### ppform\n\nThe ppform of a polynomial spline of order k provides a description in terms of its breaks ξ1..ξl+1 and the local polynomial coefficients cji of its l pieces.\n\n`$\\begin{array}{cc}{p}_{j}\\left(x\\right)={\\sum _{i=1}^{k}\\left(x-{\\xi }_{j}\\right)}^{k-i}{c}_{ji},& j=1:l\\end{array}$`\n\nFor example, a cubic spline is of order 4, corresponding to the fact that it requires four coefficients to specify a cubic polynomial. The ppform is convenient for the evaluation and other uses of a spline.\n\n### B-form\n\nThe B-form has become the standard way to represent a spline during its construction, because the B-form makes it easy to build in smoothness requirements across breaks and leads to banded linear systems. The B-form describes a spline as a weighted sum\n\n`$\\sum _{j=1}^{n}{B}_{j,k}{a}_{j}$`\n\nof B-splines of the required order k, with their number, n, at least as big as k–1 plus the number of polynomial pieces that make up the spline. Here, Bj,k = B (·|tj, ...,tj+k) is the jth B-spline of order k for the knot sequence t1t2≤··· ≤tn+k. In particular, Bj,k is piecewise-polynomial of degree < k, with breaks tj, ...,tj+k , is nonnegative, is zero outside the interval [tj, ..tj+k], and is so normalized that\n\n`$\\begin{array}{ccc}\\sum _{j=1}^{n}{B}_{j,k}\\left(x\\right)=1& on& \\left[{t}_{k}..{t}_{n+1}\\right]\\end{array}$`\n\n### Knot Multiplicity\n\nThe multiplicity of the knots governs the smoothness, in the following way: If the number τ occurs exactly r times in the sequence tj,...tj+k, then Bj,k and its first k-r-1 derivatives are continuous across the break τ, while the (k-r)th derivative has a jump at τ. You can experiment with all these properties of the B-spline in a very visual and interactive way using the command `bspligui`."
] | [
null
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https://academic-calendar.wlu.ca/course.php?c=53048&cal=1&d=2070&s=932&y=79 | [
"# MA102Introduction to Functions and Differential Calculus0.5 Credit\n\nHours per week:\n• Lecture/Discussion: 3\n• Lab: 1.5\n\nRational, algebraic, trigonometric, logarithmic and exponential functions; equations and inequalities involving them. Thorough introduction to limits of functions. Continuity and its consequences. Introduction to differential calculus."
] | [
null
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https://justtothepoint.com/maths/natural-numbers-ii/ | [
"",
null,
"",
null,
"",
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"",
null,
"# Natural numbers II\n\nGo down deep enough into anything and you will find mathematics, Dean Schlicter.\n\nEverything that can be counted does not necessarily count; everything that counts cannot necessarily be counted, Albert Einstein.\n\n# Basic Arithmetic: Addition I. What is it? How does it work?\n\nThe four basic mathematical operations are: addition (+), subtraction(-), multiplication(x), and division(:). To understand addition have a look at this picture.",
null,
"There are two sets or group of apples. Let’s count them. There are three apples on the left and two on the right. How many apples do I have in total now? You’ve guessed it! We have five apples. In other words, three plus two equals five: 3 + 2 = 5. Three and two are the addends of the addition problem and five is the result of the sum.\n\nAdding two numbers together is like hoping or moving to the right along the Number Line.",
null,
"Adding is combining or putting together two or more things (candles, pencils, toys, etc.) or numbers. Numbers to be added are addends and the results of the additions are called sums: 2 + 4 = 6 ; 1 + 3 = 4; 2 + 3 = 5.\n\nAdding double-digit numbers is not as complicated as it looks or sounds. It is easy peasy lemon squeezy. Just follow these instructions to the letter, e.g., 31 + 45 Firstly, line the numbers up correctly:\n\n31\n+ 45\n------\nAnd then add the columns from right to left. You have to start by adding the numbers in the “ones” or the units column (1, 5), place the answer at the bottom of the units column, and then move to add the numbers in the “tens” column (3, 4), the tens are written on the second column.\n\n31\n+ 45\n------\n76\n\nHowever, what happens when the sum from the “ones” column is greater than nine? Let’s say 37 + 85, 7 + 5 ( = 12 ) is greater than 10 (12 > 10).\n\nCarry the one over the next column on the left (tens) and write two at the bottom of the units column. When numbers add up to more than ten, the tens need to be carried over to the next column to be added. 1\n\n37\n+ 85\n------\n122",
null,
"Another way of thinking about it is this: Round one or both addends before adding, thus: A. 40 (37 + 3) + 85 = 125, and then compensate the result. B. 125 - 3 = 122.\n\nTuxMath is a free arcade game that allows you to practice simple arithmetic operations, such as addition, subtraction, multiplication, and division.",
null,
"# Substraction I.\n\nSimplicity is about subtracting the obvious and adding the meaningful, John Maeda.\n\nDo you remember the story of Snow White? The story goes like this: “So the dwarves went hunting without Snow White and a wicked witch came to her. -Have an apple, said the wicked witch. And she handed her an enchanted apple that made her fall asleep.”\n\nYou may say: What’s the point in that fairytale? However, it turns out that apples are essential for learning subtraction. How many apples do we have?",
null,
"That’s right! We have 4 apples. Let’s imagine that a wicked witch has poisoned one of these tasty apples or a nasty worm has ruined an apple, how many edible apples are left?",
null,
"Exactly, there are 4 - 1 = 3 edible apples left. That’s it! It is as simple as that.\n\nLet’s see another example. Your mum has bought you seven sweets. Your best friend comes to your house and you offer him three. He works like a grasshopper but eats like a ravenous wolf. How many sweets do you have left? 7 - 3 = 4. You have four sweets left.\n\nImagine that you have eight bones and three dogs steal one bone each from you. How many bones do you have left? 8 -3 = 5 . Of course, you have 5 bones left.\n\nIf you want to add numbers together, you jump forwards on the Number Line. On the contrary, if you want to subtract numbers, you jump backwards as you can see in the screenshot below.",
null,
"# Subtraction II. 2 Digit Subtraction.\n\nSubtracting double-digit numbers is not very difficult, but it requires some skill. Just follow these instructions. Let’s subtract 45 - 31. Firstly, line the numbers up correctly\n\n45\n- 31\n------\n\nAnd then, subtract the columns from right to left. You have to start by subtracting the units, the numbers in the “ones” column (5, 1) and then, move on to subtract the numbers in the “tens” column (4, 3).\n\n45\n- 31\n------\n14\n\nHowever, what happens when you can’t subtract, because we all know that 7 is bigger than 5, don’t we?\n\n85\n- 37\n------\n\nJust make the “5” larger by borrowing or carrying from the “tens” column. This is called regrouping and you should understand that the number (85 = 70 + 15) remains the same. The calculation becomes 15 - 7 = 8.\n\nIt is like having eighty-five dollars. Having eight ten-dollar bills plus five one-dollar bills is the same as having seven ten-dollar bills plus fifteen one-dollar bills.\n\n85\n- 37\n------\n48\n\nNow, it’s your turn! Calculate 45 - 32, 24 - 12, 87 - 43, 23 - 19, 93-28, etc.\n\n# Multiplication. What is it? How does it work?\n\nMultiplication is basically repeated addition or adding equal groups together. For example, 4 multiplied by 3, 4 x 3 = 4 + 4 + 4 = 12. It equals 12. In other words, the number or factor 4 is added three times.\n\nObserve the following screenshot. We have three groups of five seals. Think about them together as a single group. How many seals are there in total?",
null,
"That’s right! We have 15 seals. We express this idea as: 5 * 3 = 15.\n\nAnother way of thinking about it is as follows. Imagine that your family (your Mum, your Dad, your sister, and you -4-) is having lunch and you have a yummy portion of a pizza in front of you and everyone else, too. Now, suppose for a moment that each one of your family invites two friends.\n\nHow can you share the pizza? It is easy, isn’t it? Just split each portion into three. Mathematically, we could say that 4 * 3 = 12 pizza portions. If everyone is still hungry and wants a whole pizza each, you will need to order 12 pizzas because you are twelve. It is another way of looking at it.\n\nA multiple is the result of multiplying a number by an integer. In our example, 12 is a multiple of 3. A times table is a chart or list of multiples of a given number.",
null,
"# Multiplication II. Times tables.\n\nDo you have problems memorizing the multiplication tables? Do not worry my friend, you are in the right place!\n\n0 times table. Anything times zero is zero.\n\n1 times table. Anything times 1 is itself. 1x0=0, 1x1=1, 1x2=2, 1x3=3, 1x4=4, 1x5=5, 1x6=6, 1x7=7, 1x8=8, 1x9=9, 1x10=10.\n\n2 times table. Anything times 2 is doubled and has to end in an even number, 3 * 2 = 3 + 3 = 6. 2x0=0, 2x1=2, 2x2=4, 2x3=6, 2x4=8, 2x5=10, 2x6=12, 2x7=14, 2x8=16, 2x9=18, 2x10=20.\n\n3 and 4 times tables. You need to learn to count by three and four respectively.\n\n3x0=0, 3x1=3, 3x2=6, 3x3=9, 3x4=12, 3x5=15, 3x6=18, 3x7=21, 3x8=24, 3x9=27, 3x10=30.\n\n4x0=0, 4x1=4, 4x2=8, 4x3=12, 4x4=16, 4x5=20, 4x6=24, 4x7=28, 4x8=32, 4x9=36, 4x10=40.\n\n5 times table. Anything times 5 has to end in either a zero or a five. 5x0=0, 5x1=5, 5x2=10, 5x3=15, 5x4=20, 5x5=25, 5x6=30, 5x7=35, 5x8=40, 5x9=45, 5x10=50.\n\n10 times table. Anything times ten is itself and add a zero. 10x0=0, 10x1=10, 10x2=20, 10x3=30, 10x4=40, 10x5=50, 10x6=60, 10x7=70, 10x8=80, 10x9=90, 10x10=100.\n\nLet’s see the most difficult part. Every finger represents a number. Your thumb is the six, the index finger is the seven, and so on. We are going to multiply seven by seven. Then, the index finger (the finger number seven) of one hand has to touch the finger number seven of the other hand. These fingers (both index fingers) with all the fingers beneath them (both thumbs) are tens, thus we have 40 (two index fingers and two thumbs).\n\nNext, you multiply one hand’s remaining fingers by the other hand’s remaining fingers: 3 * 3 = 9, so 7 * 7 = 40 (four index fingers and four thumbs) + 9 = 49.\n\nTry 8 * 7. One hand’s middle finger (8) has to touch the other hand’s index finger (7). These fingers and all the fingers under them are tens, and therefore we have 50 (two thumbs, two index fingers, and one middle finger). Then, we multiply the first hand’s remaining fingers by the second hand’s remaining fingers: 2 * 3 = 6. It is very easy, isn’t it? 8 * 7 = 50 + 6 = 56.",
null,
"# Multiplication III. 2 Digit Multiplication.\n\nMultiplying double-digit numbers is a very straight forward process as I am going to illustrate to you right now. Let’s calculate 31 * 45. Firstly, you need to line the numbers up correctly.\n31\n* 45\n------\nRemember: 45 = 40 + 5, and therefore, 31 * 45 = 31 * (40 + 5) = 31 * 40 + 31 * 5. Then, we calculate 31 * 5. 31 * 45\n31\n* 45\n------\n155\nNext, we calculate 31 * 40. It is just multiplying 31 by 4 and adding a 0 on the final result (31 * 40 = 31 * 4 * 10). 31 * 45\n31\n* 45\n------\n155\n1240\n\nFinally, we add up both partial results: 31 * 5 and 31 * 40, and we obtain 31 * 45.\n\n31\n* 45\n---------\n155\n+ 1240\n---------\n1395\n\nThat’s right, 31 * 45 = 1395. Now, you should practice these multiplications: 34 * 43, 74 * 49, 14 * 58, and 28 * 76.\n\n# Division. What is it? How does it work?\n\nImagine that we have fifteen yummy bones 15 and three hungry dogs .\n\nHow do we share these bones? Of course, we want to be fair, every dog should have the same amount of bones. What is the right answer?\n\nYou’ve guessed it! You should give five bones to each dog. Mathematically, we express it as 15 ÷ 3 = 5.\n\nDivision is sharing, splitting or grouping a number of things into equal parts or groups.\n\nBesides, there is another way of thinking about this problem. You have three dogs and you want to give them five bones each. How many bones do you need? That’s right! You need 3 * 5 = 15 bones. In other words, division is the inverse or reverse of multiplication.\n\n# Division II. Repeated subtraction. Remainder.\n\nOur original division 15 ÷ 5 = 3 can be reinterpreted as repeated subtraction. You can subtract (or you can jump backwards in the Number line) 3 from 15 five times!\n\nLet’s define some concepts now. The dividend is the number that is being divided (15). The divisor is the number dividing it (3). The quotient is the result, which is the number of times that the divisor is contained in the dividend (5).\n\nSometimes things are not so easy. Imagine a relatively similar problem. There are sixteen bones, just one more 16 and we have three hungry dogs .\n\nHow do we split them? The only fair solution is to give each dog five bones and there will still be one bone left. The remainder is what is left over after dividing numbers that do not divide exactly.\n\nIt is always the case that: Dividend = Divisor * Quotient + Remainder. In our example, 16 = 3 * 5 + 1.\n\n# Division III. 2- or 3-Digit Division\n\nLet’s see how divisions by two or three-digit numbers are done! Let’s calculate 525 ÷ 3.\n\n• First things first, we rewrite 525 ÷ 3 as:",
null,
"• We look at the first digit of the dividend (5): 5 ÷ 3 = 1 and the remainder equals 2. In other words, how many times will 3 go into 5? The answer is 1, so we put 1 right above the 5. 1*3 = 3, and we do the subtraction 5 - 3 = 2 to get the remainder.",
null,
"• Let’s move on to the second digit of the dividend (2). Take the elevator and drag it down. We divide the number that we obtained (22), by the divisor (3) and thus: 22 ÷ 3 = 7 and the remainder equals 1: 22 -21 (=3*7) = 1.",
null,
"• Let’s go to the last digit of the dividend (5). Take the elevator and bring it down again. By doing so, we get 15. We divide this number by the divisor: 15 ÷ 3 = 5 and there is no reminder, so we are done!",
null,
"Thus, 525 ÷ 3 = 175. We also calculate 276 ÷ 13 = 21 and remainder 3 and 976 ÷ 21 = 46 and remainder 10. Observe that 175 * 3 = 515, 13 * 21 + 3 = 276, and 46 * 21 + 10 = 976.\n\nBitcoin donation",
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""
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http://ffacs.top/?p=420 | [
"# Codeforces Round #655 (Div. 2)\n\n## A\n\n### 解法\n\n$1,1,3,3,5,5….$\n\n## 解法\n\n$\\text{LCM}(a,b)=\\frac{a(n-a)}{(a,n-a)}=\\frac{a(n-a)}{(a,n)}=x*(n-a)$ 其中 $(x,n)=1$ ,那么 $x$ 显然等于 $1$ 最佳。即 $a\\mid n$ , 所以 $a$ 显然取 $n$ 的最大因子,若为素数则 $a$ 显然取 $1,n-1$ (和为定值则两数相离越远乘积越小)。"
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http://www.ebooklibrary.org/articles/eng/Diophantine_equation | [
"",
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"This article will be permanently flagged as inappropriate and made unaccessible to everyone. Are you certain this article is inappropriate? Excessive Violence Sexual Content Political / Social Email this Article Email Address:\n\n# Diophantine equation\n\nArticle Id: WHEBN0000009109\nReproduction Date:\n\n Title: Diophantine equation",
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"Author: World Heritage Encyclopedia Language: English Subject: Collection: Diophantine Equations Publisher: World Heritage Encyclopedia Publication Date:\n\n### Diophantine equation\n\nIn mathematics, a Diophantine equation is a polynomial equation, usually in two or more unknowns, such that only the integer solutions are sought or studied (an integer solution is a solution such that all the unknowns take integer values). A linear Diophantine equation is an equation between two sums of monomials of degree zero or one. An exponential Diophantine equation is one in which exponents on terms can be unknowns.\n\nDiophantine problems have fewer equations than unknown variables and involve finding integers that work correctly for all equations. In more technical language, they define an algebraic curve, algebraic surface, or more general object, and ask about the lattice points on it.\n\nThe word Diophantine refers to the Hellenistic mathematician of the 3rd century, Diophantus of Alexandria, who made a study of such equations and was one of the first mathematicians to introduce symbolism into algebra. The mathematical study of Diophantine problems that Diophantus initiated is now called Diophantine analysis.\n\nWhile individual equations present a kind of puzzle and have been considered throughout history, the formulation of general theories of Diophantine equations (beyond the theory of quadratic forms) was an achievement of the twentieth century.\n\n## Contents\n\n• Examples 1\n• Linear Diophantine equations 2\n• One equation 2.1\n• Chinese remainder theorem 2.2\n• System of linear Diophantine equations 2.3\n• Diophantine analysis 3\n• Typical questions 3.1\n• Typical problem 3.2\n• 17th and 18th centuries 3.3\n• Hilbert's tenth problem 3.4\n• Diophantine geometry 3.5\n• Modern research 3.6\n• Infinite Diophantine equations 3.7\n• Exponential Diophantine equations 4\n• Notes 5\n• References 6\n\n## Examples\n\nIn the following Diophantine equations, w, x, y, and z are the unknowns and the other letters are given constants:\n ax+by=1\\, This is a linear Diophantine equation. w^3+x^3=y^3+z^3\\, The smallest nontrivial solution in positive integers is 12^3+1^3=9^3+10^3=1729. It was famously given as an evident property of 1729, a taxicab number (also named Hardy–Ramanujan number) by Ramanujan to Hardy while meeting in 1917. There are infinitely many nontrivial solutions. x^n+y^n=z^n \\, For n = 2 there are infinitely many solutions (x,y,z): the Pythagorean triples. For larger integer values of n, Fermat's Last Theorem (initially claimed in 1637 by Fermat and proved by Wiles in 1995) states there are no positive integer solutions (x, y, z). x^2-ny^2=\\pm 1\\, This is Pell's equation, which is named after the English mathematician John Pell. It was studied by Brahmagupta in the 7th century, as well as by Fermat in the 17th century. \\frac{4}{n} = \\frac{1}{x} + \\frac{1}{y} + \\frac{1}{z} The Erdős–Straus conjecture states that, for every positive integer n ≥ 2, there exists a solution in x, y, and z, all as positive integers. Although not usually stated in polynomial form, this example is equivalent to the polynomial equation 4xyz = yzn + xzn + xyn = n(yz + xz + xy). x^4 + y^4 + z^4 = w^4 Conjectured incorrectly by Euler to have no nontrivial solutions. Proved by Elkies to have infinitely many nontrivial solutions, with a computer search by Frye determining the smallest nontrivial solution.\n\n## Linear Diophantine equations\n\n### One equation\n\nThe simplest linear Diophantine equation takes the form ax + by = c, where a, b and c are given integers. The solutions are completely described by the following theorem: This Diophantine equation has a solution (where x and y are integers) if and only if c is a multiple of the greatest common divisor of a and b. Moreover, if (x, y) is a solution, then the other solutions have the form (x + kv, y - ku), where k is an arbitrary integer, and u and v are the quotients of a and b (respectively) by the greatest common divisor of a and b.\n\nProof: If d is this greatest common divisor, Bézout's identity asserts the existence of integers e and f such that ae + bf = d. If c is a multiple of d, then c = dh for some integer h, and (eh, fh) is a solution. On the other hand, for every pair of integers x and y, the greatest common divisor d of a and b divides ax + by. Thus, if the equation has a solution, then c must be a multiple of d. If a = ud and b = vd, then for every solution (x, y), we have\n\na(x+kv)+ b(y-ku) = ax+by + k(av -bu) =ax+by + k(udv -vdu) =ax + by,\n\nshowing that (x + kv, y - ku) is another solution. Finally, given two solutions such that ax1 + by1 = ax2 + by2 = c, one deduces that u (x2 - x1) + v (y2 - y1) = 0. As u and v are coprime, Euclid's lemma shows that there exists an integer k such that x2 - x1 = kv and y2 - y1 = -ku. Therefore x2 = x1 + kv and y2 = y1 - ku, which completes the proof.\n\n### Chinese remainder theorem\n\nThe Chinese remainder theorem describes an important class of linear Diophantine systems of equations: let n1, ..., nk be k pairwise coprime integers greater than one, a1, ..., ak be k arbitrary integers, and N be the product n1 ··· nk. The Chinese remainder theorem asserts that the following linear Diophantine system has exactly one solution (x, x1, ..., xk) such that 0 ≤ x < N, and that the other solutions are obtained by adding to x a multiple of N:\n\n\\begin{align} x&= a_1 + n_1\\,x_1\\\\ &\\vdots\\\\ x&=a_k+n_k\\,x_k \\end{align}\n\n### System of linear Diophantine equations\n\nMore generally, every system of linear Diophantine equations may be solved by computing the Smith normal form of its matrix, in a way that is similar to the use of the reduced row echelon form to solve a system of linear equations over a field. Using matrix notation every system of linear Diophantine equations may be written\n\nA\\,X=C,\n\nwhere A is an m×n matrix of integers, X is an n×1 column matrix of unknowns and C is an m×1 column matrix of integers.\n\nThe computation of the Smith normal form of A provides two unimodular matrices (that is matrices that are invertible over the integers and have ±1 as determinant) U and V of respective dimensions m×m and n×n, such that the matrix\n\nB=\\left[b_{i,j}\\right]=UAV\n\nis such that bi,i is not zero for i not greater than some integer k, and all the other entries are zero. The system to be solved may thus be rewritten as\n\nB\\,(V^{-1}X) = UC.\n\nCalling yi the entries of V^{-1}X and di those of D=UC, this leads to the system\n\nbi,i yi = di for 1 ≤ ik,\n0 yi = di for k < in.\n\nThis system is equivalent to the given one in the following sense: A column matrix of integers x is a solution of the given system if and only if x = V y for some column matrix of integers y such that By = D.\n\nIt follows that the system has a solution if and only if bi,i divides di for ik and di = 0 for i > k. If this condition is fulfilled, the solutions of the given system are\n\nV\\,\\left[ \\begin{array}{c} \\frac{d_1}{b_{1,1}}\\\\ \\vdots\\\\ \\frac{d_k}{b_{k,k}}\\\\ h_{k+1}\\\\ \\vdots\\\\ h_n \\end{array} \\right]\\,,\n\nwhere hk+1, ..., hn are arbitrary integers.\n\nHermite normal form may also be used for solving systems of linear Diophantine equations. However, Hermite normal form does not directly provide the solutions; to get the solutions from the Hermite normal form, one has to successively solve several linear equations. Nevertheless, Richard Zippel wrote that the Smith normal form \"is somewhat more than is actually needed to solve linear diophantine equations. Instead of reducing the equation to diagonal form, we only need to make it triangular, which is called the Hermite normal form. The Hermite normal form is substantially easier to compute than the Smith normal form.\"\n\nInteger linear programming amounts to finding some integer solutions (optimal in some sense) of linear systems that include also inequations. Thus systems of linear Diophantine equations are basic in this context, and textbooks on integer programming usually have a treatment of systems of linear Diophantine equations.\n\n## Diophantine analysis\n\n### Typical questions\n\nThe questions asked in Diophantine analysis include:\n\n1. Are there any solutions?\n2. Are there any solutions beyond some that are easily found by inspection?\n3. Are there finitely or infinitely many solutions?\n4. Can all solutions be found in theory?\n5. Can one in practice compute a full list of solutions?\n\nThese traditional problems often lay unsolved for centuries, and mathematicians gradually came to understand their depth (in some cases), rather than treat them as puzzles.\n\n### Typical problem\n\nThe given information is that a father's age is 1 less than twice that of his son, and that the digits AB making up the father's age are reversed in the son's age (i.e. BA). This leads to the equation 10A + B = 2 (10B + A) - 1, thus 19B - 8A = 1. Inspection gives the result A = 7, B = 3, and thus AB = 73 years and BA = 37 years. One may easily show that there is not any other solution with A and B positive integers less than 10.\n\n### 17th and 18th centuries\n\nIn 1637, Pierre de Fermat scribbled on the margin of his copy of Arithmetica: \"It is impossible to separate a cube into two cubes, or a fourth power into two fourth powers, or in general, any power higher than the second into two like powers.\" Stated in more modern language, \"The equation an + bn = cn has no solutions for any n higher than 2.\" And then he wrote, intriguingly: \"I have discovered a truly marvelous proof of this proposition, which this margin is too narrow to contain.\" Such a proof eluded mathematicians for centuries, however, and as such his statement became famous as Fermat's Last Theorem. It wasn't until 1995 that it was proven by the British mathematician Andrew Wiles.\n\nIn 1657, Fermat attempted to solve the Diophantine equation 61x2 + 1 = y2 (solved by Brahmagupta over 1000 years earlier). The equation was eventually solved by Euler in the early 18th century, who also solved a number of other Diophantine equations.The smallest solution of this equation in positive integers is x = 226153980, y = 1766319049 (see Chakravala method).\n\n### Hilbert's tenth problem\n\nIn 1900, in recognition of their depth, David Hilbert proposed the solvability of all Diophantine problems as the tenth of his celebrated problems. In 1970, a novel result in mathematical logic known as Matiyasevich's theorem settled the problem negatively: in general Diophantine problems are unsolvable.\n\n### Diophantine geometry\n\nDiophantine geometry, which is the application of techniques from algebraic geometry in this field, has continued to grow as a result; since treating arbitrary equations is a dead end, attention turns to equations that also have a geometric meaning. The central idea of Diophantine geometry is that of a rational point, namely a solution to a polynomial equation or a system of polynomial equations, which is a vector in a prescribed field K, when K is not algebraically closed.\n\n### Modern research\n\nOne of the few general approaches is through the Hasse principle. Infinite descent is the traditional method, and has been pushed a long way.\n\nThe depth of the study of general Diophantine equations is shown by the characterisation of Diophantine sets as equivalently described as recursively enumerable. In other words, the general problem of Diophantine analysis is blessed or cursed with universality, and in any case is not something that will be solved except by re-expressing it in other terms.\n\nThe field of Diophantine approximation deals with the cases of Diophantine inequalities. Here variables are still supposed to be integral, but some coefficients may be irrational numbers, and the equality sign is replaced by upper and lower bounds.\n\nThe most celebrated single question in the field, the conjecture known as Fermat's Last Theorem, was solved by Andrew Wiles but using tools from algebraic geometry developed during the last century rather than within number theory where the conjecture was originally formulated. Other major results, such as Faltings' theorem, have disposed of old conjectures.\n\n### Infinite Diophantine equations\n\nAn example of an infinite diophantine equation is:\n\nN = A^2+2B^2+3C^2+4D^2+5E^2+...,\n\nwhich can be expressed as \"How many ways can a given integer N be written as the sum of a square plus twice a square plus thrice a square and so on?\" The number of ways this can be done for each N forms an integer sequence. Infinite Diophantine equations are related to theta functions and infinite dimensional lattices. This equation always has a solution for any positive N. Compare this to:\n\nN = A^2+4B^2+9C^2+16D^2+25E^2+...,\n\nwhich does not always have a solution for positive N.\n\n## Exponential Diophantine equations\n\nIf a Diophantine equation has as an additional variable or variables occurring as exponents, it is an exponential Diophantine equation. Examples include the Ramanujan–Nagell equation, 2n − 7 = x2, and the equation of the Fermat-Catalan conjecture and Beal's conjecture, am + bn = ck with inequality restrictions on the exponents. A general theory for such equations is not available; particular cases such as Catalan's conjecture have been tackled. However, the majority are solved via ad hoc methods such as Størmer's theorem or even trial and error."
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https://algorithmsandme.com/merge-k-sorted-arrays/ | [
"## Merge k sorted arrays\n\nGiven k sorted arrays each having n elements, merge k sorted arrays into one n*k element array in sorted order. For example, given 3 arrays are as below\n\nResult array should be like\n\n## Merge k sorted arrays\n\nSince all the input arrays are sorted, the first element in result array will be among the first elements of input arrays. How can we find the minimum among all the elements plucked from the first index of each array ? Easy, take those k elements (there are k arrays, so k first elements) and build a min heap. The root of the min heap the least element among the first elements of all arrays, so it will be the first element in the result array.\n\nOnce, we add the first element into the result array, we have to find the second element. Second element can be from the set of first elements of all input arrays except one array from which the first element of result array was added. So, we will take second element of that array.\n\nIn order to know which array gave the minimum element at a particular time, we will store additional information of about array and index at which minimum element was.\n\nIf i represents the array number, and j represents the index of the minimum number in heap in ith array, then we add (j+1)th element to the min heap next and re-heapify. If j goes out of bound for ith array, we take min heap with k-1 size and go on, till we have no elements left in heap.\n\nFollow the procedure for `(n-1)*k` times. When all array elements are processed, result array will be in the sorted array.\n\n### Merge k sorted arrays: algorithm\n\n• Build min heap with the first element of all k arrays.\n• Pick the root of min element and put it in the result array.\n• If there are remaining elements in the array, put next element at the root of min heap and heapify again\n• If all elements are already of an array are processed, reduce the size of min heap by 1.\n• Repeat step 2, 3 and 4 till min heap is empty.\n\n#### Merge k sorted arrays: implementation\n\n```package com.company;\n\nimport java.util.PriorityQueue;\n\n/**\n* Created by sangar on 2.12.18.\n*/\npublic class MergeKSortedArrays {\nprivate class HeapNode{\npublic int arrayNum;\npublic int index;\npublic int value;\n\npublic HeapNode(int arrayNum, int index, int value){\nthis.arrayNum = arrayNum;\nthis.index = index;\nthis.value = value;\n}\n}\n\npublic int [] mergeKSortedArrays(int[][] arrays){\n\nif(arrays == null) return null;\n\nPriorityQueue<HeapNode> minHeap =\nnew PriorityQueue<>(arrays.length,\n(HeapNode a,HeapNode b)-> a.value - b.value);\n\nint size = 0;\nfor(int i =0; i<arrays.length; i++){\nsize += arrays[i].length;\n}\nint[] result = new int[size]; // k * n\n\n//add first elements in the array to this heap\nfor(int i=0; i<arrays.length; i++){\nminHeap.add(new HeapNode(i, 0, arrays[i]));\n}\n\n//Complexity O(n * k * log k)\nfor(int i=0; i< size; i++){\n//Take the minimum value and put into result\nHeapNode node = minHeap.poll();\n\nif(node != null){\nresult[i] = node.value;\nif(node.index + 1 < arrays[node.arrayNum].length) {\n//Complexity of O(log k)\nnode.index + 1,\narrays[node.arrayNum][node.index + 1]));\n}\n}\n}\nreturn result;\n}\n}\n```\n\n#### Test cases\n\n```package test;\n\nimport com.company.MergeKSortedArrays;\nimport org.junit.jupiter.api.Test;\n\nimport java.util.Arrays;\n\nimport static org.junit.jupiter.api.Assertions.assertEquals;\n\n/**\n* Created by sangar on 23.9.18.\n*/\npublic class MergeKSortedArraysTest {\n\nMergeKSortedArrays tester = new MergeKSortedArrays();\n\n@Test\npublic void mergeKSortedArraysTest() {\n\nint[][] input ={\n{ 1, 2, 3, 4 }, { 5, 6, 7, 8 }, { 9, 10, 11, 12 }\n};\n\nint[] expectedOutput = {1,2,3,4,5,6,7,8,9,10,11,12};\n\nint [] output = tester.mergeKSortedArrays(input);\n\nSystem.out.println(Arrays.toString(output));\nassertEquals(Arrays.toString(expectedOutput),\nArrays.toString(output));\n}\n\n@Test\npublic void mergeKSortedArraysWithUnequalSizeTest() {\n\nint[][] input ={\n{ 1, 2 }, { 5, 6, 7}, { 9, 10, 11, 12 }\n};\n\nint[] expectedOutput = {1,2,5,6,7,9,10,11,12};\n\nint [] output = tester.mergeKSortedArrays(input);\n\nSystem.out.println(Arrays.toString(output));\nassertEquals(Arrays.toString(expectedOutput),\nArrays.toString(output));\n}\n\n@Test\npublic void mergeKSortedArraysWithNullTest() {\n\nint [] output = tester.mergeKSortedArrays(null);\n\nassertEquals(null, output);\n}\n}\n\n```\n\nComplexity of code to merge k sorted arrays is O(n * k * log k) along with space complexity of O(k).\n\nPlease share if there is something wrong or missing. If you are preparing for an interview, please sign up to receive interview preparation kit for free."
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https://owenduffy.net/blog/?p=10598 | [
"# Estimating the voltage impressed on the tuning capacitor of a small transmitting loop\n\nThe ‘net abounds with calculators for design of small transmitting loops (STL), and most estimate the voltage impressed on the tuning capacitor. Most of these calculators give an incorrect estimate.\n\nThis article describes a measurement based approach to estimating the capacitor voltage for a STL.\n\n## Theory\n\nMost of the loss in a well implemented STL is in the main loop circuit, and that can be well approximated by a series equivalent circuit consisting of the loop's inductive reactance (Xl) in series with an equal capacitive reactance (Xc) and equivalent total series resistance Rs. The ratio Xl/Rs=Xc/Rs=Q.\n\nAnother representation is as a parallel equivalent circuit with the loop inductor, capacitor, and equivalent parallel resistance Rp all in parallel. The ratio Rp/Xl=Rp/Xc=Q.\n\nThe latter relationship gives a method for estimating voltage across Xc. Since P=Erms^2/R, we can find the voltage across Rp by Erms=(P*Rp)^0.5 and substituting for Rp, Erms=(P*Q*Xl)^0.5. Since Epk=2^0.5*Erms for a sine wave, we can write Epk=(2*P*Q*Xl)^0.5.\n\n## In practice\n\n1. Xl;\n2. find Q; and\n3. Calculate Epk at given power.\n\n### Find Xl\n\nWe can reliably calculate the inductance of a STL from a formula, or use direct measurement of the loop using a suitable antenna analyser or VNA. From that, Xl=2*pi*f*L.\n\nFor example, the inductance of a circular loop of 3.75m perimeter of 8mm diameter copper tube is 3.75µH, and at 4MHz Xl=94.3Ω.\n\n### Find Q\n\nMeasure the half power bandwidth of the completed and matched antenna.\n\nHere is an example measurement made of a STL using an AA-600 analyser",
null,
"Above is the VSWR plot from the AA-600. VSWR=2.6 bandwidth corresponds to the half power bandwidth of the loop itself. Measured bandwidth is 30kHz.\n\nCalculate Q=fc/BW=4000/30=133.3.\n\n### Calculate Epk at given power\n\nLets calculate Epk for 20W input power.\n\nEpk=(2*P*Q*Xl)^0.5=(2*20*133.3*94.3)^0.5=709Vpk.\n\nThis is the working voltage, you would choose a capacitor of somewhat higher rating.\n\nYou could use the actual capacitor breakdown rating less safety margin to find safe maximum power for the capacitor, so lets say you procured a 1800V capacitor and don't want to stress it beyond 1200V, rearranging the formula give earlier you can calculate Pmax=Epk^2/(2*Q*Xl)=1200^2/(2*133.3*94.3)=57W.\n\n## Reconciliation\n\nWe can learn from experiments that don't quite go to plan.\n\nDoes your loop implementation reconcile with the design tool you used?\n\nWhy?"
] | [
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"https://owenduffy.net/blog/wp-content/uploads/2014/05/Screenshot-28_05_2014-10_10_54-300x158.png",
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https://collegephysicsanswers.com/openstax-solutions/suppose-figure-2554-represents-ray-light-going-air-through-crown-glass-water | [
"Question\nSuppose Figure 25.54 represents a ray of light going from air through crown glass into water, such as going into a fish tank. Calculate the amount the ray is displaced by the glass ($\\Delta x$), given that the incident angle is $40.0^\\circ$ and the glass is 1.00 cm thick.\nQuestion Image",
null,
"Figure 25.54 A ray of light passes from one medium to a third by traveling through a second. The final direction is the same as if the second medium were not present, but the ray is displaced by delta x.\n$3.72 \\textrm{ mm}$\nSolution Video\n\n# OpenStax College Physics Solution, Chapter 25, Problem 15 (Problems & Exercises) (3:57)",
null,
"View sample solution\n\n## Calculator Screenshots",
null,
"",
null,
"Video Transcript\n\nThis is College Physics Answers with Shaun Dychko. A ray of light is travelling through air and then goes through a pane of glass around an aquarium and then enters some water. This glass is crown glass with an index of refraction of 1.52. Index refraction for air is 1.00 and that of water is 1.33, although it turns out that the water part is not going to matter. This <i>Delta X</i>, the amount of displacement of the ray as a result of going through this glass should actually be drawn here. We're going to draw it here. So, we're going to figure out what this distance is. Now, we can consider two different triangles. This triangle in yellow here represents this triangle here. And, a calculated distance <i>X one</i>. That's from here to where the ray would be, this is all here. This is where the ray would be if there had been no refraction. In other words, if there had been no crown glass here. And then, this triangle in blue represents what's actually happening with the presence of the glass and I've drawn, that's this drawing here. And so, the <i>Delta X</i> is displacement due to the refraction through the crown glass is going to be <i>X one</i> minus <i>X two</i>. Okay. So, let's figure out <i>X one</i> first, that's the easy part. We can say that the tangent of <i>theta one</i> equals the opposite <i>X one</i> divided by the adjacent, which is the thickness of the glass <i>D</i>, or as we're told is one centimeter. And so, that means <i>X one</i> is <i>D</i> times ten <i>theta one</i>. So, that's one centimeter times tangent of 40 degrees, because we're told that the angle of incidence is 40 degrees here, <i>theta one</i>. And, this works out to 0.8391 centimeters. Now, let's next consider what <i>X two</i> is. Well, it's going to have a different angle <i>theta two</i> and we'll use Snell's law to figure out what that <i>theta two</i> should be. And, for the same reason as this triangle, <i>X two</i> is the thickness of the glass multiplied by tangent of that angle <i>theta</i>, but in this case it's <i>theta two</i>. So, Snell's law says the index of refraction of the first medium, which is air, times sine <i>theta one</i>, which is 40 degrees, equals the index of refraction of the second medium, which is crown glass times sine of the angle of refraction, <i>theta two</i>. And so, we divide both sides by <i>N two</i> and we get sine <i>theta two</i> is <i>N one</i> sine <i>theta one</i> over <i>N two</i>. And, that gives us <i>theta two</i> is the inverse sine of all of this. So, that's the inverse sine of 1.00 times sine 40 divided by the index of refraction of crown glass, which is 1.52, giving an angle of 25.02 degrees. So, we plug that in for <i>theta two</i> in our formula for <i>X two</i>. And so, <i>X two</i> is one centimeter times tangent of 25.02 degrees, giving 0.4667 centimeters. And so, the <i>Delta X</i> then is the distance if there was no refraction, <i>X one</i>, 0.8391 centimeters, minus this distance that we have with refraction 0.4667 centimeters giving a total change of 0.372 centimeters, which we'll express in millimeters by multiplying by ten millimeters per centimeter. And so, it's going to be displaced 3.72 millimeters."
] | [
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"https://collegephysicsanswers.com/sites/default/files/styles/question_image/public/question/2018-10/Figure%2025.53.jpg",
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"https://video-thumbs.collegephysicsanswers.com/ed1/ch25/ed1ch25pe15/thumbs-ed1ch25pe15-00002.png",
null,
"https://collegephysicsanswers.com/system/files/styles/large/private/calculator_screenshot/ch25pe15-1.jpg",
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"https://collegephysicsanswers.com/system/files/styles/large/private/calculator_screenshot/ch25pe15-2.jpg",
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] | {"ft_lang_label":"__label__en","ft_lang_prob":0.92216074,"math_prob":0.98079145,"size":3398,"snap":"2020-24-2020-29","text_gpt3_token_len":959,"char_repetition_ratio":0.14466706,"word_repetition_ratio":0.025641026,"special_character_ratio":0.2798705,"punctuation_ratio":0.12303665,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9993892,"pos_list":[0,1,2,3,4,5,6,7,8],"im_url_duplicate_count":[null,2,null,2,null,2,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-07-15T04:47:51Z\",\"WARC-Record-ID\":\"<urn:uuid:f58cd4b5-1e1d-458a-af7d-568c16f0acab>\",\"Content-Length\":\"50720\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:c701726e-d6d0-420b-90e0-69e99c18e90d>\",\"WARC-Concurrent-To\":\"<urn:uuid:aa2a4321-0abe-442e-8349-94d0ad1f0e44>\",\"WARC-IP-Address\":\"34.226.46.235\",\"WARC-Target-URI\":\"https://collegephysicsanswers.com/openstax-solutions/suppose-figure-2554-represents-ray-light-going-air-through-crown-glass-water\",\"WARC-Payload-Digest\":\"sha1:57DSEVLDYB2QLZ6TMZRXFFQ5SUSAWNC5\",\"WARC-Block-Digest\":\"sha1:XSUHJCV4S46PQAIAC723RYQBWIASYNMG\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-29/CC-MAIN-2020-29_segments_1593657155816.86_warc_CC-MAIN-20200715035109-20200715065109-00375.warc.gz\"}"} |
https://es.tradingview.com/script/futPZepe/ | [
"",
null,
"█ 888 BOT #backtest (open source)\n\nThis is an Expert Advisor 'EA' or Automated trading script for ‘longs’ and ‘shorts’, which uses only a Take Profit or, in the worst case, a Stop Loss to close the trade.\nIt's a much improved version of the previous ‘Repanocha’. It doesn`t use 'Trailing Stop' or 'security()' functions (although using a security function doesn`t mean that the script repaints) and all signals are confirmed, therefore the script doesn`t repaint in alert mode and is accurate in backtest mode.\nApart from the previous indicators, some more and other functions have been added for Stop-Loss, re-entry and leverage.\nIt uses 8 indicators, (many of you already know what they are, but in case there is someone new), these are the following:\n\n1. Jurik Moving Average\nIt's a moving average created by Mark Jurik for professionals which eliminates the 'lag' or delay of the signal. It's better than other moving averages like EMA , DEMA , AMA or T3.\nThere are two ways to decrease noise using JMA . Increasing the 'LENGTH' parameter will cause JMA to move more slowly and therefore reduce noise at the expense of adding 'lag'\nThe 'JMA LENGTH', 'PHASE' and 'POWER' parameters offer a way to select the optimal balance between 'lag' and over boost.\nGreen: Bullish , Red: Bearish .\n\n2. Range filter\nCreated by Donovan Wall, its function is to filter or eliminate noise and to better determine the price trend in the short term.\nFirst, a uniform average price range 'SAMPLING PERIOD' is calculated for the filter base and multiplied by a specific quantity 'RANGE MULTIPLIER'.\nThe filter is then calculated by adjusting price movements that do not exceed the specified range.\nFinally, the target ranges are plotted to show the prices that will trigger the filter movement.\nGreen: Bullish , Red: Bearish .\n\nIt's an indicator designed by Welles Wilder to measure the strength and direction of the market trend. The price movement is strong when the ADX has a positive slope and is above a certain minimum level 'ADX THRESHOLD' and for a given period 'ADX LENGTH'.\nThe green color of the bars indicates that the trend is bullish and that the ADX is above the level established by the threshold.\nThe red color of the bars indicates that the trend is down and that the ADX is above the threshold level.\nThe orange color of the bars indicates that the price is not strong and will surely lateralize.\nYou can choose between the classic option and the one created by a certain 'Masanakamura'. The main difference between the two is that in the first it uses RMA () and in the second SMA () in its calculation.\n\n4. Parabolic SAR\nThis indicator, also created by Welles Wilder, places points that help define a trend. The Parabolic SAR can follow the price above or below, the peculiarity that it offers is that when the price touches the indicator, it jumps to the other side of the price (if the Parabolic SAR was below the price it jumps up and vice versa) to a distance predetermined by the indicator. At this time the indicator continues to follow the price, reducing the distance with each candle until it is finally touched again by the price and the process starts again. This procedure explains the name of the indicator: the Parabolic SAR follows the price generating a characteristic parabolic shape, when the price touches it, stops and turns ( SAR is the acronym for 'stop and reverse'), giving rise to a new cycle. When the points are below the price, the trend is up, while the points above the price indicate a downward trend.\n\n5. RSI with Volume\nThis indicator was created by LazyBear from the popular RSI .\nThe RSI is an oscillator-type indicator used in technical analysis and also created by Welles Wilder that shows the strength of the price by comparing individual movements up or down in successive closing prices.\nLazyBear added a volume parameter that makes it more accurate to the market movement.\nA good way to use RSI is by considering the 50 'RSI CENTER LINE' centerline. When the oscillator is above, the trend is bullish and when it is below, the trend is bearish .\n\n6. Moving Average Convergence Divergence ( MACD ) and ( MAC-Z )\nIt was created by Gerald Appel. Subsequently, the histogram was added to anticipate the crossing of MA. Broadly speaking, we can say that the MACD is an oscillator consisting of two moving averages that rotate around the zero line. The MACD line is the difference between a short moving average 'MACD FAST MA LENGTH' and a long moving average 'MACD SLOW MA LENGTH'. It's an indicator that allows us to have a reference on the trend of the asset on which it is operating, thus generating market entry and exit signals.\nWe can talk about a bull market when the MACD histogram is above the zero line, along with the signal line, while we are talking about a bear market when the MACD histogram is below the zero line.\nThere is the option of using the MAC-Z indicator created by LazyBear, which according to its author is more effective, by using the parameter VWAP ( volume weighted average price ) 'Z-VWAP LENGTH' together with a standard deviation 'STDEV LENGTH' in its calculation.\n\n7. Volume Condition\nVolume indicates the number of participants in this war between bulls and bears, the more volume the more likely the price will move in favor of the trend. A low trading volume indicates a lower number of participants and interest in the instrument in question. Low volumes may reveal weakness behind a price movement.\nWith this condition, those signals whose volume is less than the volume SMA for a period 'SMA VOLUME LENGTH' multiplied by a factor 'VOLUME FACTOR' are filtered. In addition, it determines the leverage used, the more volume , the more participants, the more probability that the price will move in our favor, that is, we can use more leverage. The leverage in this script is determined by how many times the volume is above the SMA line.\nThe maximum leverage is 8.\n\n8. Bollinger Bands\nThis indicator was created by John Bollinger and consists of three bands that are drawn superimposed on the price evolution graph.\nThe central band is a moving average, normally a simple moving average calculated with 20 periods is used. ('BB LENGTH' Number of periods of the moving average)\nThe upper band is calculated by adding the value of the simple moving average X times the standard deviation of the moving average. ('BB MULTIPLIER' Number of times the standard deviation of the moving average)\nThe lower band is calculated by subtracting the simple moving average X times the standard deviation of the moving average.\nthe band between the upper and lower bands contains, statistically, almost 90% of the possible price variations, which means that any movement of the price outside the bands has special relevance.\nIn practical terms, Bollinger bands behave as if they were an elastic band so that, if the price touches them, it has a high probability of bouncing.\nSometimes, after the entry order is filled, the price is returned to the opposite side. If price touch the Bollinger band in the same previous conditions, another order is filled in the same direction of the position to improve the average entry price, (% MINIMUM BETTER PRICE ': Minimum price for the re-entry to be executed and that is better than the price of the previous position in a given %) in this way we give the trade a chance that the Take Profit is executed before. The downside is that the position is doubled in size. 'ACTIVATE DIVIDE TP': Divide the size of the TP in half. More probability of the trade closing but less profit.\n\n█ STOP LOSS and RISK MANAGEMENT.\nA good risk management is what can make your equity go up or be liquidated.\nThe % risk is the percentage of our capital that we are willing to lose by operation. This is recommended to be between 1-5%.\n\n% Risk: (% Stop Loss x % Equity per trade x Leverage) / 100\nFirst the strategy is calculated with Stop Loss, then the risk per operation is determined and from there, the amount per operation is calculated and not vice versa.\nIn this script you can use a normal Stop Loss or one according to the ATR. Also activate the option to trigger it earlier if the risk percentage is reached. '% RISK ALLOWED'\n'STOP LOSS CONFIRMED': The Stop Loss is only activated if the closing of the previous bar is in the loss limit condition. It's useful to prevent the SL from triggering when they do a ‘pump’ to sweep Stops and then return the price to the previous state.\n\n█ BACKTEST\nThe objective of the Backtest is to evaluate the effectiveness of our strategy. A good Backtest is determined by some parameters such as:\n\n- RECOVERY FACTOR: It consists of dividing the 'net profit' by the 'drawdown’. An excellent trading system has a recovery factor of 10 or more; that is, it generates 10 times more net profit than drawdown.\n\n- PROFIT FACTOR: The ‘Profit Factor’ is another popular measure of system performance. It's as simple as dividing what win trades earn by what loser trades lose. If the strategy is profitable then by definition the 'Profit Factor' is going to be greater than 1. Strategies that are not profitable produce profit factors less than one. A good system has a profit factor of 2 or more. The good thing about the ‘Profit Factor’ is that it tells us what we are going to earn for each dollar we lose. A profit factor of 2.5 tells us that for every dollar we lose operating we will earn 2.5.\n\n- SHARPE: (Return system - Return without risk) / Deviation of returns.\nWhen the variations of gains and losses are very high, the deviation is very high and that leads to a very poor ‘Sharpe’ ratio. If the operations are very close to the average (little deviation) the result is a fairly high 'Sharpe' ratio. If a strategy has a 'Sharpe' ratio greater than 1 it is a good strategy. If it has a 'Sharpe' ratio greater than 2, it is excellent. If it has a ‘Sharpe’ ratio less than 1 then we don't know if it is good or bad, we have to look at other parameters.\n\n- MATHEMATICAL EXPECTATION: (% winning trades X average profit) + (% losing trades X average loss).\nTo earn money with a Trading system, it is not necessary to win all the operations, what is really important is the final result of the operation. A Trading system has to have positive mathematical expectation as is the case with this script: ME = (0.87 x 30.74\\$) - (0.13 x 56.16\\$) = (26.74 - 7.30) = 19.44\\$ > 0\nThe game of roulette, for example, has negative mathematical expectation for the player, it can have positive winning streaks, but in the long term, if you continue playing you will end up losing, and casinos know this very well.\n\nPARAMETERS\n\n'BACKTEST DAYS': Number of days back of historical data for the calculation of the Backtest.\n'ENTRY TYPE': For '% EQUITY' if you have \\$ 10,000 of capital and select 7.5%, for example, your entry would be \\$ 750 without leverage. If you select CONTRACTS for the 'BTCUSDT' pair, for example, it would be the amount in 'Bitcoins' and if you select 'CASH' it would be the amount in \\$ dollars.\n'QUANTITY (LEVERAGE 1X)': The amount for an entry with X1 leverage according to the previous section.\n'MAXIMUM LEVERAGE': It's the maximum allowed multiplier of the quantity entered in the previous section according to the volume condition.\n\nThe settings are for Bitcoin at Binance Futures (BTC: USDTPERP ) in 15 minutes.\nFor other pairs and other timeframes, the settings have to be adjusted again. And within a month, the settings will be different because we all know the market and the trend are changing.\nScript de código abierto\n\nSiguiendo el verdadero espíritu de TradingView, el autor de este script lo ha publicado en código abierto, para que los traders puedan entenderlo y verificarlo. ¡Un hurra por el autor! Puede utilizarlo de forma gratuita, aunque si vuelve a utilizar este código en una publicación, debe cumplir con lo establecido en las Normas internas. Puede añadir este script a sus favoritos y usarlo en un gráfico."
] | [
null,
"https://es.tradingview.com/i/futPZepe/",
null
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https://nexen.partners.phpclasses.org/browse/file/65076.html | [
"",
null,
"# File: Regex.class.php",
null,
"Download\n ``` [ 'a', 1, 2, 'x' ] * => [ 'b', 1, 2, 'x' ] * => [ 'a', 1, 2, 'y' ] * => [ 'b', 1, 2, 'y' ] * => [ 'a', 1, 2, 'z' ] * => [ 'b', 1, 2, 'z' ] * ] * * Note that the combination generation is computed from left to right. * * @param array \\$array * Input array; * * @param int \\$max_results * This parameter is provided to limit exponential combinations generation. * * @return array * Returns an array of arrays containing all the combinations of the supplied input array. */ // __develop_non_recursive - // A non-recursive version for the CombinationsOf() method, that allows only one nesting level of arrays. private static function __develop_non_recursive ( &\\$results, \\$array, \\$max_results = 10000 ) { \\$array_count = count ( \\$array ) ; // Loop through input array, which is processed from right to left to generate the resulting array for ( \\$i = \\$array_count - 1 ; \\$i >= 0 ; \\$i -- ) { \\$item = \\$array [\\$i] ; \\$result_count = count ( \\$results ) ; // Current item is a nested array : we will have to demultiplicate each result in the \\$results array // to hold each \\$array items if ( is_array ( \\$item ) ) { \\$item_count = count ( \\$item ) ; // Check for possible quota overflow if ( \\$result_count * \\$item_count > \\$max_results ) throw ( new Exception ( \"Array development limit of \\$max_results results exceeded.\" ) ) ; // Then check that each subitem of this array is not an array in itself foreach ( \\$item as \\$subitem ) { if ( is_array ( \\$subitem ) ) throw ( new Exception ( \"No more than one nesting level is allowed in arrays to be developed.\" ) ) ; } // Demultiplicate existing results if ( \\$result_count ) { \\$new_results = [] ; for ( \\$j = 0 ; \\$j < \\$result_count ; \\$j ++ ) { for ( \\$k = 0 ; \\$k < \\$item_count ; \\$k ++ ) { \\$subitem = \\$item [\\$k] ; \\$new_results [] = array_merge ( [ \\$subitem ], \\$results [\\$j] ) ; } } \\$results = \\$new_results ; } // ... but for the first iteration, only add the elements of the current array item else { foreach ( \\$item as \\$subitem ) \\$results [] = [ \\$subitem ] ; } } // Current item is not an array else { // Prepend it to the existing items if ( \\$result_count ) { foreach ( \\$results as &\\$result ) array_unshift ( \\$result, \\$item ) ; } // ... or simply add it, if the results array is empty else { \\$results [] = [ \\$item ] ; } } } } public static function CombinationsOf ( \\$array, \\$max_results = 10000 ) { \\$array_count = count ( \\$array ) ; if ( ! \\$array_count ) return ( [] ) ; \\$results = [] ; self::__develop_non_recursive ( \\$results, \\$array, \\$max_results ) ; return ( \\$results ) ; } /** * * Expands a factorized expression. * * Expands (develops) a factorized string expression. * Sometimes, it is necessary to represent a set of values with a factorized expression, * such as the shell allows us to match a set of files using a pattern. * The DevelopExpression() method allows for input strings that can contain \"character * classes\" such as : * * [a-c].somestring * * which will expand to the following array of values : * * a.somestring * b.somestring * c.somestring * * Character classes can be either alphabetic or alphanumeric, such as in the following * example : * * [a-b][0-1].somestring * * which will expand to : * * a0.somestring * a1.somestring * b0.somestring * b1.somestring * * Numeric values can be zero-padded, using an optional width construct, like in the * following example : * * [a-b][0-1]/4.somestring * * which will expand to : * * a0000.somestring * a0001.somestring * b0000.somestring * b0001.somestring * * For alphabetic character classes, the case of the first character determines the case * of the expanded result ; for example : * * [A-c].somestring * * will give : * * A.somestring * B.somestring * C.somestring * * Finally, brackets can be escaped using the backslash character. * * * @param string \\$expression * Expression to be developed. * * @param int \\$limit * Maximum number of developed expressions to be returned. This limit is arbitrarily fixed to 10000. * When null or negative, no limit is applied. * * @return array * Returns an array containing the developed expression results. The returned value always contain * at least one element (the supplied input value) when no factorization expression are found. * * @todo * . Allow for real character classes, such as : * [A] (same as [A-A]) * [A-] (same as [A-Z]) * [-Z] (same as [A-Z]) * [abc012] (low/high will cycle through the characters \"abc012\") * */ public static function DevelopExpression ( \\$expression, \\$limit = 10000 ) { // Regular expression that matches : // . Either an escaped bracket // . Or a factorization expression static \\$re = '# (?P \\\\\\\\ [\\[\\]] ) | (?P \\[ (?P ( [a-z] | [0-9]+ ) ) - (?P ( [a-z] | [0-9]+ ) ) \\] ( \\/ (?P \\d+) )? ) #imsx' ; // First simplication case : the input string contain no factorization expression, return // it as is if ( ! self::PregMatchAll ( \\$re, \\$expression, \\$matches, PREG_OFFSET_CAPTURE ) ) return ( [ \\$expression ] ) ; // Second elimination case : the input string does not contain any factorization expression, // but escaped brackets are present (thus generating a \"match\") \\$found_range = false ; foreach ( \\$matches [ 'range' ] as \\$match ) { if ( \\$match ) { \\$found_range = true ; break ; } } if ( ! \\$found_range ) return ( [ \\$expression ] ) ; // Initializations \\$results = [] ; // The results that will be returned \\$result_count = 0 ; // Number of generated results - checked against the \\$limit parameter \\$ranges = [] ; // Associative arrays that describe each input string portion, either plain constant or factorization expression \\$range_indexes = [] ; // Indexes into \\$ranges of the entries containing a factorization expression \\$expression_length = strlen ( \\$expression ) ; // Compute it once and for all /*** Loop through the matches found ; upon exit, the \\$ranges array will contain associative arrays with the following keys : - 'expression' (boolean) : True if the entry is a factorization expression, false otherwise. - 'offset' (integer) : Start character. - 'length' (integer) : Length of the expression or plain substring. - 'capture' (string) : Original string (either the plain substring or the factorization expression). For factorization expressions, the following keys are also present : - 'low' (integer) : Low value of the factorization expression. - 'high' (integer) : High value of the factorization expression. - 'numeric' (boolean) : True if the factorization expression relates to numeric values, false for alphabetic values. - 'width' (boolean) : False for alphabetic values. For numeric values, specifies the zero-pad width. - 'current' (integer or string) : Current index in the generation loop. Initialized to the value of the 'low' entry. ***/ // If first match does not start at string offset zero, create a plain string entry in the \\$ranges array if ( \\$matches [ 'range' ] != 0 ) \\$ranges [] = [ 'expression' => false, 'offset' => 0, 'length' => \\$matches [ 'range' ] , 'capture' => substr ( \\$expression, 0, \\$matches [ 'range' ] ) ] ; // Loop through the matches for ( \\$i = 0 ; \\$i < count ( \\$matches [ 'range' ] ) ; \\$i ++ ) { // \\$matches [ 'range' ] [\\$i] will never be an array if an escaped bracket is met if ( ! \\$matches [ 'range' ] [\\$i] ) continue ; // Create the range entry \\$range = [ 'expression' => true, 'low' => \\$matches [ 'rangelo' ] [\\$i] , 'high' => \\$matches [ 'rangehi' ] [\\$i] , 'offset' => \\$matches [ 'range' ] [\\$i] , 'current' => \\$matches [ 'rangelo' ] [\\$i] , 'length' => strlen ( \\$matches [ 'range' ] [\\$i] ), 'capture' => \\$matches [ 'range' ] [\\$i] , 'width' => ( \\$matches [ 'width' ] [\\$i] ) ? \\$matches [ 'width' ] [\\$i] : false ] ; // If low value is alphabetic... if ( ctype_alpha ( \\$range [ 'low' ] ) ) { // ... and if high value is also alphabetic if ( ctype_alpha ( \\$range [ 'high' ] ) ) { // ... the case of the factorized expressions will be the case of the 'low' value if ( ctype_lower ( \\$range [ 'low' ] ) ) \\$range [ 'high' ] = strtolower ( \\$range [ 'high' ] ) ; else \\$range [ 'high' ] = strtoupper ( \\$range [ 'high' ] ) ; } // ... but complain if out of alphabetic range else throw ( new Exception ( \"Invalid combination of letters and numbers in factorized expression : \" . \\$matches [ 'range' ] [\\$i] ) ) ; \\$range [ 'numeric' ] = false ; // This entry is alphabetic } // Low value is not alphabetic : due to the regex construct, this must be an integer, so check that the high // value is also an integer else if ( ! is_numeric ( \\$range [ 'high' ] ) ) throw ( new Exception ( \"Invalid combination of letters and numbers in factorized expression : \" . \\$matches [ 'range' ] [\\$i] ) ) ; // Both low and high values are numeric else \\$range [ 'numeric' ] = true ; // Check that low range is not greater than upper range if ( \\$range [ 'numeric' ] ) { if ( ( integer ) \\$range [ 'low' ] > ( integer ) \\$range [ 'high' ] ) throw ( new Exception ( \"Lower numeric value cannot be greater than upper value in factorized expression : \" . \\$matches [ 'range' ] [\\$i] ) ) ; } else if ( \\$range [ 'low' ] > \\$range [ 'high' ] ) throw ( new Exception ( \"Lower alphabetic value cannot be greater than upper value in factorized expression : \" . \\$matches [ 'range' ] [\\$i] ) ) ; // If there is a plain string between the previous range and this one, then we need to add // a plain string entry before it \\$count = count ( \\$ranges ) ; if ( \\$count ) // ... but only if we already have found ranges { \\$previous_range = \\$ranges [ \\$count - 1 ] ; \\$last_found = \\$previous_range [ 'offset' ] + \\$previous_range [ 'length' ] ; if ( \\$last_found < \\$range [ 'offset' ] ) { \\$ranges [] = [ 'expression' => false, 'offset' => \\$last_found, 'length' => \\$range [ 'offset' ] - \\$last_found, 'capture' => substr ( \\$expression, \\$last_found, \\$range [ 'offset' ] - \\$last_found ) ] ; } } // Since the \\$ranges array contains both plain strings and factorization expressions, we need an array // to store factorization expression indexes, in order to simplify the generation process \\$range_indexes [] = count ( \\$ranges ) ; // Add this factorization expression to the list \\$ranges [] = \\$range ; } // If the string does not end with a factorization expression, then we have to add this plain string to // the \\$ranges array \\$count = count ( \\$ranges ) ; if ( \\$count ) { \\$previous_range = \\$ranges [ \\$count - 1 ] ; \\$last_found = \\$previous_range [ 'offset' ] + \\$previous_range [ 'length' ] ; if ( \\$last_found < \\$expression_length ) { \\$ranges [] = [ 'expression' => false, 'offset' => \\$last_found, 'length' => \\$expression_length - \\$last_found, 'capture' => substr ( \\$expression, \\$last_found, \\$expression_length - \\$last_found ) ] ; } } // After all this preparatory stuff, we are finally ready to generate the developed values ! \\$range_index_count = count ( \\$range_indexes ) ; while ( true ) { \\$current = \"\" ; // Generate the current developed value foreach ( \\$ranges as \\$range ) { if ( \\$range [ 'expression' ] ) { if ( \\$range [ 'width' ] ) \\$current .= sprintf ( \"%0{\\$range [ 'width' ]}d\", \\$range [ 'current' ] ) ; else \\$current .= \\$range [ 'current' ] ; } else \\$current .= \\$range [ 'capture' ] ; } \\$results [] = \\$current ; \\$result_count ++ ; // Stop if we reached the limit (if any...) if ( \\$limit > 0 && \\$result_count == \\$limit ) break ; // This loop finds the next increment value, when multiple factorization expressions are specified for ( \\$i = \\$range_index_count - 1 ; \\$i >= 0 ; \\$i -- ) { // Look only the entries in the \\$range array that are factorization expressions, starting // with the very last one \\$range_index = \\$range_indexes [\\$i] ; \\$current_range = &\\$ranges [ \\$range_index ] ; // Increment the value if ( \\$current_range [ 'numeric' ] ) \\$current_range [ 'current' ] = \\$current_range [ 'current' ] + 1 ; else \\$current_range [ 'current' ] = chr ( ord ( \\$current_range [ 'current' ] ) + 1 ) ; // When the current (last) value reaches the high-end of the range... if ( \\$current_range [ 'current' ] > \\$current_range [ 'high' ] ) { // Just start again with the low-end value if ( \\$i ) \\$current_range [ 'current' ] = \\$current_range [ 'low' ] ; // ... but only if there are still values to be incremented else break 2 ; } // Current value is still within the [low..high] range else break ; } } // All done, return return ( \\$results ) ; } /** * Allows a regex match result to have captures with the same name. * * After the result of calling a preg_* function, takes the resulting matches and groups * them using the specified replacement associative array. * The \\$replacement array comes from a possible call to Regex::RenumberNamedCaptures() * method ; each key defines the renumbered capture names, whereas each value is the * original name. * There is a 1 -> n relationship between the new and old names, allowing a single * regular expression to contain more than one capture having the same name. * * @param mixed \\$match * A match result, as can be returned by the self::PregMatch*() functions. * * @param array \\$replacements * An associative array returned by the Regex::RenumberNamedCaptures() method, * having the following shape : * - key : New capture name * - value : old capture name * * @return array */ public static function GroupNamedCaptures ( \\$match, \\$replacements ) { \\$new_match = [] ; foreach ( \\$match as \\$key => \\$value ) { // If the key corresponds to one of the matched replacements, group it into an array if ( isset ( \\$replacements [ \\$key ] ) ) { if ( isset ( \\$new_match [ \\$replacements [ \\$key ] ] ) ) \\$new_match [ \\$replacements [ \\$key ] ] [] = \\$value ; else \\$new_match [ \\$replacements [ \\$key ] ] = [ \\$value ] ; } else { if ( isset ( \\$new_match [ \\$key ] ) ) \\$new_match [ \\$key ] [] = \\$value ; else \\$new_match [ \\$key ] = [ \\$value ] ; } } return ( \\$new_match ) ; } /** * * Checks if the specified string is a valid regular expression. * * @param string \\$str * String to be checked. * * @param string \\$delimiter * Regular expression delimiter. If not specified, the delimiter is taken from * the first character of the specified input string. * * @return bool * Returns true if the specified string represents a regular expression, false otherwise. */ public static function IsRegex ( \\$str, \\$delimiter = false ) { static \\$pcre_options = 'imsxe' ; \\$length = strlen ( \\$str ) ; // Basic re's must have at least 3 characters : 2 delimiters and a character inside if ( \\$length < 3 ) return ( false ) ; // Check that the starting character is not an alphanumeric, backslash or whitespace character if ( \\$str == '\\\\' || ctype_alnum ( \\$str ) || ctype_space ( \\$str ) ) return ( false ) ; // If a delimiter has been specified, check that the supplied string starts with it if ( \\$delimiter !== false ) { if ( \\$str != \\$delimiter ) return ( false ) ; } // Otherwise, the delimiter will be the first character of the string else \\$delimiter = \\$str ; // Handle asymetric delimiters switch ( \\$delimiter ) { case '<' : \\$end_delimiter = '>' ; break ; case '{' : \\$end_delimiter = '}' ; break ; case '[' : \\$end_delimiter = ']' ; break ; case '(' : \\$end_delimiter = ')' ; break ; default : \\$end_delimiter = \\$delimiter ; } // Find the trailing delimiter from the end of the string for ( \\$i = \\$length - 1 ; \\$i > 0 ; \\$i -- ) { \\$ch = \\$str [\\$i] ; // Delimiter found : we can safely say this is a regex if ( \\$ch == \\$end_delimiter ) { // ... but only if the previous character is not an escape character if ( \\$i > 0 && \\$str [ \\$i - 1 ] == '\\\\' ) return ( false ) ; return ( true ) ; } // But if we find a non-pcre option after the trailing delimiter, then this definitely is not a regex else if ( stripos ( \\$pcre_options, \\$ch ) === false ) return ( false ) ; } // No trailing delimiter found return ( false ) ; } /** * * Checks if a filename corresponds to a filemask. * * @param string \\$file * Filename to be checked. * * @param string \\$pattern * Wildcard pattern. See the Regex::WildcardToRegex() method for an explanation on wildcard expressions syntax. * * @param bool \\$case_sensitive * When true, comparisons are case-sensitive. * * @return bool|int * Returns true if \\$pattern matches \\$file, false otherwise. * */ public static function Matches ( \\$file, \\$pattern, \\$case_sensitive = false ) { \\$length = strlen ( \\$pattern ) ; \\$newpattern = \"\" ; for ( \\$i = 0 ; \\$i < \\$length ; \\$i ++ ) { \\$char = \\$pattern [ \\$i ] ; \\$depth = 0 ; switch ( \\$char ) { case '/' : case '\\\\' : \\$newpattern .= '[\\\\/\\\\\\\\]' ; break ; case '.' : case '+' : case '^' : case '\\$' : case '(' : case ')' : case '|' : case '{' : case '}' : case '=' : case '!' : case '<' : case '>' : case '/' : \\$newpattern .= '\\\\' . \\$char ; break ; case '?' : case '*' : \\$newpattern .= '[^\\\\/\\\\\\\\]' . \\$char ; break ; case '[' : \\$newpattern .= '[' ; \\$depth ++ ; break ; case ']' : if ( ! \\$depth ) return ( false ) ; \\$newpattern .= ']' ; break ; default : \\$newpattern .= \\$char ; } } if ( \\$case_sensitive ) \\$extra = '' ; else \\$extra = 'i' ; \\$status = preg_match ( '/^' . \\$newpattern . '\\$/' . \\$extra, \\$file ) ; return ( ( \\$status ) ? true : false ) ; } /** * A meta-matching artefact for regular expressions. * * Suppose you have to scan a sequence of lines, such as in a log file. You want to * recognize which sequence follows which pattern. * * A sequence in an example log file could be, for example : * - A line containing \"message start\" * - Any number of lines starting with \"log:\" and followed by any sequence of characters * - A line containing \"message end\" * * The following example gives a layout of such a log file : * * message start * log: message 1 * log: message 2 * ... * log: message n * message end * * The purpose is to check whether a sequence of lines would match this scheme ; a set * of regular expressions would be first needeed to match every particular line in a sequence : * * \\$regex_list = * [ * '1' => '/message start/', * '2' => 'log: \\s* (?P .*), * '3' => '/message end/' * ] ; * * Then, to match a set of lines containing 'message start', having an unlimited number * of lines starting with 'log:', then ending with a line containing 'message end', you * would have to provide a regular expression using a backreference-style syntax * referencing the keys of our \\$regex_list array, which would give : * * \\$sequence = '\\1 \\2* \\3' ; * * meaning : * - The first line must be the one identified by '\\1', ie 'message start' * - There can be any number of lines identified by '\\2', ie starting with 'log:' * - The last line must be 'message end' * * Note that each \\$regex_list item is a regular expression which can contain group * captures, either named or not. * If it does not contain re delimiters, then '/ /imsx' is assumed, so do not forget that * spaces will not be significant. * * Thus, checking if a set of lines (in an array) matches the regular expressions * specified in \\$sequence and defined in \\$regex_list, a simple call will be enough : * * \\$status = Regex::MetaPregMatchEx ( \\$sequence, \\$regex_list, \\$lines ) ; * * @param string \\$sequence * A regular expression containing preg backreference-style constructs that * refer to array keys in the \\$regex_list array. * * The following preg-style backreferences are supported ('x' stands for a * sequence of digits, 'name' for a group capture name) : * - \\x * - \\gx * - \\g{x} * - (?P=name) * - \\k * - \\k'name' * - \\k{name} * - \\g{name} * * @param array \\$regex_list * An associative array whose keys are backreference ids (either the 'x' or the * 'name' string described in the \\$sequence parameter help) and whose values * are regular expressions. * Each entry is meant to match one or more lines of a sequence of lines. * * If no delimiter encloses the regex, then a default delimiter '/' will be used, * and the 'imsx' preg options will be automatically added before performing the * match. * * * @param array \\$subject_array * Array of input lines to be matched against the specified sequence. * * @param array \\$matches * Reference to an array which will receive the individual matches. * Each entry is an associative array having the following keys : * - 'reference' : * The original string reference. * - 'regex' : * The regex that matched the line. * - 'matches' : * Array of matches. Note that since the method uses PregMatchEx(), * an additional level of indirection is added with regards to self::PregMatch, * since several captures can have the same name. * * @param int \\$flags * PREG_* Flags for the self::PregMatch*() function. * * @param array \\$missing_matches * When specified, the indexes of non-matching lines will be stored in this array. * * @return bool * Returns true if the sequence of lines matches the specified sequence, false otherwise. */ public static function MetaPregMatchEx ( \\$sequence, \\$regex_list, \\$subject_array, &\\$matches = null, \\$flags = 0, \\$match_all = false, \\$missing_matches = [] ) { \\$match_list = [] ; // List of matched results in \\$subject_array \\$match_references = [] ; // List of corresponding match references (keys in regex_list array) // Normalize the sequence \\$new_sequence = self::NormalizeMetaSequence ( \\$sequence ) ; \\$subject_index = 0 ; // Loop through each log line foreach ( \\$subject_array as \\$subject ) { \\$found = false ; // Compare with each item in regex list \\$regex_index = 0 ; foreach ( \\$regex_list as \\$regex_key => \\$regex_value ) { // Normalize regular expression if ( ! self::IsRegex ( \\$regex_value ) ) \\$regex_value = '/^ \\s* ' . str_replace ( '/', '\\\\/', \\$regex_value ) . '/imsx' ; // Call either the PregMatchEx or PregMatchAllEx method if ( \\$match_all ) \\$status = self::PregMatchAllEx ( \\$regex_value, \\$subject, \\$match_result, \\$flags ) ; else \\$status = self::PregMatchEx ( \\$regex_value, \\$subject, \\$match_result, \\$flags ) ; // Match found : add this line to the match list if ( \\$status ) { \\$reference = '\\\\' . \\$regex_key ; \\$new_match = [ 'reference' => \\$regex_key, 'subject' => \\$subject, 'subject-index' => \\$subject_index, 'regex' => \\$regex_value, 'regex-index' => \\$regex_index, 'matches' => \\$match_result ] ; // Handle the case where several regex match the same string // For example, if both regex indexed by \"\\4\" and \"\\5\" match the same string, we will have // to construct a matching regex having the following contents : // ( (\\4) | (\\5) ) if ( isset ( \\$match_list [ \\$subject_index ] ) ) { \\$match_list [ \\$regex_key ] [] = \\$new_match ; \\$match_references [ \\$subject_index ] [] = \\$reference ; } else { \\$match_list [ \\$regex_key ] = [ \\$new_match ] ; \\$match_references [ \\$subject_index ] = [ \\$reference ] ; } \\$found = true ; } \\$regex_index ++ ; } // If no matching regex has been found, record the index of the current line if ( ! \\$found ) \\$missing_matches [] = \\$subject_index ; \\$subject_index ++ ; } // Not all subject lines have a match in the \\$regex_list array : consider this match has failed \\$status = false ; if ( ! count ( \\$missing_matches ) ) { // Since an input string may correspond to several matches, get all the possible combination of matches \\$key_subjects = self::CombinationsOf ( \\$match_references ) ; // Make \\$sequence a regex if not already specified : add delimiters and options if ( ! self::IsRegex ( \\$new_sequence ) ) \\$new_sequence = '/^ ' . str_replace ( '/', '\\\\/', \\$new_sequence ) . ' \\$/imsx' ; // Find a match \\$status = false ; foreach ( \\$key_subjects as \\$key_subject ) { \\$subject_string = implode ( '', \\$key_subject ) ; if ( self::PregMatchAll ( \\$new_sequence, \\$subject_string, \\$seq_match ) ) { \\$matches = \\$match_list ; \\$status = true ; } } } // Return match status return ( \\$status ) ; } /** * Performs multiple inline substrings replacements. * * @param string \\$subject * String where replacements are to be performed. * * @param array \\$replacements * Array of arrays, each of them containing 3 elements : * - Element 1 : * The string to be replaced in \\$subject. * - Element 2 : * The replacement string. * - Element 3 : * The offset, in \\$subject, of the string to be replaced. * * @return string * The input string, with all replacements having taken place. * */ public static function MultiSubstrReplace ( \\$subject, \\$replacements ) { // First, sort entries by ascending offset if ( count ( \\$replacements ) > 1 ) usort ( \\$replacements, function ( \\$a, \\$b ) { return ( \\$a - \\$b ) ; } ) ; // Parts that are extracted from the subject \\$list = [] ; // Last seen subject string offset so far \\$last_seen_offset = 0 ; \\$subject_length = strlen ( \\$subject ) ; // Loop through replacement strings foreach ( \\$replacements as \\$replacement ) { \\$length = strlen ( \\$replacement ) ; // Delta between current offset and last seen offset : add this substring to the list of items to be joined at the end if ( \\$replacement > \\$last_seen_offset ) { \\$list [] = substr ( \\$subject, \\$last_seen_offset, \\$replacement - \\$last_seen_offset ) ; \\$last_seen_offset = \\$replacement + \\$length ; } // Include the replacement string \\$list [] = \\$replacement ; // Update currently last seen offset (= current offset + current string length) \\$last_seen_offset = \\$replacement + \\$length ; } // Don't forget the trailing characters if ( \\$last_seen_offset < \\$subject_length ) \\$list [] = substr ( \\$subject, \\$last_seen_offset ) ; // All done, return return ( implode ( '', \\$list ) ) ; } /** * * Normalizes a sequence for the MetaPregMatchEx method. * * Normalizes a meta-sequence, which uses preg-like backreference syntax to reference * regular expressions indexed by the backreference value in the \\$match_definitions array. * The method accepts all the backreference syntaxes that are recognized by the preg_replace * function ('x' stands for a sequence of digits, 'name' for a group capture name) : * - \\x * - \\gx * - \\g{x} * - (?P=name) * - \\k * - \\k'name' * - \\k{name} * - \\g{name} * All those forms are normalized in the input sequence as : * (\\x) * or : * (\\name) * Note the enclosing parentheses to prevent side effects when performing the match. * * @param string \\$sequence * Sequence to be normalized. * * @param mixed \\$subsequences * Associative array whose keys are sequence references and whose values are * regular expressions to be matched. * When specified, all references specified in the \\$sequence parameter are checked * for existence in this array. * * @return string * Returns the normalized sequence. * */ // A regular expression matching all the possible backreferences allowed in PHP // ('x' stands for a sequence of digits, 'name' for a group capture name) : // - \\x // - \\gx // - \\g{x} // - (?P=name) // - \\k // - \\k'name' // - \\k{name} // - \\g{name} // Because of the (?P=name) form, we cannot unify all the regular expressions matching the // above syntaxes, so we need to split the matching in two groups const META_SEQUENCE_MATCH = '# [^\\\\\\\\]? (?P (?P \\\\\\\\ ( ( g (?P \\d+) ) | ( g \\{ (?P \\d+) \\} ) | ( k \\< (?P [\\w.\\-]+) \\> ) | ( k \\' (?P [\\w.\\-]+) \\' ) | ( [kg] \\{ (?P [\\w.\\-]+) \\} ) | ( (?P [\\w.\\-]+) ) | ( (?P \\d+) ) ) ) | (?P \\( \\? P = (?P [\\w_.\\-]+) \\) ) ) #imsx' ; public static function NormalizeMetaSequence ( \\$sequence, &\\$subsequences = null ) { // Are there any references to match items in the sequence string ? if ( preg_match_all ( self::META_SEQUENCE_MATCH, \\$sequence, \\$matches, PREG_OFFSET_CAPTURE ) ) { \\$substrings = [] ; // Loop through found matches foreach ( \\$matches as \\$key => \\$match ) { // Numeric keys simply indicate unnamed group captures - ignore them if ( is_numeric ( \\$key ) ) continue ; // In order to obtain the real capture length, we need to determine whether the match comes // from or \\$group = false ; if ( ! strncmp ( \\$key, 'number', 5 ) || ! strncmp ( \\$key, 'name', 4 ) ) \\$group = '1' ; else if ( ! strncmp ( \\$key, 'named', 5 ) ) \\$group = '2' ; else continue ; \\$groupname = \"group\\$group\" ; \\$index = 0 ; // Loop through each match found foreach ( \\$matches [ \\$key ] as \\$value ) { // ... but only if the value is an array and its offset item is not negative if ( is_array ( \\$value ) && \\$value != -1 ) { // Add it to the substrings array which will be passed to the Regex::MultiSubstrReplace() method // Note the extra 4th element, not used by Regex::MultiSubstrReplace, which serves to determine // if the reference exists as a key in the \\$match_definitions array, when specified \\$substrings [] = [ \\$matches [ 'match' ] [ \\$index ] , '(\\\\\\\\' . \\$value . ')', \\$matches [ \\$groupname ] [ \\$index ] , \\$matches [ \\$key ] [ \\$index ] ] ; } \\$index ++ ; } } // Replace all reference syntaxes allowed with a much simpler \"(\\reference)\" form \\$new_sequence = Regex::MultiSubstrReplace ( \\$sequence, \\$substrings ) ; // If matches have been specified, check that all the references found in \\$sequence have a corresponding entry // in the \\$match_definitions array if ( \\$subsequences !== null ) \\$subsequences = \\$substrings ; return ( \\$new_sequence ) ; } // Useless sequence, since it contains no reference to a match string else throw new Exception ( \"The following sequence does not contain any reference to match strings :\\n\\$sequence\" ) ; } /** * * Removes unnamed captures from the result of a call to a preg_* function. * * @param array \\$matches * Matches returned as the 3rd parameter of a preg_* call. * * @param int \\$flags * PREG_* flags specified when calling a preg_* function. When the PREG_OFFSET_CAPTURE flag is * specified, it happens that some results are an empty string instead of a 2-elements array. * This helps removing unnecessary entries. * */ public static function PregWipeMatches ( &\\$matches, \\$flags ) { \\$new_matches = [] ; foreach ( \\$matches as \\$key => \\$value ) { if ( is_numeric ( \\$key ) ) continue ; if ( \\$flags & PREG_OFFSET_CAPTURE ) { if ( ! is_array ( \\$value ) ) continue ; if ( \\$value == -1 ) continue ; } \\$new_matches [ \\$key ] = \\$value ; } \\$matches = \\$new_matches ; } /** * * Encapsulates the preg_match() function and optionnally wipes unnamed captures if the PREG_WIPE_MATCHES flag * is specified. * */ public static function PregMatch ( \\$pattern, \\$subject, &\\$matches = null, \\$flags = 0, \\$offset = 0 ) { // Perform the match and handle potential error \\$status = @preg_match ( \\$pattern, \\$subject, \\$matches, \\$flags, \\$offset ) ; if ( \\$status === false ) throw ( new Exception ( \"Invalid regex : \\$pattern\" ) ) ; // If needed, wipe any unnamed captures if ( \\$flags & PREG_WIPE_MATCHES ) self::PregWipeMatches ( \\$matches, \\$flags ) ; // All done, return return ( \\$status ) ; } /** * * Encapsulates the preg_match_all() function and optionnally wipes unnamed captures if the PREG_WIPE_MATCHES flag * is specified. * */ public static function PregMatchAll ( \\$pattern, \\$subject, &\\$matches = null, \\$flags = PREG_PATTERN_ORDER, \\$offset = 0 ) { // Perform the match and handle potential error \\$status = @preg_match_all ( \\$pattern, \\$subject, \\$matches, \\$flags, \\$offset ) ; if ( \\$status === false ) throw ( new Exception ( \"Invalid regex : \\$pattern\" ) ) ; // If needed, wipe any unnamed captures if ( \\$flags & PREG_WIPE_MATCHES ) self::PregWipeMatches ( \\$matches, \\$flags ) ; // All done, return return ( \\$status ) ; } /** * * Encapsulates the preg_replace() function. * */ public static function PregReplace ( \\$pattern, \\$replacement, \\$subject, \\$limit = -1, \\$count = null ) { \\$status = @preg_replace ( \\$pattern, \\$replacement, \\$subject, \\$limit, \\$count ) ; if ( \\$status === false ) throw ( new Exception ( \"Invalid regex : \\$pattern\" ) ) ; return ( \\$status ) ; } /** * * An extended version of the preg_match() function, that allows for specifying multiple named captures * with the same name. * * @param array \\$matches * Strings matched by the captures. Since named captures can be specified more than once, each array item * will contain an additional level of indirection, an array for each matched item. * Thus, the elements of a capture named will be accessible through the following expressions : * - \\$match [ 'pat' ] will yield to the first capture of a group named 'pat' * - count ( \\$match [ 'pat' ] ) will give the number of expressions matched by the named capture 'pat' * The same applies to unnamed captures. * */ public static function PregMatchEx ( \\$pattern, \\$subject, &\\$matches = null, \\$flags = 0, \\$offset = 0 ) { \\$newpattern = self::RenumberNamedCaptures ( \\$pattern, \\$replacements ) ; if ( \\$status = self::PregMatch ( \\$newpattern, \\$subject, \\$matches, \\$flags, \\$offset ) ) { \\$matches = self::GroupNamedCaptures ( \\$matches, \\$replacements ) ; } return ( \\$status ) ; } /** * * An extended version of the preg_match_all() function, that allows for specifying multiple named captures * with the same name. * */ public static function PregMatchAllEx ( \\$pattern, \\$subject, &\\$matches = null, \\$flags = 0, \\$offset = 0 ) { \\$replacements = [] ; \\$newpattern = self::RenumberNamedCaptures ( \\$pattern, \\$replacements ) ; if ( \\$status = self::PregMatchAll ( \\$newpattern, \\$subject, \\$matches, \\$flags, \\$offset ) ) { \\$matches = self::GroupNamedCaptures ( \\$matches, \\$replacements ) ; // Cancel one level of indirection in the results ; the resulting match array will have // the same shape as the one returned by the PregMatchEx() method foreach ( \\$matches as \\$key => \\$value ) { // Non-numeric keys are named pattern matches : get rid of one indirection level and collect only // the successful matches ; this is a deviation from the normal preg_match_all() function, where the // results could include as well an empty string or a sub-array with an empty string and an offset of -1 if ( ! is_numeric ( \\$key ) ) { \\$new_array = [] ; foreach ( \\$value as \\$subvalue ) { foreach ( \\$subvalue as \\$subsubkey => \\$subsubvalue ) { if ( isset ( \\$subsubvalue ) && is_array ( \\$subsubvalue ) && \\$subsubvalue != -1 ) \\$new_array [ \\$subsubkey ] = \\$subsubvalue ; } } \\$matches [ \\$key ] = \\$new_array ; } // For numeric keys, when the sub-array contains only one element, then this is a normal preg_match result, // so get rid of the level of indirection that has been added by the GroupNamedCaptures() method else if ( count ( \\$value ) == 1 ) \\$matches [ \\$key ] = \\$value ; } } return ( \\$status ) ; } /*-------------------------------------------------------------------------------------------------------------- NAME PregStrReplace - Replace string(s) using regular expression(s) PROTOTYPE \\$result = PdfToText::PregStrReplace ( \\$pattern, \\$replacement, \\$subject, \\$limit = -1, &\\$match_count = null ) DESCRIPTION This function behaves like a mix of str_replace() and preg_replace() ; it allows to search for strings using regular expressions, but the replacements are plain-text strings and no reference to a capture specified in the regular expression will be interpreted. This is useful when processing replacement strings that contain constructs such as \"\\00\" or \"\\$\", which are interpreted by preg_replace() as references to captures. This function has the same parameters as preg_replace(). RETURN VALUE Returns the substituted text. *-------------------------------------------------------------------------------------------------------------*/ public static function PregStrReplace ( \\$pattern, \\$replacement, \\$subject, \\$limit = -1, &\\$match_count = null ) { // Make sure that \\$pattern and \\$replacement become arrays of the same size if ( is_array ( \\$pattern ) ) { if ( is_array ( \\$replacement ) ) { if ( count ( \\$pattern ) !== count ( \\$replacement ) ) { trigger_error ( \"The \\\\$replacement parameter should have the same number of element as \\\\$pattern.\" ) ; return ( \\$subject ) ; } } else \\$replacement = array_fill ( \\$replacement, count ( \\$pattern ), \\$replacement ) ; } else { if ( is_array ( \\$replacement ) ) { trigger_error ( \"Expected string for the \\\\$replacement parameter.\" ) ; return ( \\$subject ) ; } \\$pattern = array ( \\$pattern ) ; \\$replacement = array ( \\$replacement ) ; } // Upper limit if ( \\$limit < 1 ) \\$limit = PHP_INT_MAX ; // Loop through each supplied pattern \\$current_subject = \\$subject ; \\$count = 0 ; for ( \\$i = 0, \\$pattern_count = count ( \\$pattern ) ; \\$i < \\$pattern_count ; \\$i ++ ) { \\$regex = \\$pattern [\\$i] ; // Get all matches for this pattern if ( preg_match_all ( \\$regex, \\$current_subject, \\$matches, PREG_OFFSET_CAPTURE ) ) { \\$result = '' ; // Current output result \\$last_offset = 0 ; // Process each match foreach ( \\$matches as \\$match ) { \\$offset = ( integer ) \\$match ; // Append data from the last seen offset up to the current one if ( \\$last_offset < \\$offset ) \\$result .= substr ( \\$current_subject, \\$last_offset, \\$offset - \\$last_offset ) ; // Append the replacement string for this match \\$result .= \\$replacement [\\$i] ; // Compute next offset in \\$current_subject \\$last_offset = \\$offset + strlen ( \\$match ) ; // Limit checking \\$count ++ ; if ( \\$count > \\$limit ) break 2 ; } // Append the last part of the subject that has not been matched by anything \\$result .= substr ( \\$current_subject, \\$last_offset ) ; // The current subject becomes the string that has been built in the steps above \\$current_subject = \\$result ; } } /// All done, return return ( \\$current_subject ) ; } /** * * Gives a unique id to each named capture within a regex. * * Reassigns unique identifiers to named captures within a regular expression. The new * identifiers will have the form \"prefix_x\", where \"prefix\" is given by the \\$prefix * parameter, and \"x\" a unique identifier starting from 0. * * @param string \\$pattern * Regex pattern containing potential named captures to be renamed. * * @param array \\$correspondances * On output, will hold an associative array whose keys are the new capture group names, and values the old ones. * * @param string \\$prefix * Prefix string for capture name replacements. * * @return string * Returns the input pattern with all named captures replaced by unique identifiers. * * @notes * This method, along with the GroupNamedCaptures() one, is used by the Preg*Ex methods * to allow processing of regular expressions having duplicate named captures. * */ public static function RenumberNamedCaptures ( \\$pattern, &\\$correspondances = [], \\$prefix = 'match_' ) { static \\$re = '/ \\( \\? P < (?P [^>]+ ) > /imsx' ; // Get named captures if ( self::PregMatchAll ( \\$re, \\$pattern, \\$matches, PREG_OFFSET_CAPTURE ) ) { \\$index = 0 ; \\$pattern_matches = [] ; // Loop through pattern matches foreach ( \\$matches [ 'pattern' ] as \\$match ) { \\$pname = \\$match ; \\$poffset = \\$match ; \\$newpattern = \"\\$prefix\\$index\" ; // Build the correspondance array \\$correspondances [ \\$newpattern ] = \\$pname ; // Add this entry (old name, new name, offset) into an array for the Regex::MultiSubsrReplace() method \\$pattern_matches [] = [ \\$pname, \\$newpattern, \\$poffset ] ; \\$index ++ ; } // Perform the multiple-string replace \\$new_pattern = Regex::MultiSubstrReplace ( \\$pattern, \\$pattern_matches ) ; } else \\$new_pattern = \\$pattern ; // All done, return return ( \\$new_pattern ) ; } /** * * Replaces patterns in a regular expression string. * * Replace named patterns in a string. This function uses the result of self::PregMatchAll() * to match named patterns with the supplied input array \\$replacements. * * @param string \\$pattern * A pattern matching subpart(s) of the specified subject string. * * @param string \\$subject * String to be matched against. * * @param array \\$replacements * Associative array whose keys are the pattern name (as specified in the * (?P re) parts of a regular expression) and whose values are also * an associative array. Each entry in the array have the following meaning : * * - key : A regular expression specifying the value of the named pattern * name. Do not put anchors nor delimiters in this pattern since * they are automatically added. * - value : The replacement value for the named pattern specified by the key * value. * * @param int \\$options * PREG_* options. * * @return string * Returns the substituted string. * * @example * The following example will replace : * - every matched pattern named \"toto\" by one of the string matching this pattern, * either 'the new replacement for the pattern string' or 'the replacement of thepattern', * for captures matching either 'pattern.*' or 'thepattern', respectively. * The (?P ...) or (?P ...) match the first item. * - Every matched pattern name \"aaa\" by the string 'replacement of aaa'. * * \\$subject = \"aaa (?P coucou) zzzz (?P coucou2) aaa (?P zzzz)\"; * \\$pattern = \"# ( \\( \\? P < (?P [^>]+) > .*? \\) ) | (?P aaa*) #imsx\" ; * \\$replacement = * [ * \"toto\" => * [ * 'pattern.*' => 'the new replacement for the pattern string', * 'thepattern' => 'the replacement of thepattern' * ], * \"aaa\" => * [ * 'aaa' => 'replacement of aaa' * ] * ] ; * \\$result = String::RegReplaceNamedPatterns ( \\$pattern, \\$subject, \\$replacement ) ) ; * * The resulting string will be : * replacement of aaa (?P coucou) zzzz (?P coucou2) replacement of aaa (?P zzzz) * */ public static function ReplaceNamedPatterns ( \\$pattern, \\$subject, \\$replacements, \\$options = null ) { // Process the substitutions only if there is a match... if ( self::PregMatchAll ( \\$pattern, \\$subject, \\$matches, PREG_OFFSET_CAPTURE | \\$options ) ) { \\$substitutions = [] ; // Loop through matches foreach ( \\$matches as \\$match_key => \\$match_values ) { // ... then through each matched value foreach ( \\$match_values as \\$match_value ) { // Ignore empty matches if ( ! \\$match_value || \\$match_value == -1 ) continue ; // Loop through replacement patterns foreach ( \\$replacements as \\$replacement_key => \\$replacement_values ) { // Skip non-matching ones if ( strcmp ( \\$match_key, \\$replacement_key ) ) continue ; // Find the replacement values for each matched pattern foreach ( \\$replacement_values as \\$replacement_re => \\$replacement_value ) { if ( self::PregMatch ( \"/^\\$replacement_re\\\\$/imsx\", \\$match_value ) ) { \\$substitutions [] = [ \\$match_value , // Original value to be replaced \\$replacement_value, // Replacement value \\$match_value // Original value offset ] ; } } } } } // Replace catched captures \\$new_subject = self::MultiSubstrReplace ( \\$subject, \\$substitutions ) ; return ( \\$new_subject ) ; } // No match found : return the subject as is else return ( \\$subject ) ; } /** * Converts an Msdos or Unix-style wildcard string to a regular expression. * * Converts an Msdos or Unix-style wildcard string to a regular expression. Allowed wildcard forms are : * '?' - * Matches 0 or 1 character Path separator cannot be matched with this expression. * '*' - * Matches 0 or more characters. Path separator cannot be matched with this expression. * '[cclass]' - * A character class that matches one character, for example \"[a-z]\" to match any lowercase alphabetic character, or * \"[^a-z]\" to match anything but a lowercase alphabetic character. * * Note that the path separator can either be '/' or '\\' : this method does not take care of the host operating system conventions. * * @param string \\$pattern * Wildcard pattern to be converted. * * @param string \\$escaped_chars * Optional characters to be escaped in the regular expression (regex special characters are systematically escaped). * * @return bool|string * Returns false if the wilcard string cannot be converted to a regular expression (typically because there is an angle * bracket mismatch) or the regular expression corresponding to the supplied wildcard pattern. * Note that the returned value does not include the leading and trailing delimiters, so that it can be included into * an existing regex. * */ public static function WildcardToRegex ( \\$pattern, \\$escaped_chars = \"\" ) { \\$length = strlen ( \\$pattern ) ; \\$newpattern = \"\" ; for ( \\$i = 0 ; \\$i < \\$length ; \\$i ++ ) { \\$char = \\$pattern [ \\$i ] ; \\$depth = 0 ; switch ( \\$char ) { case '.' : case '+' : case '^' : case '\\$' : case '(' : case ')' : case '|' : case '{' : case '}' : case '=' : case '!' : case '<' : case '>' : case '/' : \\$newpattern .= '\\\\' . \\$char ; break ; case '?' : case '*' : \\$newpattern .= '[^\\\\/]' . \\$char ; break ; case '[' : \\$newpattern .= '[' ; \\$depth ++ ; break ; case ']' : if ( ! \\$depth ) return ( false ) ; \\$newpattern .= ']' ; break ; default : if ( strpos ( \\$escaped_chars, \\$char ) !== false ) \\$newpattern .= '\\\\' ; \\$newpattern .= \\$char ; } } return ( \\$newpattern ) ; } } ```",
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https://www.engineeringdaily.net/brain-teaser-a-distribution-managers-dilemma/ | [
"# Brain teaser – A distribution manager’s dilemma\n\nJohn the distribution manager for a leading mobile phone company has a dilemma. The warehouse has 10 unlabelled rows of pallets, each row contains thousands of phones destined for different countries. Each 100g mobile phone is exactly the same except for those in the row destined for Japan, which have a “special” 2g chip encased within the phone to make sure they work on the Japanese networks.\n\nAll the trucks are waiting outside ready to go their separate ways, how can John make sure the right phones go to Japan in the quickest time possible? All John has at his disposal is a digital balance.",
null,
"## Calculate the velocity of water coming out of a double-entry pipe\n\nIf we know the volumetric flow rates of the water going into the two branches, …\n\n1.",
null,
"Weigh R1 n R2..if both are of equal weight, use either R1 or R2 against the other rows to find the odd one out..\nif R1 n R2 are of unequal weight, use R1 against R3,\nif the balance is equal then R2 is the odd one out…\nif the balance is again unequal then R1 is the odd one out..\n\n2.",
null,
"Take 1 phone from row 1, 2 phones from row 2, 3 phones from row 3 etc.\nThe total weight if all the phones were 100g each would be 10!, or 550g.\n\nX = Total weight\nY = Row number destined for Japan\n\nY = (X – 10!)/2\n\n3.",
null,
"Assuming a balance scale can only John tell John which of two weights is heavier (or lighter), he can identify the heavier (102g) Japanese row from the others (100g) in 2-3 measurements using one phone from each row (R1-R10).\n1. Determine which group is heavier between R1-R5 and R6-R10. Keep the heavier group (e.g., R1-R5).\n2. Determine which pair is heavier between R1-R2 and R3-R4. Keep the heavier pair (e.g., R1-R2).\n3. Determine which phone is heavier between R1 and R2. The heavier phone is Japanese. 3 measurements.\n4. If the two pairs are equal weight in step 2, assume R5 is the heavier Japanese phone. 2 measurements.\n\n4.",
null,
"John should take a different number of phones from each 9 rows and put them all on the digital balance. Since there are 10 rows, he should get a weight of 4500 grams (by doing [9+8+7+6+5+4+3+2+1] multiplied by weight of 100g) plus the extra weight of 2g per phone from the Japanese row. So if, for example, he gets a total weight of 4516 grams, then he knows the row that he took 8 phones from is the row destined for Japan (since 8*2 equals the extra 16g in the weight.) If the weight comes out to be exactly 4500 grams, then John will know that the row which he did not take out any phone from is the one destined to Japan, since no extra weight of 2g was added to the scale.\nLet me know if this makes sense 😉\n\n5.",
null,
"I like the brain teasers!\n\n•",
null,
"I am glad that you do. We will keep bringing them to you.\nKen.\n\nSahifa Theme License is not validated, Go to the theme options page to validate the license, You need a single license for each domain name."
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"https://secure.gravatar.com/avatar/6b36dbc9b758565a986b6b1c2605b164",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.94752157,"math_prob":0.9775658,"size":2519,"snap":"2023-40-2023-50","text_gpt3_token_len":663,"char_repetition_ratio":0.13876739,"word_repetition_ratio":0.0,"special_character_ratio":0.27312425,"punctuation_ratio":0.107334524,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.96154606,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14],"im_url_duplicate_count":[null,null,null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-10-03T11:51:12Z\",\"WARC-Record-ID\":\"<urn:uuid:6db10e1d-d4a9-4b26-8244-80e46cbf2639>\",\"Content-Length\":\"135292\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4fe7267b-e9fc-4300-9529-3a5504d24b1b>\",\"WARC-Concurrent-To\":\"<urn:uuid:57056718-5069-4f7f-9137-b7588953ca63>\",\"WARC-IP-Address\":\"159.203.120.8\",\"WARC-Target-URI\":\"https://www.engineeringdaily.net/brain-teaser-a-distribution-managers-dilemma/\",\"WARC-Payload-Digest\":\"sha1:6TKSV6LOLPVWFZX7I626DFVMFD4MT7AW\",\"WARC-Block-Digest\":\"sha1:EVM6DFRHME4HSIPC4DOYRLYFNMD6AATM\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233511075.63_warc_CC-MAIN-20231003092549-20231003122549-00057.warc.gz\"}"} |
https://www.marktechpost.com/2019/02/17/tensors-the-building-block-of-tensorflow/embed/ | [
"TensorFlow uses tensor to define the framework and processing data. A tensor conceptualized multidimensions vectors and matrices. Mathematically, a tensor is a geometric object that maps in a multi-linear manner geometric vectors, scalars, and another tensor(s) to a resulting tensor. Rank Entity 0 Scalar 1 Vector 2 Matrix 3 3-Tensor n n-Tensor These tensor objects used to … Continue reading Tensors: The building block of TensorFlow"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7794739,"math_prob":0.71760184,"size":584,"snap":"2022-27-2022-33","text_gpt3_token_len":125,"char_repetition_ratio":0.13965517,"word_repetition_ratio":0.04494382,"special_character_ratio":0.1900685,"punctuation_ratio":0.07692308,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99374676,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-08-16T01:43:42Z\",\"WARC-Record-ID\":\"<urn:uuid:b2ddb5c7-df67-4a69-b4d3-14c4e75420d9>\",\"Content-Length\":\"17865\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:765231d5-85e4-426a-83cf-7f850f924635>\",\"WARC-Concurrent-To\":\"<urn:uuid:85753c2f-f0c8-4142-ab44-b902bb451ddb>\",\"WARC-IP-Address\":\"35.208.2.109\",\"WARC-Target-URI\":\"https://www.marktechpost.com/2019/02/17/tensors-the-building-block-of-tensorflow/embed/\",\"WARC-Payload-Digest\":\"sha1:EDBA3I6X7BSH7MWSXQTATLMN44BCD2FO\",\"WARC-Block-Digest\":\"sha1:KPWR25ALIEGYSRGOUKJ2YJYJPAUL4H5M\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-33/CC-MAIN-2022-33_segments_1659882572215.27_warc_CC-MAIN-20220815235954-20220816025954-00031.warc.gz\"}"} |
https://tug.org/pipermail/macostex-archives/2005-June/016093.html | [
"# [OS X TeX] Tex4ht Problem?\n\nHerbert Schulz herbs at wideopenwest.com\nWed Jun 22 15:12:30 CEST 2005\n\nHowdy,\n\nI used to get a nicely formatted table using htlatex on the source\nbelow. The compile options (i.e., first option list after the file\nname) to compile was \"html, pic-m, pic-tabular, pic-fbox\" (as in the\ncommented out \\usepackage) and it was compiled via CLI. Of course\nthe table and all of its contents were really graphical images but\nthey looked nice on the screen. Somewhere along the line things went\nbad and with the latest 2005 gwTeX the image of the table isn't even\nbuilt. If I leave out the options or change $...$ to $$...$$ I get\nsomething but it's really ugly.\n\n---------- snip ----------\n%!TEX TS-program = htlatex\n\\documentclass[11pt]{article}\n%\\usepackage{tmmtmx}\n%\\usepackage[html, pic-m, pic-tabular, pic-fbox]{tex4ht}\n\n\\begin{document}\n\\noindent This is a fancy table from the \\TeX Book written in \\LaTeX\n\\ which includes mathematics within it:\n\\begin{center}\n\\setlength\\fboxrule{0.7pt}%\n\\setlength\\fboxsep{0pt}%\n\\newcommand\\tblstrut[0 pt]{\\rule[-#1]{0 pt}{#1}\\rule{0 pt}{#2}}%\n\\newcommand\\erf{\\mathop{\\mathrm{erf}}}%\n\\fbox{%\n\\begin{tabular}{l|r@{$\\displaystyle{}={}$}l}\n\\tblstrut[9 pt]{14 pt} \\textit{Name} &\n\\multicolumn{2}{c}{\\textit{Definition}} \\\\\n\\hline\n\\tblstrut[15 pt]{20 pt} Gamma & $\\displaystyle\\Gamma(z)$ & $\\displaystyle\\int_0^\\infty\\!\\!t^{z-1}e^{-t}\\,dt$ \\\\\n\\hline\n\\tblstrut[15 pt]{20 pt} Sine & $\\displaystyle\\sin(x)$ &\n$\\displaystyle\\frac1{2i}(e^{ix} - e^{-ix})$ \\\\\n\\hline\n\\tblstrut[15 pt]{20 pt} Error & $\\displaystyle\\erf(z)$ &\n$\\displaystyle\\frac2{\\sqrt\\pi}\\int_0^z\\!\\!e^{-z^2}\\,dz$ \\\\\n\\hline\n\\tblstrut[15 pt]{20 pt} Bessel & $\\displaystyle J_0(z)$ &\n$\\displaystyle\\frac1{\\pi}\\int_0^\\pi\\!\\!\\cos(z\\sin\\theta)\\,d\\theta$ \\\\\n\\hline\n\\tblstrut[15 pt]{20 pt} Zeta & $\\displaystyle\\zeta(s)$ &\n$\\displaystyle\\sum_{k=1}^\\infty k^{-s}\\quad(\\Re s>1)$\n\\end{tabular}}\n\\end{center}\n\\end{document}\n---------- snip ----------\n\nGood Luck,\n\nHerb Schulz\n(herbs at wideopenwest.com)\n\n--------------------- Info ---------------------\nMac-TeX Website: http://www.esm.psu.edu/mac-tex/\n& FAQ: http://latex.yauh.de/faq/\nTeX FAQ: http://www.tex.ac.uk/faq\nList Post: <mailto:MacOSX-TeX at email.esm.psu.edu>"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5650233,"math_prob":0.91606796,"size":2278,"snap":"2023-40-2023-50","text_gpt3_token_len":785,"char_repetition_ratio":0.14995602,"word_repetition_ratio":0.019379845,"special_character_ratio":0.35338014,"punctuation_ratio":0.13647059,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.996782,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-25T18:52:23Z\",\"WARC-Record-ID\":\"<urn:uuid:9f342b78-b27c-4024-94e5-ac082a215d37>\",\"Content-Length\":\"5220\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:af0a248f-46d0-40f3-bce2-1ff82805a357>\",\"WARC-Concurrent-To\":\"<urn:uuid:81b14464-ce46-46ae-8137-35fcb910833b>\",\"WARC-IP-Address\":\"46.4.94.215\",\"WARC-Target-URI\":\"https://tug.org/pipermail/macostex-archives/2005-June/016093.html\",\"WARC-Payload-Digest\":\"sha1:WFUALHQ6J6JKV7MORHT4O7PW6DA4TWWL\",\"WARC-Block-Digest\":\"sha1:YVIY3SW2JDFMCQ6OKH5V5C44I3NORT4Y\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233510085.26_warc_CC-MAIN-20230925183615-20230925213615-00833.warc.gz\"}"} |
http://ccrl.chessdom.com/ccrl/4040/cgi/engine_details.cgi?print=Details&each_game=1&eng=Minic%202.46%2064-bit | [
"Contents: CCRL 40/15 Downloads and Statistics September 26, 2020 Testing summary: Total: 1'179'815 games played by 2'715 programs White wins: 406'597 (34.5%) Black wins: 300'322 (25.5%) Draws: 472'896 (40.1%) White score: 54.5%\n\n## Engine Details\n\n Options Show each game results\nMinic 2.46 64-bit#50 (3050+25\n−25\n)Quote\n Author: Vivien Clauzon (France) Link: Homepage\nThis is one of the 13 Minic versions we tested: Compare them!\n Opponent Elo Diff Results Score LOS Perf – Pedone 2.1 64-bit 3146 +56−55 (+96) 1.5 − 4.5(+0−3=3) 25.0%1.5 / 6 0.1% −54 0 0 0 = = = – Xiphos 0.4 64-bit 3145 +11−11 (+95) 8.5 − 11.5(+3−6=11) 42.5%8.5 / 20 0.0% +54 0 = 0 = 0 = = 1 = = 1 = = = 1 0 = = 0 0 – Roc 1.7 64-bit 3144 +40−40 (+94) 12 − 8(+6−2=12) 60.0%12.0 / 20 0.0% +149 1 = = = = = = 1 = 1 = = 1 0 = = 1 = 0 1 – Arasan 22.1 64-bit 3144 +24−24 (+94) 6.5 − 13.5(+1−8=11) 32.5%6.5 / 20 0.0% −8 = 0 = = 1 0 = = = 0 0 0 = 0 = = = = 0 0 – Laser 1.6 64-bit 3131 +11−11 (+81) 7 − 13(+1−7=12) 35.0%7.0 / 20 0.0% −5 = 0 = 0 0 = = = = 0 = = = 1 = 0 = 0 0 = – Nemorino 5.00 64-bit 3087 +13−13 (+37) 2.5 − 1.5(+2−1=1) 62.5%2.5 / 4 0.6% +132 0 = 1 1 – Winter 0.8 64-bit 3082 +21−21 (+32) 2 − 2(+1−1=2) 50.0%2.0 / 4 2.7% +32 1 = = 0 – chess22k 1.14 64-bit 3076 +18−18 (+26) 6.5 − 13.5(+1−8=11) 32.5%6.5 / 20 5.1% −75 = 0 = = 0 = 0 = = 0 = 0 = = = = 0 0 0 1 – Lc0 0.23.2 wLD2 64-bit 3068 +36−36 (+18) 8 − 12(+3−7=10) 40.0%8.0 / 20 20.5% −41 0 1 = = 1 = 0 0 = = = 1 = = = = 0 0 0 0 – Combusken 1.3.0 64-bit 3052 +24−24 (+2) 10.5 − 13.5(+4−7=13) 43.8%10.5 / 24 45.0% −36 = = = = = 1 1 = 0 0 = 0 = = 0 = 1 1 = 0 = 0 = 0 – Fat Fritz Junior w510 64-bit 3027 +34−34 (−23) 7 − 13(+2−8=10) 35.0%7.0 / 20 86.0% −112 0 0 = = 0 = = 0 0 = 0 1 = 1 = 0 0 = = = – Pirarucu 3.3.5 64-bit 3027 +19−19 (−23) 2 − 2(+1−1=2) 50.0%2.0 / 4 91.9% −33 0 = 1 = – Rybka 4 32-bit 3018 +15−15 (−32) 10 − 10(+5−5=10) 50.0%10.0 / 20 98.3% −30 1 0 = 0 0 = 1 = = = 1 = = = = 0 1 = 1 0 – Marvin 3.6.0 64-bit 3013 +21−21 (−37) 16.5 − 7.5(+12−3=9) 68.8%16.5 / 24 98.9% +82 1 = 1 = = = 1 = 1 = 0 = 1 0 = 1 1 0 1 1 1 1 = 1 – Monolith 2 64-bit 3001 +19−19 (−49) 12 − 12(+5−5=14) 50.0%12.0 / 24 99.9% −49 = = = 1 0 1 1 = = = = = = 0 1 0 1 = = = = 0 0 = – Bagatur 2.2 64-bit 2997 +21−21 (−53) 12.5 − 11.5(+5−4=15) 52.1%12.5 / 24 99.9% −42 = 0 = = = 1 = = = = 1 = 1 = = 0 = = 1 1 0 0 = = – Amoeba 3.2 64-bit 2993 +25−25 (−57) 3.5 − 0.5(+3−0=1) 87.5%3.5 / 4 99.9% +231 1 1 1 = – Rodent IV 022 64-bit 2990 +21−22 (−60) 13 − 11(+9−7=8) 54.2%13.0 / 24 100.0% −30 = = 1 0 1 1 = 0 0 = 0 1 1 0 = = = 0 1 1 1 0 1 = – Stockfish 1.8 32-bit 2990 +17−17 (−60) 10.5 − 9.5(+7−6=7) 52.5%10.5 / 20 100.0% −42 0 1 1 = = 1 = 1 1 1 0 = = 0 1 = 0 0 = 0 – Topple 0.7.5 64-bit 2984 +18−18 (−66) 11.5 − 8.5(+7−4=9) 57.5%11.5 / 20 100.0% −18 0 = = = = 1 1 1 1 1 0 = = 0 = = 1 1 0 = – Godel 7.0 64-bit 2981 +19−19 (−69) 12.5 − 11.5(+8−7=9) 52.1%12.5 / 24 100.0% −54 1 = 1 = 0 0 1 1 = 1 = 0 1 = 1 0 1 0 = = = = 0 0 – Amoeba 3.1 64-bit 2969 +20−20 (−81) 15 − 5(+10−0=10) 75.0%15.0 / 20 100.0% +68 1 1 = = 1 = = = 1 1 = 1 = 1 = 1 1 = 1 = – FabChess 1.15 64-bit 2943 +22−22 (−107) 19 − 5(+17−3=4) 79.2%19.0 / 24 100.0% +125 1 1 1 = = 1 1 = 1 1 1 0 0 1 1 1 0 1 1 1 1 = 1 1 – Naum 4 32-bit 2930 +14−13 (−120) 13 − 7(+9−3=8) 65.0%13.0 / 20 100.0% −22 = = = = 1 1 = = 0 1 1 1 0 0 1 1 1 = 1 = – Francesca MAD 0.29 64-bit 2914 +25−25 (−136) 21 − 5(+17−1=8) 80.8%21.0 / 26 100.0% +86 = 1 1 1 = 1 1 1 1 = = 1 1 1 1 1 = = = 1 1 0 = 1 1 1 – Counter 3.5 64-bit 2905 +21−21 (−145) 14.5 − 5.5(+11−2=7) 72.5%14.5 / 20 100.0% +4 1 = 1 = = = = = 1 1 1 0 1 1 1 0 = 1 1 1\n\n### Rating changes by day",
null,
"### Rating changes with played games",
null,
"Created in 2005-2013 by CCRL team Last games added on September 26, 2020"
] | [
null,
"http://ccrl.chessdom.com/ccrl/4040/rating-history-by-day-graphs/Minic_2_46_64-bit.png",
null,
"http://ccrl.chessdom.com/ccrl/4040/rating-history-by-day-graphs-2/Minic_2_46_64-bit.png",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.5605555,"math_prob":1.0000094,"size":3416,"snap":"2020-34-2020-40","text_gpt3_token_len":2270,"char_repetition_ratio":0.29396248,"word_repetition_ratio":0.33613446,"special_character_ratio":0.9145199,"punctuation_ratio":0.13013013,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.998457,"pos_list":[0,1,2,3,4],"im_url_duplicate_count":[null,2,null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-09-30T23:01:32Z\",\"WARC-Record-ID\":\"<urn:uuid:7f3d8e86-b891-47d2-900d-9e59c1b72b7d>\",\"Content-Length\":\"27639\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:238df94f-ec04-4a84-b1bd-018fa895c493>\",\"WARC-Concurrent-To\":\"<urn:uuid:53bba307-9941-438f-99c0-b589950ef721>\",\"WARC-IP-Address\":\"185.45.66.155\",\"WARC-Target-URI\":\"http://ccrl.chessdom.com/ccrl/4040/cgi/engine_details.cgi?print=Details&each_game=1&eng=Minic%202.46%2064-bit\",\"WARC-Payload-Digest\":\"sha1:QMP6PCDHNRKGAYQRWRKACPD6LRAAMCCV\",\"WARC-Block-Digest\":\"sha1:KAA5F3OQTBXBL3E323UYMSCDMXP2PM3D\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-40/CC-MAIN-2020-40_segments_1600402128649.98_warc_CC-MAIN-20200930204041-20200930234041-00759.warc.gz\"}"} |
https://www.c-sharpcorner.com/article/how-to-implement-graph-and-chart-control-in-windows-10-unive/ | [
"Post\n\n# How To Implement Graph And Chart Control In Windows 10 Universal App\n\n• 55.4k\n• 0\n• 1\n\nGraphs and charts are useful for visualizing and summarizing data for our users but in Windows 10 Universal app there is no default XAML control in Visual Studio for graphs and charts so we need to use other libraries paid or free such as WinRT XAML Toolkit or TelerikRadControls for Windows UWP.\n\nLet’s see the steps.\n\nCreate new Windows 10 universal project.\n\nThen we need to add WinRTXaml Toolkit reference.\n\nRight-click References in Solution Explorer, select Manage NuGet Packages, search WinRTXamlToolkit.Controls.DataVisualization.UWP and install it like the following screen.\n\nAfter successful installation go to your UI page “MainPage.XAML” and write the following code.\n\nxmlns:Charting=\"using:WinRTXamlToolkit.Controls.DataVisualization.Charting\"\n\nNow design the required chart and here I am going to add three charts: pie chart, line chart and column chart using the following code.\n\n1. <Charting:Chart\n2. x:Name=\"PieChart\"\n3. HorizontalAlignment=\"Left\"\n4. VerticalAlignment=\"Top\"\n5. Margin=\"0\" Width=\"323\" >\n6. <Charting:PieSeries Margin=\"0\"\n7. IndependentValuePath=\"Name\"\n8. DependentValuePath=\"Amount\"\n9. IsSelectionEnabled=\"True\"/>\n10. </Charting:Chart>\n11. <Charting:Chart\n12. x:Name=\"lineChart\"\n13. HorizontalAlignment=\"Left\"\n14. VerticalAlignment=\"Top\"\n15. Margin=\"0\" Height=\"159\" Width=\"316\" >\n16. <Charting:LineSeries Margin=\"0\"\n17. IndependentValuePath=\"Name\"\n18. DependentValuePath=\"Amount\"\n19. IsSelectionEnabled=\"True\"/>\n20. </Charting:Chart>\n21. <Charting:Chart\n22. x:Name=\"ColumnChart\"\n23. HorizontalAlignment=\"Left\"\n24. VerticalAlignment=\"Top\"\n25. Margin=\"0\" Width=\"329\" >\n26. <Charting:ColumnSeries Margin=\"0\"\n27. IndependentValuePath=\"Name\"\n28. DependentValuePath=\"Amount\"CharacterSpacing=\"5\"\n29. IsSelectionEnabled=\"True\"/>\n30. </Charting:Chart>\nNow go to code behind page and write the following code. I am going to show record of the user.\n1. publicclassRecords\n2. {\n3. publicstring Name\n4. {\n5. get;\n6. set;\n7. }\n8. publicint Amount\n9. {\n10. get;\n11. set;\n12. }\n13. }\n14. publicMainPage()\n15. {\n16. this.InitializeComponent();\n18. }\n20. {\n21. Random rand = newRandom();\n22. List < Records > records = newList < Records > ();\n24. {\n25. Name = \"Suresh\", Amount = rand.Next(0, 200)\n26. });\n28. {\n29. Name = \"C# Corner\", Amount = rand.Next(0, 200)\n30. });\n32. {\n33. Name = \"Sam\", Amount = rand.Next(0, 200)\n34. });\n36. {\n37. Name = \"Sri\", Amount = rand.Next(0, 200)\n38. });\n39. (PieChart.Series asPieSeries).ItemsSource = records;\n40. (ColumnChart.Series asColumnSeries).ItemsSource = records;\n41. (lineChart.Series asLineSeries).ItemsSource = records;\n42. }\nNow run the app and see the expected output like the following screen."
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.61459917,"math_prob":0.55251515,"size":2868,"snap":"2023-40-2023-50","text_gpt3_token_len":742,"char_repetition_ratio":0.11452514,"word_repetition_ratio":0.17357513,"special_character_ratio":0.2764993,"punctuation_ratio":0.17620137,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9658868,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-21T18:16:12Z\",\"WARC-Record-ID\":\"<urn:uuid:d4ac03b2-d160-4fd6-8a4a-9c960e97c808>\",\"Content-Length\":\"169665\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5cdb6f5f-abb6-47b2-8074-6dee7234b81a>\",\"WARC-Concurrent-To\":\"<urn:uuid:51c04839-2c89-4df7-bef1-8aa4554a9548>\",\"WARC-IP-Address\":\"40.65.205.118\",\"WARC-Target-URI\":\"https://www.c-sharpcorner.com/article/how-to-implement-graph-and-chart-control-in-windows-10-unive/\",\"WARC-Payload-Digest\":\"sha1:P2TO5K5URKYYLSBHX6EM4ZY75LHOA25W\",\"WARC-Block-Digest\":\"sha1:RARUHCGJRN4NH4B45YOM5T57BAANE4NW\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233506029.42_warc_CC-MAIN-20230921174008-20230921204008-00272.warc.gz\"}"} |
https://www.examrace.com/Study-Material/Statistics/Statistics-Mean.html | [
"# Competitive Exams: Mean and Its Types\n\nGlide to success with Doorsteptutor material for competitive exams : get questions, notes, tests, video lectures and more- for all subjects of your exam.\n\nDescribe arithmetic, geometric and harmonic means with suitable example. Explain merits and limitation of geometric mean.\n\n## Arithmetic Mean\n\nThe arithmetic mean is the “standard” average, often simply called the “mean” It is used for many purposes but also often abused by incorrectly using it to describe skewed distributions, with highly misleading results. The classic example is average income-using the arithmetic mean makes it appear to be much higher than is in fact the case. Consider the scores (1, 2, 2,2, 3,9) . The arithmetic mean is 3.16, but five out of six scores are below this!\n\nThe arithmetic mean of a set of numbers is the sum of all the members of the set divided by the number of items in the set (The word set is used perhaps somewhat loosely; for example, the number 3.8 could occur more than once in such a “set” ) . The arithmetic mean is what pupils are taught very early to call the “average.” If the set is a statistical population, then we speak of the population mean. If the set is a statistical sample, we call the resulting statistic a sample mean. The mean may be conceived of as an estimate of the median. When the mean is not an accurate estimate of the median, the set of numbers, or frequency distribution, is said to be skewed.\n\nWe denote the set of data by X = (x1, x2, … xn) . The symbol μ (Greek: Mu) is used to denote the arithmetic mean of a population. We use the name of the variable, X, with a horizontal bar over it as the symbol ( “X bar” ) for a sample mean. Both are computed in the same way:\n\nThe arithmetic mean is greatly influenced by outliers. In certain situations, the arithmetic mean is the wrong concept of “average” altogether. For example, if a stock rose 10 % in the first year, 30 % in the second year and fell 10 % in the third year, then it would be incorrect to report its “average” increase per year over this three year period as the arithmetic mean (10 %+ 30 %+ (-10 %) ) /3 = 10 % ; the correct average in this case is the geometric mean which yields an average increase per year of only 8.8 % .\n\n## Geometric Mean\n\nThe geometric mean is an average which is useful for sets of numbers which are interpreted according to their product and not their sum (as is the case with the arithmetic mean) . For example rates of growth.\n\nThe geometric mean of a set of positive data is defined as the product of all the members of the set, raised to a power equal to the reciprocal of the number of members. In a formula: The geometric mean of a1, a2, … an is, which is. The geometric mean is useful to determine “average factors” For example, if a stock rose 10 % in the first year, 20 % in the second year and fell 15 % in the third year, then we compute the geometric mean of the factors 1.10,1.20 and 0.85 as (1.10 × 1.20 × 0.85) = 1.0391 … And we conclude that the stock rose on average 3.91 percent per year. The geometric mean of a data set is always smaller than or equal to the set՚s arithmetic mean (the two means are equal if and only if all members of the data set are equal) . This allows the definition of the arithmetic-geometric mean, a mixture of the two which always lies in between. The geometric mean is also the arithmetic-harmonic mean in the sense that if two sequences (an) and (hn) are defined:\n\nand Then an and hn will converge to the geometric mean of x and y.\n\n## Harmonic Mean\n\nThe harmonic mean is an average which is useful for sets of numbers which are defined in relation to some unit, for example speed (distance per unit of time) .\n\nIn mathematics, the harmonic mean is one of several methods of calculating an average.\n\nThe harmonic mean of the positive real numbers a1, … an is defined to be\n\nThe harmonic mean is never larger than the geometric mean or the arithmetic mean (see generalized mean) . In certain situations, the harmonic mean provides the correct notion of “average” For instance, if for half the distance of a trip you travel at 40 miles per hour and for the other half of the distance you travel at 60 miles per hour, then your average speed for the trip is given by the harmonic mean of 40 and 60, which is 48; that is, the total amount of time for the trip is the same as if you traveled the entire trip at 48 miles per hour. Similarly, if in an electrical circuit you have two resistors connected in parallel, one with 40 ohms and the other with 60 ohms, then the average resistance of the two resistors is 48 ohms; that is, the total resistance of the circuit is the same as it would be if each of the two resistors were replaced by a 48-ohm resistor (Note: This is not to be confused with their equivalent resistance, 24 ohm, which is the resistance needed for a single resistor to replace the wo resistors at once.) . Typically, the harmonic mean is appropriate for situations when the average of rates is desired.\n\nAnother formula for the harmonic mean of two numbers is to multiply the two numbers, and divide that quantity by the arithmetic mean of the two numbers. In mathematical terms:\n\nMerits and limitation of geometric mean\n\n### Merits\n\n• It is based on each and every item of the series.\n• It is rigidly defined\n• It is useful in averaging ratio and percentage in determining rates of increase or decrease.\n• it gives less weight to large items and more to small items. Thus geometric mean of the geometric of values is always less than their arithmetic mean.\n• It is capable of algebraic manipulation like computing the grand geometric mean of the geometric mean of different sets of values.\n\n### Limitation\n\n• It is relatively difficult to comprehend, compute and interpret.\n• A GM with zero value cannot be compounded with similar other non-zero values with negative sign"
] | [
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.9382079,"math_prob":0.99564356,"size":5860,"snap":"2022-27-2022-33","text_gpt3_token_len":1331,"char_repetition_ratio":0.17810792,"word_repetition_ratio":0.055452865,"special_character_ratio":0.23430035,"punctuation_ratio":0.098305084,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9996124,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-08-14T13:28:19Z\",\"WARC-Record-ID\":\"<urn:uuid:a9610a92-a4c9-49e5-a42d-060a5276cf33>\",\"Content-Length\":\"20529\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:831abf4e-d076-4895-9e18-2957a0231196>\",\"WARC-Concurrent-To\":\"<urn:uuid:367316ea-565a-4aad-8dbd-0f9d21d90a08>\",\"WARC-IP-Address\":\"104.21.25.24\",\"WARC-Target-URI\":\"https://www.examrace.com/Study-Material/Statistics/Statistics-Mean.html\",\"WARC-Payload-Digest\":\"sha1:FTM25WBPE3XZ2GB7NO5YTHJJ7IQLJWYK\",\"WARC-Block-Digest\":\"sha1:X2AJZSGE6HXRSK3KVCEL7VJ44VQVNHDM\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-33/CC-MAIN-2022-33_segments_1659882572033.91_warc_CC-MAIN-20220814113403-20220814143403-00407.warc.gz\"}"} |
https://converter.ninja/volume/us-pints-to-imperial-pints/597-uspint-to-imperialpint/ | [
"# 597 US pints in imperial pints\n\n## Conversion\n\n597 US pints is equivalent to 497.106488223506 imperial pints.\n\n## Conversion formula How to convert 597 US pints to imperial pints?\n\nWe know (by definition) that: $1\\mathrm{uspint}\\approx 0.832674184628989\\mathrm{imperialpint}$\n\nWe can set up a proportion to solve for the number of imperial pints.\n\n$1 uspint 597 uspint ≈ 0.832674184628989 imperialpint x imperialpint$\n\nNow, we cross multiply to solve for our unknown $x$:\n\n$x\\mathrm{imperialpint}\\approx \\frac{597\\mathrm{uspint}}{1\\mathrm{uspint}}*0.832674184628989\\mathrm{imperialpint}\\to x\\mathrm{imperialpint}\\approx 497.10648822350646\\mathrm{imperialpint}$\n\nConclusion: $597 uspint ≈ 497.10648822350646 imperialpint$",
null,
"## Conversion in the opposite direction\n\nThe inverse of the conversion factor is that 1 imperial pint is equal to 0.00201164141625604 times 597 US pints.\n\nIt can also be expressed as: 597 US pints is equal to $\\frac{1}{\\mathrm{0.00201164141625604}}$ imperial pints.\n\n## Approximation\n\nAn approximate numerical result would be: five hundred and ninety-seven US pints is about four hundred and ninety-seven point one one imperial pints, or alternatively, a imperial pint is about zero times five hundred and ninety-seven US pints.\n\n## Footnotes\n\n The precision is 15 significant digits (fourteen digits to the right of the decimal point).\n\nResults may contain small errors due to the use of floating point arithmetic."
] | [
null,
"https://converter.ninja/images/597_uspint_in_imperialpint.jpg",
null
] | {"ft_lang_label":"__label__en","ft_lang_prob":0.7863752,"math_prob":0.99449265,"size":920,"snap":"2020-34-2020-40","text_gpt3_token_len":208,"char_repetition_ratio":0.16375546,"word_repetition_ratio":0.013333334,"special_character_ratio":0.23043478,"punctuation_ratio":0.09248555,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.990937,"pos_list":[0,1,2],"im_url_duplicate_count":[null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-09-30T19:19:17Z\",\"WARC-Record-ID\":\"<urn:uuid:0e4ecd94-759c-47ac-9db1-72e7451088e9>\",\"Content-Length\":\"18239\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e695ecd1-e2a5-4dd6-a91d-807df7c668ec>\",\"WARC-Concurrent-To\":\"<urn:uuid:2eb543e5-3b21-4ed5-ab9a-4487358c1bc9>\",\"WARC-IP-Address\":\"104.24.100.215\",\"WARC-Target-URI\":\"https://converter.ninja/volume/us-pints-to-imperial-pints/597-uspint-to-imperialpint/\",\"WARC-Payload-Digest\":\"sha1:I5MR5ODRZJFMY32WKEHQXAFM3OCCGRD4\",\"WARC-Block-Digest\":\"sha1:723IAJFKS7ANAYVGURZC2ADWYFN7L5ZD\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-40/CC-MAIN-2020-40_segments_1600402127397.84_warc_CC-MAIN-20200930172714-20200930202714-00584.warc.gz\"}"} |
https://chem.libretexts.org/Bookshelves/Organic_Chemistry/Supplemental_Modules_(Organic_Chemistry)/Chirality/Optical_Activity | [
"# Optical Activity\n\n$$\\newcommand{\\vecs}{\\overset { \\rightharpoonup} {\\mathbf{#1}} }$$ $$\\newcommand{\\vecd}{\\overset{-\\!-\\!\\rightharpoonup}{\\vphantom{a}\\smash {#1}}}$$$$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\id}{\\mathrm{id}}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$ $$\\newcommand{\\kernel}{\\mathrm{null}\\,}$$ $$\\newcommand{\\range}{\\mathrm{range}\\,}$$ $$\\newcommand{\\RealPart}{\\mathrm{Re}}$$ $$\\newcommand{\\ImaginaryPart}{\\mathrm{Im}}$$ $$\\newcommand{\\Argument}{\\mathrm{Arg}}$$ $$\\newcommand{\\norm}{\\| #1 \\|}$$ $$\\newcommand{\\inner}{\\langle #1, #2 \\rangle}$$ $$\\newcommand{\\Span}{\\mathrm{span}}$$\n\nOptical activity is an effect of an optical isomer's interaction with plane-polarized light.\n\n## Introduction\n\nOptical isomers, or enantiomers, have the same sequence of atoms and bonds but are different in their 3D shape. Two enantiomers are nonsuperimposible mirror images of one another (i.e., chiral), with the most common cited example being our hands. Our left hand is a mirror image of our right, yet there is no way our left thumb can be over our right thumb if our palms are facing the same way and placed over one another. Optical isomers also have no axis of symmetry, which means that there is no line that bisects the compound such that the left half is a mirror image of the right half.\n\nOptical isomers have basically the same properties (melting points, boiling points, etc.) but there are a few exceptions (uses in biological mechanisms and optical activity). There are drugs, called enantiopure drugs, that have different effects based on whether the drug is a racemic mixture or purely one enantiomer. For example, d-ethambutol treats tuberculosis, while l-ethambutol causes blindness. Optical activity is the interaction of these enantiomers with plane-polarized light.\n\n## A Brief History\n\nOptical activity was first observed by the French physicist Jean-Baptiste Biot. He concluded that the change in direction of plane-polarized light when it passed through certain substances was actually a rotation of light, and that it had a molecular basis. His work was supported by the experimentation of Louis Pasteur. Pasteur observed the existence of two crystals that were mirror images in tartaric acid, an acid found in wine. Through meticulous experimentation, he found that one set of molecules rotated polarized light clockwise while the other rotated light counterclockwise to the same extent. He also observed that a mixture of both, a racemic mixture (or racemic modification), did not rotate light because the optical activity of one molecule canceled the effects of the other molecule. Pasteur was the first to show the existence of chiral molecules.\n\n## Rotation of Light\n\nAn enantiomer that rotates plane-polarized light in the positive direction, or clockwise, is called dextrorotary [(+), or d-], while the enantiomer that rotates the light in the negative direction, or counterclockwise, is called levorotary [(-), or l-]. When both d- and l- isomers are present in equal amounts, the mixture is called a racemic mixture.",
null,
"image source\n\nIn the picture above, you can see that unpolarized light passes through a filter so that only waves that oscillate in a certain direction can pass through. When these waves interact with an optically active material, they are rotated either clockwise or counterclockwise, depending on the enantiomer. In the case of the image above, the light is rotated clockwise so the substance is the dextrorotary enantiomer.\n\n## Measuring Optical Activity\n\nOptical activity is measured by a polarimeter, and is dependent on several factors: concentration of the sample, temperature, length of the sample tube or cell, and wavelength of the light passing through the sample. Rotation is given in +/- degrees, depending on whether the sample has d- (positive) or l- (negative) enantiomers. The standard measurement for rotation for a specific chemical compound is called the specific rotation, defined as an angle measured at a path length of 1 decimeter and a concentration of 1g/ml. The specific rotation of a pure substance is an intrinsic property. In solution, the formula for specific rotation is:\n\n$[\\alpha]^T_\\lambda = \\dfrac{\\alpha}{I\\cdot c}$\n\nwhere\n\n• [α] is the specific rotation in degrees cm3 dm-1 g-1.\n• λ is the wavelength in nanometers,\n• α is the measured angle of rotation of a substance,\n• T is the temperature in degrees,\n• l is the path length in decimeters,\n• c is the concentration in g/ml, and\n\n## References\n\n1. Pettrucci, Ralph H., Harwood, Herring, Madura. General Chemistry: Principles and Modern Applications. 9th. Upper Saddle River: Pearson Prentice Hall, 2007.\n2. Raymond, Kenneth W. General Organic and Biological Chemistry. 3rd. Hoboken: John Wiley & Sons, Inc. 2010."
] | [
null,
"http://image.tutorvista.com/content/stereochemistry/polarization-plane.jpeg",
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https://affairscloud.com/machine-input-output-based-sbi-po-mains-set-29/ | [
"",
null,
"Machine Input-Output Based on SBI PO Mains – Set 29\n\nHello Aspirants.\n\nWelcome to Online Reasoning Section with explanation in AffairsCloud.com. Here we are creating Best question samples from Machine Input-output, which is common for all the IBPS, SBI , LIC, and other competitive exams. We have included questions that are repeatedly asked in bank exams !!!\n\nI. Study the following information carefully and answer the given questions.\nA number arrangement machine arranges two digit numbers into a typical manner. Each step takes gives output taking input from the previous step. The following is an illustration of Input and rearrangement. Using the illustration answer the question given below.\n\nExample:",
null,
"Input:",
null,
"",
null,
"Step I: Multiply the first digit of first number with second digit of fourth Number. Multiply the second digit of first number with first digit fourth number.\n\nStep II: Add the first digit of all numbers in Step I for the first number and second digit of all numbers in Step I for the second number\n\nStep III: Divide second digit by first digit\n\nStep IV: Second number is subtracted from the first number.\n\n1. If the value “5” is subtracted from the final output then what will be the resultant value?\nA. -1\nB. 1\nC. -11\nD. 11\nE. None of these\n\n2. If in the first step the first digit of every number is added and multiplied by 4 then which will be the resultant value?\nA. 56\nB. 60\nC. 52\nD. 64\nE. None of these\n\n3. Which of the following combinations represent the first digit of the second value and the second digit of the first value in Step I of the given input?\nA. 6, 4\nB. 4, 6\nC. 8, 2\nD. 2, 8\nE. 2, 4\n\n4. Which of the following represents the sum of the first digit of the second value and the second digit of the first value in Step II of the given input?\nA. 8\nB. 7\nC. 6\nD. 4\nE. 9\n\n5. Which of the following represents the difference between the first value and the second value of Step III of the given input?\nA. 8\nB. 7\nC. 9\nD. 4\nE. 6\n\nI. Study the following information carefully and answer the given questions.\nA number arrangement machine arranges two digit numbers into a typical manner. Each step takes gives output taking input from the previous step. The following is an illustration of Input and rearrangement. Using the illustration answer the question given below.\n\nExample:",
null,
"Input:",
null,
"",
null,
"Step I: Multiply the first digit of first number with second digit of fourth Number. Multiply the second digit of first number with first digit fourth number.\n\nStep II: Add the first digit of all numbers in Step I for the first number and second digit of all numbers in Step I for the second number and then multiply by 2.\n\nStep III: Divide second digit by first digit\n\n1. If the value “6” is added to the final output then what will be the resultant value?\nA. 12\nB. 13\nC. 10\nD. 11\nE. None of these\n\n2. If in the first step the second digit of every number is added and divided by 3 then which will be the resultant value?\nA. 5\nB. 6\nC. 2\nD. 4\nE. None of these\n\n3. Which of the following combinations represent the first digit of the third value and the second digit of the first value in Step I of the given input?\nA. 5, 1\nB. 1, 5\nC. 8, 6\nD. 6, 8\nE. 8, 8\n\n4. Which of the following represents the sum of the second digit of the second value and the first digit of the first value in Step II of the given input?\nA. 8\nB. 7\nC. 6\nD. 4\nE. 9"
] | [
null,
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null,
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null,
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null,
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null,
"https://affairscloud.com/assets/uploads/2017/06/question-two.jpg",
null,
"https://affairscloud.com/assets/uploads/2017/06/question-io.jpg",
null
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