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https://calculator.academy/land-to-building-ratio-calculator/ | [
"Enter the total square footage of the land parcel and the total square footage of the building to determine the land to building ratio.\n\n## Land to Building Ratio Formula\n\nThe following formula is used to calculate a land to building ratio:\n\nL:B = AL / AB\n\n• Where L:B is the land to building ratio\n• AL is the area of the land (ft^2)\n• AB is the area of the buildling (ft^2)\n\n## What is land to building ratio?\n\nDefinition:\n\nA land to building ratio is defined as the total square footage of a land parcel divided by the total area of the building footprint.\n\nThe land to building ratio is used in real estate to evaluate how much land is taken up by a building to determine if there is room for my development.\n\n## How to calculate a land to building ratio?\n\nExample Problem:\n\nThe following example outlines how to calculate a land to building ratio.\n\nFirst, determine the total square footage taken up by the building. In this case, the total land area is 5000 square feet.\n\nNext, determine the area of the entire lot. In this example, the entire lot of land is 10,000 square feet.\n\nFinally, calculate the land to building ratio using the formula above:\n\nL:B = AL / AB\n\nL:B = 10,000 / 5,000\n\nL:B = 2:1"
]
| [
null
]
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https://www.advanceexcelforum.com/excel-double-vlookup-iferror-vlookup/ | [
"# 03 Best Ways: EXCEL DOUBLE VLOOKUP/ IFERROR VLOOKUP/ NESTED VLOOKUP\n\n0\n\nDOUBLE VLOOKUP is a term in Advance Excel where two VLOOKUP functions nested with the IFERROR function to make a nested formula that sequentially works in two different tables or columns of the same workbook or different workbooks and retrieves the value. Thus, Excel Double VLOOKUP is often known as IFERROR VLOOKUP or NESTED VLOOKUP\n\nBroadly, NESTED VLOOKUP is an advanced level of DOUBLE VLOOKUP where two or more VLOOKUP functions work together with two or more IFERROR functions, making a nested formula that sequentially works in two or more different tables or columns of the same workbook or different workbooks. NESTED VLOOKUP is a kind of IFERROR VLOOKUP in Excel.\n\nThe IFERROR function is a logic function that checks a cell to determine if that cell contains an error or if a formula will result in an error. If no error exists, the function returns the value of the formula. If an error exists, the function returns an error.\n\nThe IFERROR function can’t distinguish the type of error. The error could be #NAME, #N/A, #REF, DIV/0, and so on. What is used as the value_if_error argument will be displayed regardless of the error type.\n\n# A. SIMPLE METHOD OF DOUBLE VLOOKUP / IFERROR VLOOKUP / NESTED VLOOKUP\n\nExcel Double VLOOKUP is a term where two VLOOKUP functions nested with the IFERROR function will make a unique formula, that is able to match the lookup_value in two different columns. It is also known as IFERROR VLOOKUP or NESTED VLOOKUP.\n\nThe logic behind the Excel DOUBLE VLOOKUP formula or IFERROR VLOOKUP formula is that when the first VLOOKUP fails to find the lookup_value in the first column range returns an Error, then the IFERROR function replaces the Error with the second VLOOKUP function which finds the same lookup_value in the second column range and retrieves the value.\n\nAs a result, with a single formula, we can retrieve the value matches with two different columns.\n\n➢ SYNTAX:\n\n➢ STEPS TO START:\n\n=IFERROR(VLOOKUP(\\$G3,\\$B\\$3:\\$D\\$12,3,0), (VLOOKUP(\\$G3,\\$C\\$3:\\$D\\$12,2,0)))\n\n• STEP 1: Select a cell to get the result of Double VLOOKUP (i.e., H3).\n\nIn this cell, place an equality “=” sign to start the formula and just type a few letters ‘=IF….‘ and select the IFERROR function from the Excel provided suggestion list with the help of a down arrow (↓) key, if required.",
null,
"Then press the ‘Tab’ key, IFERROR syntax appears with the open parenthesis.",
null,
"The IFERROR function has 2 arguments: value and value_if_error.\n\n• Value is the expression being tested.\n\n• Value_if_error is the text that will be returned if there is an error in the formula (or expression).\n\nWe place the first VLOOKUP in the value position and place the second VLOOKUP in the value_if_error position. Therefore, the new formula works in such a way, if the first VLOOKUP returns any #N/A error, it will be replaced by the value of the second VLOOKUP.\n\n• STEP 2: Then type a few letters of vlookup such as ‘=vlo….’ and select the VLOOKUP function from the given suggestion list.",
null,
"Then press the ‘Tab’ key, VLOOKUP syntax appears with the open parenthesis within the IFERROR function.",
null,
"• STEP 3: The first VLOOKUP retrieves the value from a first table_array, likes\n\n=IFERROR( VLOOKUP( \\$G3, \\$B\\$3:\\$D\\$12, 3, 0),\n\n➢ \\$G3 – select the lookup value locates in cell G3 (i.e., CAN-1) and fix the Column address by pressing the F4 key thrice. Thus the range converts from the relative to the mixed cell reference where it indicates the absolute column and relative row.\n\nAs a result, while the formula is copied to the right side or horizontally, the column address does not change but the row address changes accordingly.\n\n➢ \\$B\\$3:\\$D\\$12 lookup_value found in the range is called lookup_array and fixed the range by pressing the F4 key once. Thus the range is converted to absolute from the relative cell reference.\n\nAs a result, the range does not change when the formula is copied to another cell either horizontally or vertically.\n\n➢ 3 – the column_index_num is the count of columns between the lookup value column and the return value column.\n\n➢ 0 – the last argument of the VLOOKUP function is range_lookup. If we are looking for an exact match, place either 0 or FALSE.\n\n■ Note: We had detail explained on Cell Reference in a separate tutorial. Request you read this tutorial: 03 Types of Excel Cell Reference: Relative, Absolute & Mixed\n\n• STEP 4: When the first VLOOKUP formula cannot find a match, it returns the #N/A error (i.e., lookup_value does not find a match in the first column of table_array).\n\nThen the wrapped IFERROR function to replace the #N/A error either with the ‘values’ or ‘suggested texts’. We should place the texts in double quotation marks (” “).\n\nBut here the #N/A error is replaced with the values, those values are getting from the Second VLOOKUP.\n\nWe should place the second VLOOKUP in place of value_if_error, the second argument of the IFERROR function. Then, we write the formula as:\n\n=IFERROR(VLOOKUP(\\$G3, \\$B\\$3:\\$D\\$12, 3, 0), (VLOOKUP(\\$G3, \\$C\\$3:\\$D\\$12, 2, 0)))\n\n➢ \\$G3 – as the same as first Lookup, select the lookup value locates in cell G3 (i.e., CAN-1) and fix the Column address by pressing the F4 key thrice. Thus the range converts from the relative to the mixed cell reference where it indicates the absolute column and relative row.\n\nAs a result, while the formula is copied to the right side or horizontally, the column address does not change but the row address changes accordingly.\n\n\\$C\\$3:\\$D\\$12 – lookup_value found in the range is called lookup_array and in this case, lookup_array should be different from the first lookup_array.\n\nFixed the range by pressing the F4 key once. Thus the range is converted from the relative cell reference to the absolute.\n\nAs a result, the range does not change when the formula is copied to another cell either horizontally or vertically.\n\n➢ 2 – the column_index_num is the count of columns between the lookup value column and the return value column.\n\n0 – the last argument of the VLOOKUP function is range_lookup. If we are looking for an exact match we put either 0 or FALSE.\n\n• STEP 5: Finally, press Enter to accept the formula. Formula ends by default and closes the last parenthesis as well.\n\n• STEP 6: EXTEND THE FORMULA TILL THE END OF THE RANGE (WITHOUT FORMATTING)\n\nCopy (Ctrl+C) the cell with formula Select the range of cells where to copy the formula (Shift+Down Arrow) Press either Alt+E+S+R (press sequentially, Alt, E, S, R) or Alt+Ctrl+V+R (press Alt+Ctrl+V, then R) which will select the “Formulas and number formats” in the Paste Special dialog box Then press Enter or click OK.",
null,
"• STEP 7: OBSERVATIONS",
null,
"In the Excel double VLOOKUP two ranges are used for retrieving data: one is the range B3:D12 and the second one is C3:D12.\n\n(01). In the first case, the lookup_value is CAN-1 and the Excel Double VLOOKUP returns the result value CAN-124 as a Number Code (UN). The lookup_value found in the range C3:D12.\n\n(02). In the second case, the lookup_value is IN-91 and the Excel Double VLOOKUP returns the result value IND-356 as a Number Code (UN). The lookup_value found in the different range B3:D12.\n\n(03). In the third case, the lookup_value is USA-840 and the Excel Double VLOOKUP returns the #N/A error. That means the lookup_value does not exist either in range C3:D12 or B3:D12.\n\n(04). In the fourth case, using another IFERROR function to replace the #N/A error with a text likes “Not Found”. The text should be in double quotation. We can keep it blanks ” ” instead of a text.\n\n# B. ADVANCED METHOD OF DOUBLE VLOOKUP / IFERROR VLOOKUP / NESTED VLOOKUP\n\nNested VLOOKUP in Excel is an advanced level of multiple VLOOKUP functions in the IFERROR functions, where individual VLOOKUP function finds the match from the suggested table array and retrieves the value. If the VLOOKUP function fails to match, it returns a #N/A error.\n\nThe IFERROR function in Excel allows replacing the #N/A error with suggested ‘value’ or ‘text’. To make the formula more dynamic, rather than put any value manually replaces it with the second VLOOKUP. Similarly, the second VLOOKUP formula finds the match from another table array and retrieves the value. If it fails to find the match, it returns a #N/A error.\n\nAgain and again, apply the IFERROR function to replace the #N/A error by third, fourth, fifth,…returns by the VLOOKUP functions. The combination of multiple IFERROR and VLOOKUP functions makes a formula that allows to sequential lookup with first table array, second table array, third.., fourth…so on.\n\nThe advanced method of using the IFERROR VLOOKUP in Excel is called the Advanced Double VLOOKUP or Advanced Nested VLOOKUP or Advanced IFERROR VLOOKUP\n\n➢ SYNTAX:",
null,
"➢ STEPS TO START:\n\n=IFERROR(VLOOKUP(\\$G3,\\$B\\$3:\\$D\\$12,3,0), IFERROR(VLOOKUP(\\$G3,\\$C\\$3:\\$D\\$12,2,0), VLOOKUP(\\$G3,\\$D\\$3:\\$D\\$12,1,0)))\n\n• STEP 1: Select the cell to get the result of Advanced Double VLOOKUP (i.e., H3).\n\nIn this cell, press equality “=” sign to start formula and just type a few letters of IFERROR e.g., =if…. and select the IFERROR function from the Excel provided suggestion list with the help of a down arrow (↓), if required.",
null,
"Then press the ‘Tab’ key, IFERROR syntax appears with the open parenthesis.",
null,
"The IFERROR function has two arguments: value and value_if_error.\n\nWe put the first VLOOKUP in place of the value argument and put the second VLOOKUP in place of the value_if_error argument. So, the new formula works in such a way, if the first VLOOKUP returns any #N/A error, it will be replaced by the value of the second VLOOKUP.\n\n• STEP 2: Then type a few letters of the VLOOKUP, for example, =vlo… and select the VLOOKUP function from the Excel provided suggestion list.",
null,
"Then press the ‘Tab’ key, VLOOKUP syntax appears with the open parenthesis within the IFERROR function.",
null,
"• STEP 3: The first VLOOKUP retrieves the value from a first table_array. This formula allows retrieving the values against match cases and returns the #N/A errors in non-match cases.\n\nIn this case, we wrap the formula with another IFERROR function to replace the #N/A error. The #N/A error should be replaced with the value, this value comes from the Second VLOOKUP.\n\nIf the second VLOOKUP formula fails to find the match from the range, it returns the #N/A error. This error is replaced by the value of the third VLOOKUP\n\nThe position of the first VLOOKUP in place of the ‘value’ argument of the first IFERROR function and in place of the ‘value_if_error’ argument puts the second IFERROR function. The position of the second VLOOKUP and third VLOOKUP in place of the ‘value’ and ‘value_if_error’ arguments in the second IFERROR function, respectively.\n\nTherefore, now the formula works in such a way, if the first VLOOKUP returns any #N/A error, the second VLOOKUP replaces the error with the value. If the second VLOOKUP returns any #N/A error, it will be replaced by the value of the third VLOOKUP.\n\n=IFERROR(VLOOKUP(\\$G3,\\$B\\$3:\\$D\\$12,3,0), IFERROR(VLOOKUP(\\$G3,\\$C\\$3:\\$D\\$12,2,0), VLOOKUP(\\$G3,\\$D\\$3:\\$D\\$12,1,0)))\n\n➢ \\$G3 – the lookup value locates in cell G3 (i.e., CAN-1) and same for the first, the second and the third VLOOKUP function.\n\nFix the Column address by pressing three times the F4 key. Thus the range converts from the relative to the mixed cell reference where it indicates the absolute column and relative row.\n\nAs a result, while the formula is copied to the right side or horizontally, the column address does not change but the row address changes accordingly.\n\n\\$B\\$3:\\$D\\$12lookup_array for the first VLOOKUP (lookup_array is the range where lookup_value is found).\n\n\\$C\\$3:\\$D\\$12lookup_array for the second VLOOKUP.\n\n\\$D\\$3:\\$D\\$12lookup_array for the third VLOOKUP.\n\nFixed every range by pressing the F4 key once. Thus the range is converted to absolute from the relative cell reference.\n\nAs a result, the range does not change when the formula is copied to another cell either horizontally or vertically.\n\n➢ 3 – column_index_num for the first VLOOKUP (the column_index_num is the count of columns between the lookup value column and the return value column.\n\n2 – column_index_num for the second VLOOKUP.\n\n1 column_index_num for the third VLOOKUP.\n\n➢ 0 – the last argument of the VLOOKUP function is range_lookup. We are looking for an exact match, so we put either 0 or FALSE. So, range_lookup is the same for three VLOOKUP functions.\n\n• STEP 4: Finally, press Enter to accept the formula. Formula ends by default and closes the last parenthesis as well.\n\n• STEP 5: EXTEND THE FORMULA TILL THE END OF THE RANGE (WITHOUT FORMATTING)\n\nCopy (Ctrl+C) the cell with formula Select the range of cells where to copy the formula (Shift+Down Arrow) Press either Alt+E+S+R (press sequentially, Alt, E, S, R) or Alt+Ctrl+V+R (press Alt+Ctrl+V, then R) which will select the “Formulas and number formats” in the Paste Special dialog box Then press Enter or click OK.\n\n# C. DYNAMIC METHOD OF DOUBLE VLOOKUP / IFERROR VLOOKUP / NESTED VLOOKUP\n\nUsing of MATCH function in the Advanced Double VLOOKUP (or Advanced Nested VLOOKUP or Advanced IFERROR VLOOKUP) makes it dynamic formula.\n\nThe MATCH() function returns the position of an item within an array that matches a specific value.\n\nUsing the MATCH() function in place of column_index_num automatically updates the column number that makes the dynamic formula.\n\nThe Syntax of the MATCH function is as follows:",
null,
"➢ Lookup_value is the item to match. It can be a number, text string, a logical value, or a reference.\n\n➢ Lookup_array is the table or an array containing all of the values to search.\n\n➢ Match_type is a number that specifies how the match will be applied.\n\nA match_type of zero (0) finds the first item in the array that is an exact match with the lookup_value.\n\nTo find the item closest to but less than the lookup_value, use a match_type of -1.\n\nTo find the item closest to but greater than the lookup_value, use a match_type of 1.\n\nIn the last two cases, the values in the lookup_array must be in ascending order for the MATCH function to work correctly.\n\nThe match_type is optional and will default to 1 if omitted from the arguments\n\n➢ SYNTAX:",
null,
"➢ STEPS TO START:\n\n• STEP 1: Select the cell to get the result of Advanced Double VLOOKUP (i.e., H3).\n\nIn this cell, press equality “=” sign to start formula and just type a few letters of IFERROR e.g., =if…. and select the IFERROR function from the Excel provided suggestion list with the help of a down arrow (↓), if required.",
null,
"Then press the ‘Tab’ key, the IFERROR syntax appears with the open parenthesis.",
null,
"The IFERROR function has two arguments: value and value_if_error.\n\nWe put the first VLOOKUP in place of the value argument and put the second VLOOKUP in place of the value_if_error argument. So, the new formula works in such a way, if the first VLOOKUP returns any #N/A error, it will be replaced by the value of the second VLOOKUP.\n\n• STEP 2: Then type a few letters of the VLOOKUP, for example, =vlo… and select the VLOOKUP function from the Excel provided suggestion list.",
null,
"Then press the ‘Tab’ key, VLOOKUP syntax appears with the open parenthesis within the IFERROR function.",
null,
"• STEP 3: The position of the first VLOOKUP in place of the ‘value’ argument of the first IFERROR function and in place of the ‘value_if_error‘ argument puts the second IFERROR function. The position of the second VLOOKUP and third VLOOKUP in place of the ‘value‘ and ‘value_if_error‘ arguments in the second IFERROR function, respectively.\n\nSo, the formula works in such a way, if the first VLOOKUP returns any #N/A error, the second VLOOKUP replaces the error with the value. If the second VLOOKUP returns any #N/A error, it will be replaced by the value of the third VLOOKUP.\n\n=IFERROR(VLOOKUP(\\$G3,\\$B\\$3:\\$D\\$12, MATCH(H\\$2,\\$B\\$2:\\$D\\$2,0),0),\n\nIFERROR(VLOOKUP(\\$G3,\\$C\\$3:\\$D\\$12, MATCH(H\\$2,\\$C\\$2:\\$D\\$2,0),0),\n\nVLOOKUP(\\$G3,\\$D\\$3:\\$D\\$12, MATCH(H\\$2,\\$D\\$2:\\$D\\$2,0),0)))\n\n➢ EXPLANATION OF THE FIRST VLOOKUP FUNCTION:\n\nVLOOKUP(\\$G3,\\$B\\$3:\\$D\\$12, MATCH(H\\$2,\\$B\\$2:\\$D\\$2,0),0)\n\n• \\$G3 – the lookup value locates in cell G3 (i.e., CAN-1) and the same for the first, the second and the third VLOOKUP function.\n\nFix the Column address by pressing the F4 key thrice. Thus the range converts from the relative to the mixed cell reference where it indicates the absolute column and relative row.\n\nAs a result, while the formula is copied to the right side or horizontally, the column address does not change but the row address changes accordingly.\n\n• \\$B\\$3:\\$D\\$12 – lookup_array for the first VLOOKUP (lookup_array is the range where lookup_value is found).\n\n• MATCH(H\\$2,\\$B\\$2:\\$D\\$2,0) – we place the MATCH() function in place of column_index_num to update the column number automatically. Please note that the lookup column in both the lookup_array of the VLOOKUP function and the lookup_array of the MATCH function should be the same. Otherwise, the formula returns the #N/A error. In both cases, Column B is the lookup column.\n\n• H\\$2 = lookup_value reference to ‘Number Code (UN)’ and fixed the row address by pressing two times F4 Key. As a result, the lookup_value is converted from the relative cell reference to the mixed column cell reference, where it indicates the relative column and absolute row address.\n\nAs a result, while the formula is copied to the other cells, the row address does not change but the column address changes accordingly.\n\n• \\$B\\$2:\\$D\\$2 = lookup_value found in the range is called lookup_array and fixed the range by pressing a single time F4 key. Thus the range is converted from the relative cell reference to the absolute cell reference.\n\nAs a result, the range does not change when the formula is copied to another cell either horizontally or vertically.\n\n• 0 = for exact match\n\n• 0 – range_lookup the last argument of VLOOKUP function. The value zero (0) or FALSE signifies the exact match.\n\n➢ EXPLANATION OF THE SECOND VLOOKUP FUNCTION:\n\nVLOOKUP(\\$G3, \\$C\\$3:\\$D\\$12, MATCH(H\\$2,\\$C\\$2:\\$D\\$2,0), 0)\n\nWe should follow the same steps described in the first VLOOKUP function.\n\n➢ EXPLANATION OF THE THIRD VLOOKUP FUNCTION:\n\nVLOOKUP(\\$G3,\\$D\\$3:\\$D\\$12, MATCH(H\\$2,\\$D\\$2:\\$D\\$2,0),0)\n\nWe should follow the same steps described in the first VLOOKUP function.\n\n• STEP 4: Finally, press Enter to accept the formula. Formula ends by default and closes the last parenthesis as well.\n\n• STEP 5: EXTEND THE FORMULA TILL THE END OF THE RANGE (WITHOUT FORMATTING)\n\nCopy (Ctrl+C) the cell with formula Select the range of cells where to copy the formula (Shift+Down Arrow) Press either Alt+E+S+R (press sequentially, Alt, E, S, R) or Alt+Ctrl+V+R (press Alt+Ctrl+V, then R) which will select the “Formulas and number formats” in the Paste Special dialog box Then press Enter or click OK.\n\n# D. CONCLUSION\n\n(01). Excel Double VLOOKUP (or IFERROR VLOOKUP or Nested VLOOKUP) is the most important formulas in Advance Excel. The formula helps to reduce the time span in data analysis.\n\n(02). Multiple VLOOKUPS nested with IFERROR function make an advanced formula in Advance Excel that works sequentially in two or more tables or columns in the same workbook or the different workbooks.\n\n(03). Using of MATCH function in Advanced Double VLOOKUP (or Advanced Nested VLOOKUP or Advanced IFERROR VLOOKUP) makes it a dynamic formula.",
null,
"If you would like to improve your academic and professional career as well, then the below courses help you a lot. Instead of Advanced Excel, a number of best courses suggested you through this platform that boosts your confidence and flies your career high.",
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]
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null,
"https://www.advanceexcelforum.com/wp-content/uploads/2019/10/Observations-of-Simple-DOUBLE-VLOOKUP-or-IFERROR-VLOOKUP-or-NESTED-VLOOKUP-1024x265.png",
null,
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null,
"https://www.advanceexcelforum.com/wp-content/uploads/2019/10/Syntax-of-Dynamic-DOUBLE-VLOOKUP-or-IFERROR-VLOOKUP-or-NESTED-VLOOKUP-1024x693.png",
null,
"https://www.advanceexcelforum.com/wp-content/uploads/2019/10/IFERROR-Syntax.png",
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https://discuss.codechef.com/t/regarding-codechef-problems/376 | [
"",
null,
"# Regarding Codechef Problems\n\nI tried to solve below problems and I have written cod in PHP. Can you tell me why it is giving me wrong answer. I want to know where I am being wrong or what I am doing wrong.\n\nMy Submitted Code for above problem in PHP as below.\n\n``````//Suppose below are my posted array\n\n\\$nTimeMul = array(4,9);\n\\$nToAppear = array(2,3);\nfunction getDezireOutput(\\$nTimeMul = array(), \\$nToAppear = array()) {\n\\$i = 0;\nforeach (\\$nTimeMul as \\$num) {\n\\$tempNum = 1;\nfor (\\$t=0; \\$t < \\$num; \\$t++) {\n\n\\$tempNum = \\$tempNum * \\$num;\n}\necho substr (\\$tempNum, 0, \\$nToAppear[\\$i]).' '.substr (\\$tempNum, -\\$nToAppear[\\$i]).'\n``````\n\n';\n\\$i++;\n}\n}\ngetDezireOutput (\\$nTimeMul, \\$nToAppear);\n\nPlease have look into above problem and let me know the problems with above code so, I can figure it out."
]
| [
null,
"https://s3.amazonaws.com/discourseproduction/original/3X/2/6/26ff6c8c380a45aa03cbe51d74b4b0f9fd44daa9.svg",
null
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https://web2.0calc.com/questions/probability_30746 | [
"+0\n\n# Probability\n\n0\n33\n1\n\nA positive integer divisor of 11 is chosen at random. What is the probability that this divisor is prime? Express your answer as a common fraction.\n\nJul 12, 2022\n\nIt is $$\\frac{1}{2},$$ since 11 has only two divisors, 1 and 11, and 11 is prime while 1 is not."
]
| [
null
]
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https://www.teachoo.com/8083/2629/Example-13/category/Addition-of-decimal-numbers/ | [
"Chapter 8 Class 6 Decimals\nConcept wise",
null,
"",
null,
"Learn in your speed, with individual attention - Teachoo Maths 1-on-1 Class\n\n### Transcript\n\nExample 3 Samson travelled 5 km 52 m by bus, 2 km 265 m by car and the rest 1km 30 m he walked. How much distance did he travel in all? Distance travelled by bus = 5 km 52 m Distance travelled by car = 2 km 265 m Distance travelled by foot = 1 km 30 m Total distance travelled = 5 km 52 m + 2 km 265 m + 1 km 30 m = (5 km + 52 m) + (2 km + 265 m) + (1 km + 30 m) = (5 km + 2 km + 1 km) + (52 m + 265 m + 30 m) = 8 km + 347 m = 8 km 347 m = 8 km 347 m Converting to decimals = 8 km + 347 m = 8 km + 347 × 1 m = 8 km + 347 × 1/1000 km = 8 km + 347/1000 km = (8+347/1000) km = ((8 × 1000 + 347)/1000) km = ((8000 + 347)/1000) km = 8347/1000 km = 8.347 km ∴ Total distance = 8.347 km",
null,
""
]
| [
null,
"https://d1avenlh0i1xmr.cloudfront.net/3eeb9bd2-7fbe-410b-a205-b22cc0e3ec59/slide28.jpg",
null,
"https://d1avenlh0i1xmr.cloudfront.net/affefde0-b93c-4808-951c-2f85de4f9ff9/slide29.jpg",
null,
"https://www.teachoo.com/static/misc/Davneet_Singh.jpg",
null
]
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https://inches-to-mm.appspot.com/pl/1281-cal-na-milimetr.html | [
"Inches To Mm\n\n# 1281 in to mm1281 Inch to Millimeters\n\nin\n=\nmm\n\n## How to convert 1281 inch to millimeters?\n\n 1281 in * 25.4 mm = 32537.4 mm 1 in\nA common question is How many inch in 1281 millimeter? And the answer is 50.4330708662 in in 1281 mm. Likewise the question how many millimeter in 1281 inch has the answer of 32537.4 mm in 1281 in.\n\n## How much are 1281 inches in millimeters?\n\n1281 inches equal 32537.4 millimeters (1281in = 32537.4mm). Converting 1281 in to mm is easy. Simply use our calculator above, or apply the formula to change the length 1281 in to mm.\n\n## Convert 1281 in to common lengths\n\nUnitUnit of length\nNanometer32537400000.0 nm\nMicrometer32537400.0 µm\nMillimeter32537.4 mm\nCentimeter3253.74 cm\nInch1281.0 in\nFoot106.75 ft\nYard35.5833333334 yd\nMeter32.5374 m\nKilometer0.0325374 km\nMile0.020217803 mi\nNautical mile0.0175687905 nmi\n\n## What is 1281 inches in mm?\n\nTo convert 1281 in to mm multiply the length in inches by 25.4. The 1281 in in mm formula is [mm] = 1281 * 25.4. Thus, for 1281 inches in millimeter we get 32537.4 mm.\n\n## 1281 Inch Conversion Table",
null,
"## Alternative spelling\n\n1281 Inch to Millimeters, 1281 Inch in Millimeters, 1281 Inches to Millimeter, 1281 Inches in mm, 1281 Inch to Millimeter, 1281 Inch in Millimeter, 1281 in in Millimeter, 1281 in in Millimeters,"
]
| [
null,
"https://inches-to-mm.appspot.com/image/1281.png",
null
]
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http://ixtrieve.fh-koeln.de/birds/litie/document/27790 | [
"# Document (#27790)\n\nAuthor\nRinn, R.\nWerner, C.\nTitle\n¬Der Neuerscheinungsdienst Der Deutschen Bibliothek : Eine Bilanz nach eineinhalb Jahren\nSource\nDialog mit Bibliotheken. 16(2004) H.2, S.47-51\nYear\n2004\nAbstract\nMit der Auslieferung der ersten Ausgabe im Januar 2003 löste der Neuerscheinungsdienst (ND) Der Deutschen Bibliothek den CIP-Dienst ab. Über die Gründe für die Neukonzeption der Dienstleistungen bezüglich der Vorankündigungen, über die Ziele und die Funktion des neuen Dienstes sowie über seine ersten Ausgaben wurde bereits im Detail berichtet\". Nur soviel sei in Erinnerung gerufen: Die Deutsche Bibliothek bietet neben ihren anderen Dienstleistungen nun je einen auf die jeweilige Funktion zugeschnittenen Spezialdienst für Erwerbung bzw. Katalogisierung an: Für Erwerbungszwecke ist dies der Neuerscheinungsdienst, der die Verlegermeldungen anzeigt, die parallel dazu auch in das VLB aufgenommen werden. Die Titeldaten der Verleger werden in Der Deutschen Bibliothek mit Sachgruppen versehen, ansonsten aber nicht weiter bearbeitet. Sie enthalten keine hierarchischen Verknüpfungen und ihre Personen- oder Körperschaftseintragungen sind nicht mit den entsprechenden Normdateien PND und GKD verknüpft. Die Daten sind insoweit standardisiert, als dies von dem für die VLB-Meldungen verwendeten ONIX-Format verlangt wird und sie dem Regelwerk des VLB entsprechen, und unter bibliothekarischen Gesichtspunkten teilweise von heterogener Qualität. Für Katalogisierungszwecke werden natürlich weiterhin die Daten der Reihen A, B und C der Deutschen Nationalbibliografie für Eigenkatalogisierung angeboten, deren »autopsierte« Daten nationalbibliografisch autorisiert sind und als endgültige Katalogisate ohne weitere Korrekturen übernommen werden können. Diese beiden Dienste ergänzen sich gegenseitig und sie beide, nicht der Neuerscheinungsdienst allein, sind als funktionale Nachfolger des CIP-Dienstes anzusehen. Um die Nutzbarkeit der beiden Dienste weiter zu verbessern, hat Die Deutsche Bibliothek in den vergangenen eineinhalb Jahren eine ganze Reihe von Maßnahmen ergriffen, auf die hier näher eingegangen werden soll. Dabei sind vor allem auch Anregungen und Kritik berücksichtigt worden, die verschiedene Dienstleistungsbezieher zu den ersten Ausgaben des Neuerscheinungsdienstes dankenswerterweise geäußert haben. Die wichtigsten Einzelpunkte sind im Folgenden vorangestellt. Die statistischen Angaben beziehen sich auf das Jahr 2003, in dem insgesamt ca. 94.000 Titelmeldungen im Neuerscheinungsdienst angezeigt worden sind. - Bereits in der Deutschen Nationalbibliografie angezeigte Titel werden nochmals im ND angezeigt: Durch einen Dublettencheck werden seit März 2003 bereits in der Datenbank Der Deutschen Bibliothek vorhandene Titel erkannt und nicht mehr in den ND übernommen. - Es werden vermehrt Titel ausländischer Verlage ohne deutschen Verlagssitz angezeigt: So genannte NSG-Titel, d. h. Titel, die nicht in das Sammelgebiet Der Deutschen Bibliothek gehören, werden nicht übernommen, soweit sie als solche erkennbar sind. Dazu zählen auch alle Titel von ausländischen Verlagen ohne deutschen Verlagssitz. Zur Information sei erwähnt, dass von den 2003 im ND angezeigten Titeln 96 % eine ISBN mit der Länderkennzeichnung »3-« hatten.\nTheme\nBibliographie\nObject\nDNB-ND\nCIP\nLocation\nD\n\n## Similar documents (author)\n\n1. Rinn, R.: Vom CIP- zum Neuerscheinungsdienst (2003) 2.14\n```2.142108 = sum of:\n2.142108 = product of:\n4.284216 = sum of:\n4.284216 = weight(author_txt:rinn in 992) [ClassicSimilarity], result of:\n4.284216 = score(doc=992,freq=1.0), product of:\n0.7710363 = queryWeight, product of:\n1.1003704 = boost\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.07881691 = queryNorm\n5.5564384 = fieldWeight in 992, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.625 = fieldNorm(doc=992)\n0.5 = coord(1/2)\n```\n2. Rinn, R.: ¬Die Normdatei für Personennamen : PND (1995) 2.14\n```2.142108 = sum of:\n2.142108 = product of:\n4.284216 = sum of:\n4.284216 = weight(author_txt:rinn in 2194) [ClassicSimilarity], result of:\n4.284216 = score(doc=2194,freq=1.0), product of:\n0.7710363 = queryWeight, product of:\n1.1003704 = boost\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.07881691 = queryNorm\n5.5564384 = fieldWeight in 2194, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.625 = fieldNorm(doc=2194)\n0.5 = coord(1/2)\n```\n3. Rinn, R.: ¬Die Personennamendatei (PND) (1993) 2.14\n```2.142108 = sum of:\n2.142108 = product of:\n4.284216 = sum of:\n4.284216 = weight(author_txt:rinn in 4356) [ClassicSimilarity], result of:\n4.284216 = score(doc=4356,freq=1.0), product of:\n0.7710363 = queryWeight, product of:\n1.1003704 = boost\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.07881691 = queryNorm\n5.5564384 = fieldWeight in 4356, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.625 = fieldNorm(doc=4356)\n0.5 = coord(1/2)\n```\n4. Rinn, R.: ¬Das Projekt Personennamendatei : PND-Projekt (1994) 2.14\n```2.142108 = sum of:\n2.142108 = product of:\n4.284216 = sum of:\n4.284216 = weight(author_txt:rinn in 6568) [ClassicSimilarity], result of:\n4.284216 = score(doc=6568,freq=1.0), product of:\n0.7710363 = queryWeight, product of:\n1.1003704 = boost\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.07881691 = queryNorm\n5.5564384 = fieldWeight in 6568, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.625 = fieldNorm(doc=6568)\n0.5 = coord(1/2)\n```\n5. Rinn, R.: ¬Die überregionale Normdatei für Personennamen (PND) : Bericht zum Projektstand September 1995 (1995) 2.14\n```2.142108 = sum of:\n2.142108 = product of:\n4.284216 = sum of:\n4.284216 = weight(author_txt:rinn in 2771) [ClassicSimilarity], result of:\n4.284216 = score(doc=2771,freq=1.0), product of:\n0.7710363 = queryWeight, product of:\n1.1003704 = boost\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.07881691 = queryNorm\n5.5564384 = fieldWeight in 2771, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n8.890302 = idf(docFreq=15, maxDocs=42740)\n0.625 = fieldNorm(doc=2771)\n0.5 = coord(1/2)\n```\n\n## Similar documents (content)\n\n1. 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Heiner-Freiling, M.: DDC in der Deutschen Nationalbibliografie (2003) 0.47\n```0.46667176 = sum of:\n0.46667176 = product of:\n0.9722329 = sum of:\n0.026958628 = weight(abstract_txt:auch in 2954) [ClassicSimilarity], result of:\n0.026958628 = score(doc=2954,freq=4.0), product of:\n0.065436125 = queryWeight, product of:\n3.7667098 = idf(docFreq=2686, maxDocs=42740)\n0.017372224 = queryNorm\n0.41198388 = fieldWeight in 2954, product of:\n2.0 = tf(freq=4.0), with freq of:\n4.0 = termFreq=4.0\n3.7667098 = idf(docFreq=2686, maxDocs=42740)\n0.0546875 = fieldNorm(doc=2954)\n0.030432817 = weight(abstract_txt:deutsche in 2954) [ClassicSimilarity], result of:\n0.030432817 = score(doc=2954,freq=1.0), product of:\n0.098379225 = queryWeight, product of:\n1.0011457 = boost\n5.6565375 = idf(docFreq=405, maxDocs=42740)\n0.017372224 = queryNorm\n0.3093419 = fieldWeight in 2954, product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n5.6565375 = idf(docFreq=405, maxDocs=42740)\n0.0546875 = 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product of:\n1.0 = tf(freq=1.0), with freq of:\n1.0 = termFreq=1.0\n3.9433165 = idf(docFreq=2251, maxDocs=42740)\n0.0546875 = fieldNorm(doc=2954)\n0.057385135 = weight(abstract_txt:werden in 2954) [ClassicSimilarity], result of:\n0.057385135 = score(doc=2954,freq=3.0), product of:\n0.17188527 = queryWeight, product of:\n2.807186 = boost\n3.524618 = idf(docFreq=3422, maxDocs=42740)\n0.017372224 = queryNorm\n0.3338572 = fieldWeight in 2954, product of:\n1.7320508 = tf(freq=3.0), with freq of:\n3.0 = termFreq=3.0\n3.524618 = idf(docFreq=3422, maxDocs=42740)\n0.0546875 = fieldNorm(doc=2954)\n0.1789168 = weight(abstract_txt:titel in 2954) [ClassicSimilarity], result of:\n0.1789168 = score(doc=2954,freq=2.0), product of:\n0.366837 = queryWeight, product of:\n3.3484418 = boost\n6.3063045 = idf(docFreq=211, maxDocs=42740)\n0.017372224 = queryNorm\n0.48772833 = fieldWeight in 2954, product of:\n1.4142135 = tf(freq=2.0), with freq of:\n2.0 = termFreq=2.0\n6.3063045 = idf(docFreq=211, maxDocs=42740)\n0.0546875 = fieldNorm(doc=2954)\n0.14575695 = weight(abstract_txt:deutschen in 2954) [ClassicSimilarity], result of:\n0.14575695 = score(doc=2954,freq=2.0), product of:\n0.36628768 = queryWeight, product of:\n4.097915 = boost\n5.1452193 = idf(docFreq=676, maxDocs=42740)\n0.017372224 = queryNorm\n0.39793023 = fieldWeight in 2954, product of:\n1.4142135 = tf(freq=2.0), with freq of:\n2.0 = termFreq=2.0\n5.1452193 = idf(docFreq=676, maxDocs=42740)\n0.0546875 = fieldNorm(doc=2954)\n0.48 = coord(12/25)\n```"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.6659812,"math_prob":0.99710107,"size":32524,"snap":"2020-45-2020-50","text_gpt3_token_len":12662,"char_repetition_ratio":0.26666668,"word_repetition_ratio":0.57846713,"special_character_ratio":0.5437523,"punctuation_ratio":0.28357604,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9998333,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-11-26T12:26:50Z\",\"WARC-Record-ID\":\"<urn:uuid:151d942a-28ae-48b4-bed7-061f33856153>\",\"Content-Length\":\"55719\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:5fb1a2dd-4049-492f-ad9b-ed3ddf1021d9>\",\"WARC-Concurrent-To\":\"<urn:uuid:0253d6bd-d5ff-4391-b0df-8b4685be6013>\",\"WARC-IP-Address\":\"139.6.160.6\",\"WARC-Target-URI\":\"http://ixtrieve.fh-koeln.de/birds/litie/document/27790\",\"WARC-Payload-Digest\":\"sha1:LO5LWAHOZUGXKTGZWDMECJUJCREP5RFR\",\"WARC-Block-Digest\":\"sha1:GFKZ64ZCLH7UNSOMISBFMLGDBI5SJQRY\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-50/CC-MAIN-2020-50_segments_1606141188146.22_warc_CC-MAIN-20201126113736-20201126143736-00163.warc.gz\"}"} |
http://dronesuavreport.com/2019/09/21/how-many-watts-does-a-drone-use/ | [
"## How many watts does a drone use?\n\nDrones these days, arrive in a variety of different sizes. Obviously, it is the new technology, and it has been made and modified into so many different models. You can get a drone in whatever size you like. How much power do they use? Here are some examples:\n\n1. A Mavic Air uses 44 Watts/hour.\n\n2. A Mavic 2 uses 59 watts/hour.\n\n3. A DJI Spark uses 17 watts/hour.\n\n4. Holy Stone HS700D 21 watts/hour.\n\nOne thing that is worth noticing is that the flying time is directly proportional to the size of the drone that you have. The bigger the drone, the more is its flying time. However, the smaller drones cannot even last five minutes in the air sometimes.\n\nOn the other hand, the bigger ones are capable of going half an hour in the air, easily. Why do you think, that a larger, and more probably a heavier drone would last longer in the air? To understand this phenomenon, we would have to probe deeper into the science of the drones.\n\nWatt is the unit of power. How do you estimate the power that is needed by a drone to hover in the air? Let’s suppose you have a drone with the rotors that spin. It doesn’t matter how many rotors you have. They could be one, or way more than one as well.\n\nWhat actually matters is that these rotors function by pushing the stationary rotors above them, downward. When the momentum of the air is increased, the rotor will exert a force on the air, and the air will push back on to the rotor. The drone will only be capable of hovering when the weight of the drone equals the weight of the air force.\n\nAirspeed and size of rotors are directly proportional to each other. So, increasing the size means that you would be increasing the power in watts that are being used by the drone.\n\nThis is an important phenomenon when you want to determine the power, which can be expressed by using the following expression.\n\nFrom this expression, we can deduce that the more area a rotor has, the more flying time it has. The power is going to depend upon the area of the rotors of the drone.\n\nPower also depends upon the air pressure. The drone will use less power if its speed is low. On the other hand, if you make it fly at high speed, it will use more power.\n\nPower is defined as the work done in a unit time. It is basically the rate at which a drone will use energy.\n\nThe power will be in watts if you will measure the energy in joules and time interval in seconds.\n\nIn a nutshell, a big drone is going to use more watts, and a smaller drone is going to"
]
| [
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9507389,"math_prob":0.9303913,"size":2469,"snap":"2019-51-2020-05","text_gpt3_token_len":566,"char_repetition_ratio":0.1444219,"word_repetition_ratio":0.0,"special_character_ratio":0.22478737,"punctuation_ratio":0.11111111,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9715049,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-12-12T06:34:26Z\",\"WARC-Record-ID\":\"<urn:uuid:d73cbce2-02d6-48a7-b989-5232f1cb3942>\",\"Content-Length\":\"27775\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:94794f0d-4f83-460c-891a-68ecc12c224c>\",\"WARC-Concurrent-To\":\"<urn:uuid:f08fe7b1-6680-4b1b-9386-1685099b615e>\",\"WARC-IP-Address\":\"146.66.113.49\",\"WARC-Target-URI\":\"http://dronesuavreport.com/2019/09/21/how-many-watts-does-a-drone-use/\",\"WARC-Payload-Digest\":\"sha1:V2423QYKRADZH6CFXBJWHEPWQ2SSGQE3\",\"WARC-Block-Digest\":\"sha1:GH4HQOIXVLX4ZILYT3L2YT5DAECF5NPT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-51/CC-MAIN-2019-51_segments_1575540537212.96_warc_CC-MAIN-20191212051311-20191212075311-00369.warc.gz\"}"} |
https://dev.to/robertobutti/tdd-with-pestphp-13c3 | [
"## DEV Community",
null,
"Roberto B.\n\nPosted on • Updated on\n\n# TDD with PestPHP\n\nTest Driven Development (TDD) is a software development practice.\n\nThe typical flow is:\n\n• writing the test cases starting from the requirements;\n• writing the code that solves the tests;\n• refactoring the code to pass all tests.\n\nWriting tests before the code, allows the developer to:\n\n• focus on requirements;\n• see if some requirements are missing or not detailed;\n• focus about the edge cases (empty params, invalid params etc). This is very useful for thinking outside the \"happy path\".\n\nThis approach helps and supports the developer for creating a \"better and more maintainable code\" because it forces the developer making the code/functions testable from the beginning:\n\n• splitting code in smaller and easier \"pieces\";\n• favoring the single responsibility approach;\n• favoring the code isolation (or encapsulation).\n\nBut, yes, fewer words and more code.\n\nFor our example, we are going to create a class with a static function for calculating the mean (the average).\n\n## Create your project from scratch\n\nCreate a new directory and jump into the new directory:\n\n``````mkdir tdd\ncd tdd\n``````\n\n## Install PestPHP\n\nNow you can install the testing framework PestPHP.\nPestPHP is built on top of the mature PHPUnit, and it aims to provide a nice and smooth interface for the developer that want to write tests.\n\n``````composer require pestphp/pest --dev --with-all-dependencies\nmkdir tests\n./vendor/bin/pest --init\n``````\n\nI'm going to skip the right configuration for PSR-4 autoloading, so I will create a file and include that in the test file via require\n\n## Create Stat class\n\nCreate your \"stat.php\" file with the class \"Stat\":\n\n``````<?php\n\nclass Stat\n{\n}\n``````\n\nYes, I know, the class is empty. Before to write the method and the implementation, you need to create the new test file.\nCreate \"StatTest.php\" file in the \"tests\" directory. The convention to write tests in \"tests\" directory and naming the file with \"Test.php\" suffix, allows PestPHP to automatically find the right tests.\n\n## Create the test file\n\nFile \"tests/StatTest.php\":\n\n``````<?php\nrequire('./stat.php');\n\ntest('test mean', function () {\nexpect(Stat::mean([1,2,3]))->toEqual(2);\n});\n``````\n\nBefore implementing the \"mean()\" method, we are expecting (expect()) that calling \"Stat::mean()\" with an array [1,2,3] as input parameter, it returns a value equal \"2\".\n\nThis is the happy path.\n\nBut I want also to think about \"bad scenarios\" for example if the user will call the method \"Stat::mean()\" with an empty array, I expect to retrieve a \"null\" value\n\n``````test('test mean with empty data', function () {\nexpect(Stat::mean([]))->toBeNull();\n});\n``````\n\nCalling \"Stat::mean()\" with a non array parameter (for example an integer) I expect to have an exception:\n\n``````test('test mean with not array', function () {\nexpect(\nfn () => Stat::mean(42)\n)->toThrow(TypeError::class);\n\n});\n``````\n\nIf you run the tests:\n\n``````./vendor/bin/pest\n``````\n\nYou will receive errors like \"undefined method\" because the class Stat is still empty, and it doesn't implement any methods.\n\n``````Call to undefined method Stat::mean()\n``````\n\nSo now, jump into \"stat.php\" file and implement the method mean() that for now will always return the value 0.0.\n\n``````<?php\n\nclass Stat\n{\npublic static function mean(array \\$data): ?float\n{\nreturn 0.0;\n}\n}\n``````\n\nIf you run the test now, you will still receive errors.",
null,
"The first one is about the assertion that expect to receive 2 as value. The current implementation is returning 0.0:\n\n`````` • Tests\\StatTest > test mean() with array parameter\nFailed asserting that 0.0 matches expected 2.\n``````\n\nThe second one is about the assertion that expect to receive \"null\" if the input parameter is an empty array. The current implementation is returning 0.0:\n\n`````` • Tests\\StatTest > test mean() with empty array parameter\nFailed asserting that 0.0 is null.\n``````\n\nThe test are failing, so now you need to focus on your implementation, on your code and implement the logic and making the test \"green\".\n\nIn your \"stat.php\" file in the \"mean()\" method, try to implement the mean:\n\n• count the elements in the array;\n• calculate the sum of the elements of the array;\n• divide the sum with the count.\n``````<?php\n\nclass Stat\n{\npublic static function mean(array \\$data): ?float\n{\n\\$count = count(\\$data);\n\\$sum = array_sum(\\$data);\nreturn \\$sum / \\$count;\n}\n}\n``````\n\nIf you execute the tests, the only one that fails is the test that calls \"mean()\" method with empty array and raises a \"Division by zero exception\".",
null,
"\"Division by zero\" is raised because the count is equal to 0. So, you need to check the length of the array, and if it is 0, you need to return \"null\".\n\n``````<?php\n\nclass Stat\n{\npublic static function mean(array \\$data): ?float\n{\n\\$count = count(\\$data);\nif ( ! \\$count) {\nreturn null;\n}\n\\$sum = array_sum(\\$data);\nreturn \\$sum / \\$count;\n}\n}\n``````\n\nIf you execute the tests ...",
null,
"All GREEN for us!\n\nSo, we:\n\n• Wrote the test focusing on happy path and \"bad scenarios\";\n• Wrote the code iteratively until all test passes.\n\nAnd you, are you applying TDD practice in your development process?",
null,
""
]
| [
null,
"https://res.cloudinary.com/practicaldev/image/fetch/s--Ya9UksYX--/c_imagga_scale,f_auto,fl_progressive,h_420,q_auto,w_1000/https://dev-to-uploads.s3.amazonaws.com/uploads/articles/77lj8rfwx633k9g8vqft.png",
null,
"https://res.cloudinary.com/practicaldev/image/fetch/s--qYzPKvV0--/c_limit%2Cf_auto%2Cfl_progressive%2Cq_auto%2Cw_880/https://dev-to-uploads.s3.amazonaws.com/uploads/articles/7git7mxw2uyt8t2f0135.png",
null,
"https://res.cloudinary.com/practicaldev/image/fetch/s--KzckTukZ--/c_limit%2Cf_auto%2Cfl_progressive%2Cq_auto%2Cw_880/https://dev-to-uploads.s3.amazonaws.com/uploads/articles/eekf5e793w93orgkplfx.png",
null,
"https://res.cloudinary.com/practicaldev/image/fetch/s--s6tArFuX--/c_limit%2Cf_auto%2Cfl_progressive%2Cq_auto%2Cw_880/https://dev-to-uploads.s3.amazonaws.com/uploads/articles/zt94mj34hc78kbgifroc.png",
null,
"https://res.cloudinary.com/practicaldev/image/fetch/s--PpzoLqR---/c_fill,f_auto,fl_progressive,h_50,q_auto,w_50/https://dev-to-uploads.s3.amazonaws.com/uploads/user/profile_image/589/jHw75m_5.jpg",
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]
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https://www.futuristicmath.com/grades.html | [
"# Free Math Activities by Grade For Kids\n\nFree math activities by grade for kids, math quizzes online, math games online, math board games, math flash cards, math puzzles and more. This page contains links to varied math resources which have been arranged by grade.\n\n### Pre-K / Kindergarten Math",
null,
"Pre-K and Kindergarten math: games, quizzes, worksheets & more.",
null,
"1st grade math activities: games, quizzes, worksheets & more.",
null,
"Practice 2nd grade math: games, quizzes, worksheets & more.",
null,
"Third grade math: games, quizzes, worksheets & more.",
null,
"4th grade math for kids : games, quizzes, worksheets & more.",
null,
"5th grade math : games, quizzes, worksheets & more.",
null,
"",
null,
""
]
| [
null,
"https://www.futuristicmath.com/thumbs/img/kindergarten.png",
null,
"https://www.futuristicmath.com/thumbs/img/1st-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/2nd-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/3rd-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/4th-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/5th-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/6th-grade.png",
null,
"https://www.futuristicmath.com/thumbs/img/7th-grade.png",
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https://wangdoc.com/es6/destructuring.html | [
"# 变量的解构赋值\n\n## 数组的解构赋值 #\n\n### 基本用法 #\n\nES6 允许按照一定模式,从数组和对象中提取值,对变量进行赋值,这被称为解构(Destructuring)。\n\n``````let a = 1;\nlet b = 2;\nlet c = 3;\n``````\n\nES6 允许写成下面这样。\n\n``````let [a, b, c] = [1, 2, 3];\n``````\n\n``````let [foo, [[bar], baz]] = [1, [, 3]];\nfoo // 1\nbar // 2\nbaz // 3\n\nlet [ , , third] = [\"foo\", \"bar\", \"baz\"];\nthird // \"baz\"\n\nlet [x, , y] = [1, 2, 3];\nx // 1\ny // 3\n\nlet [head, ...tail] = [1, 2, 3, 4];\ntail // [2, 3, 4]\n\nlet [x, y, ...z] = ['a'];\nx // \"a\"\ny // undefined\nz // []\n``````\n\n``````let [foo] = [];\nlet [bar, foo] = ;\n``````\n\n``````let [x, y] = [1, 2, 3];\nx // 1\ny // 2\n\nlet [a, [b], d] = [1, [2, 3], 4];\na // 1\nb // 2\nd // 4\n``````\n\n``````// 报错\nlet [foo] = 1;\nlet [foo] = false;\nlet [foo] = NaN;\nlet [foo] = undefined;\nlet [foo] = null;\nlet [foo] = {};\n``````\n\n``````let [x, y, z] = new Set(['a', 'b', 'c']);\nx // \"a\"\n``````\n\n``````function* fibs() {\nlet a = 0;\nlet b = 1;\nwhile (true) {\nyield a;\n[a, b] = [b, a + b];\n}\n}\n\nlet [first, second, third, fourth, fifth, sixth] = fibs();\nsixth // 5\n``````\n\n### 默认值 #\n\n``````let [foo = true] = [];\nfoo // true\n\nlet [x, y = 'b'] = ['a']; // x='a', y='b'\nlet [x, y = 'b'] = ['a', undefined]; // x='a', y='b'\n``````\n\n``````let [x = 1] = [undefined];\nx // 1\n\nlet [x = 1] = [null];\nx // null\n``````\n\n``````function f() {\nconsole.log('aaa');\n}\n\nlet [x = f()] = ;\n``````\n\n``````let x;\nif ( === undefined) {\nx = f();\n} else {\nx = ;\n}\n``````\n\n``````let [x = 1, y = x] = []; // x=1; y=1\nlet [x = 1, y = x] = ; // x=2; y=2\nlet [x = 1, y = x] = [1, 2]; // x=1; y=2\nlet [x = y, y = 1] = []; // ReferenceError: y is not defined\n``````\n\n## 对象的解构赋值 #\n\n### 简介 #\n\n``````let { foo, bar } = { foo: 'aaa', bar: 'bbb' };\nfoo // \"aaa\"\nbar // \"bbb\"\n``````\n\n``````let { bar, foo } = { foo: 'aaa', bar: 'bbb' };\nfoo // \"aaa\"\nbar // \"bbb\"\n\nlet { baz } = { foo: 'aaa', bar: 'bbb' };\nbaz // undefined\n``````\n\n``````let {foo} = {bar: 'baz'};\nfoo // undefined\n``````\n\n``````// 例一\nlet { log, sin, cos } = Math;\n\n// 例二\nconst { log } = console;\nlog('hello') // hello\n``````\n\n``````let { foo: baz } = { foo: 'aaa', bar: 'bbb' };\nbaz // \"aaa\"\n\nlet obj = { first: 'hello', last: 'world' };\nlet { first: f, last: l } = obj;\nf // 'hello'\nl // 'world'\n``````\n\n``````let { foo: foo, bar: bar } = { foo: 'aaa', bar: 'bbb' };\n``````\n\n``````let { foo: baz } = { foo: 'aaa', bar: 'bbb' };\nbaz // \"aaa\"\nfoo // error: foo is not defined\n``````\n\n``````let obj = {\np: [\n'Hello',\n{ y: 'World' }\n]\n};\n\nlet { p: [x, { y }] } = obj;\nx // \"Hello\"\ny // \"World\"\n``````\n\n``````let obj = {\np: [\n'Hello',\n{ y: 'World' }\n]\n};\n\nlet { p, p: [x, { y }] } = obj;\nx // \"Hello\"\ny // \"World\"\np // [\"Hello\", {y: \"World\"}]\n``````\n\n``````const node = {\nloc: {\nstart: {\nline: 1,\ncolumn: 5\n}\n}\n};\n\nlet { loc, loc: { start }, loc: { start: { line }} } = node;\nline // 1\nloc // Object {start: Object}\nstart // Object {line: 1, column: 5}\n``````\n\n``````let obj = {};\nlet arr = [];\n\n({ foo: obj.prop, bar: arr } = { foo: 123, bar: true });\n\nobj // {prop:123}\narr // [true]\n``````\n\n``````// 报错\nlet {foo: {bar}} = {baz: 'baz'};\n``````\n\n``````const obj1 = {};\nconst obj2 = { foo: 'bar' };\nObject.setPrototypeOf(obj1, obj2);\n\nconst { foo } = obj1;\nfoo // \"bar\"\n``````\n\n### 默认值 #\n\n``````var {x = 3} = {};\nx // 3\n\nvar {x, y = 5} = {x: 1};\nx // 1\ny // 5\n\nvar {x: y = 3} = {};\ny // 3\n\nvar {x: y = 3} = {x: 5};\ny // 5\n\nvar { message: msg = 'Something went wrong' } = {};\nmsg // \"Something went wrong\"\n``````\n\n``````var {x = 3} = {x: undefined};\nx // 3\n\nvar {x = 3} = {x: null};\nx // null\n``````\n\n### 注意点 #\n\n(1)如果要将一个已经声明的变量用于解构赋值,必须非常小心。\n\n``````// 错误的写法\nlet x;\n{x} = {x: 1};\n// SyntaxError: syntax error\n``````\n\n``````// 正确的写法\nlet x;\n({x} = {x: 1});\n``````\n\n(2)解构赋值允许等号左边的模式之中,不放置任何变量名。因此,可以写出非常古怪的赋值表达式。\n\n``````({} = [true, false]);\n({} = 'abc');\n({} = []);\n``````\n\n(3)由于数组本质是特殊的对象,因此可以对数组进行对象属性的解构。\n\n``````let arr = [1, 2, 3];\nlet {0 : first, [arr.length - 1] : last} = arr;\nfirst // 1\nlast // 3\n``````\n\n## 字符串的解构赋值 #\n\n``````const [a, b, c, d, e] = 'hello';\na // \"h\"\nb // \"e\"\nc // \"l\"\nd // \"l\"\ne // \"o\"\n``````\n\n``````let {length : len} = 'hello';\nlen // 5\n``````\n\n## 数值和布尔值的解构赋值 #\n\n``````let {toString: s} = 123;\ns === Number.prototype.toString // true\n\nlet {toString: s} = true;\ns === Boolean.prototype.toString // true\n``````\n\n``````let { prop: x } = undefined; // TypeError\nlet { prop: y } = null; // TypeError\n``````\n\n## 函数参数的解构赋值 #\n\n``````function add([x, y]){\nreturn x + y;\n}\n\n``````\n\n``````[[1, 2], [3, 4]].map(([a, b]) => a + b);\n// [ 3, 7 ]\n``````\n\n``````function move({x = 0, y = 0} = {}) {\nreturn [x, y];\n}\n\nmove({x: 3, y: 8}); // [3, 8]\nmove({x: 3}); // [3, 0]\nmove({}); // [0, 0]\nmove(); // [0, 0]\n``````\n\n``````function move({x, y} = { x: 0, y: 0 }) {\nreturn [x, y];\n}\n\nmove({x: 3, y: 8}); // [3, 8]\nmove({x: 3}); // [3, undefined]\nmove({}); // [undefined, undefined]\nmove(); // [0, 0]\n``````\n\n`undefined`就会触发函数参数的默认值。\n\n``````[1, undefined, 3].map((x = 'yes') => x);\n// [ 1, 'yes', 3 ]\n``````\n\n## 圆括号问题 #\n\n### 不能使用圆括号的情况 #\n\n(1)变量声明语句\n\n``````// 全部报错\nlet [(a)] = ;\n\nlet {x: (c)} = {};\nlet ({x: c}) = {};\nlet {(x: c)} = {};\nlet {(x): c} = {};\n\nlet { o: ({ p: p }) } = { o: { p: 2 } };\n``````\n\n(2)函数参数\n\n``````// 报错\nfunction f([(z)]) { return z; }\n// 报错\nfunction f([z,(x)]) { return x; }\n``````\n\n(3)赋值语句的模式\n\n``````// 全部报错\n({ p: a }) = { p: 42 };\n([a]) = ;\n``````\n\n``````// 报错\n[({ p: a }), { x: c }] = [{}, {}];\n``````\n\n### 可以使用圆括号的情况 #\n\n``````[(b)] = ; // 正确\n({ p: (d) } = {}); // 正确\n[(parseInt.prop)] = ; // 正确\n``````\n\n## 用途 #\n\n(1)交换变量的值\n\n``````let x = 1;\nlet y = 2;\n\n[x, y] = [y, x];\n``````\n\n(2)从函数返回多个值\n\n``````// 返回一个数组\n\nfunction example() {\nreturn [1, 2, 3];\n}\nlet [a, b, c] = example();\n\n// 返回一个对象\n\nfunction example() {\nreturn {\nfoo: 1,\nbar: 2\n};\n}\nlet { foo, bar } = example();\n``````\n\n(3)函数参数的定义\n\n``````// 参数是一组有次序的值\nfunction f([x, y, z]) { ... }\nf([1, 2, 3]);\n\n// 参数是一组无次序的值\nfunction f({x, y, z}) { ... }\nf({z: 3, y: 2, x: 1});\n``````\n\n(4)提取 JSON 数据\n\n``````let jsonData = {\nid: 42,\nstatus: \"OK\",\ndata: [867, 5309]\n};\n\nlet { id, status, data: number } = jsonData;\n\nconsole.log(id, status, number);\n// 42, \"OK\", [867, 5309]\n``````\n\n(5)函数参数的默认值\n\n``````jQuery.ajax = function (url, {\nasync = true,\nbeforeSend = function () {},\ncache = true,\ncomplete = function () {},\ncrossDomain = false,\nglobal = true,\n// ... more config\n} = {}) {\n// ... do stuff\n};\n``````\n\n(6)遍历 Map 结构\n\n``````const map = new Map();\nmap.set('first', 'hello');\nmap.set('second', 'world');\n\nfor (let [key, value] of map) {\nconsole.log(key + \" is \" + value);\n}\n// first is hello\n// second is world\n``````\n\n``````// 获取键名\nfor (let [key] of map) {\n// ...\n}\n\n// 获取键值\nfor (let [,value] of map) {\n// ...\n}\n``````\n\n(7)输入模块的指定方法\n\n``````const { SourceMapConsumer, SourceNode } = require(\"source-map\");\n``````"
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https://socratic.org/questions/how-do-you-differentiate-y-sin-3x-cot-x-3-8 | [
"How do you differentiate y = (sin(3x) + cot(x^3))^8?\n\nJul 31, 2015\n\n${y}^{'} = 24 \\cdot {\\left[\\sin \\left(3 x\\right) + \\cot \\left({x}^{3}\\right)\\right]}^{7} \\cdot \\left[\\cos \\left(3 x\\right) - {x}^{2} \\csc \\left({x}^{3}\\right)\\right]$\n\nExplanation:\n\nNotice that you can write your function $y$ as\n\n$y = {u}^{8}$, with $u = \\sin \\left(3 x\\right) + \\cot \\left({x}^{3}\\right)$\n\nThis means that you can use the power rule and the chain rule to differentiate $y$.\n\nFor a function $y$ that depends on a variable $u$, which in turn depends on a variable $x$, you can determine its derivative by using the chain rule\n\n$\\textcolor{b l u e}{\\frac{d}{\\mathrm{dx}} \\left(y\\right) = \\frac{d}{\\mathrm{du}} \\left(y\\right) \\cdot \\frac{d}{\\mathrm{dx}} \\left(u\\right)}$\n\nIn your case, this would be equivalent to\n\n${y}^{'} = \\frac{d}{\\mathrm{du}} \\left({u}^{8}\\right) \\cdot \\frac{d}{\\mathrm{dx}} \\left(u\\right)$\n\n${y}^{'} = 8 {u}^{7} \\cdot \\frac{d}{\\mathrm{dx}} {\\underbrace{\\left(\\sin \\left(3 x\\right) + \\cot \\left({x}^{3}\\right)\\right)}}_{\\textcolor{red}{a \\left(x\\right)}}$\n\nNow focus on differentiating function $\\textcolor{red}{a \\left(x\\right)}$, which can be written as\n\n$\\frac{d}{\\mathrm{dx}} \\left(a\\right) = \\frac{d}{\\mathrm{dx}} \\left(\\sin \\left(3 x\\right)\\right) + \\frac{d}{\\mathrm{dx}} \\left(\\cot \\left({x}^{3}\\right)\\right)$\n\nOnce again, use the chain rule to differentiate these functions. Remember that\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\sin x\\right) = \\cos x$\n\nand that\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\cot x\\right) = - {\\csc}^{2} x$\n\nThe first one will be\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\sin {u}_{1}\\right) = \\frac{d}{{\\mathrm{du}}_{1}} \\cdot \\left(\\sin {u}_{1}\\right) \\cdot \\frac{d}{\\mathrm{dx}} \\left({u}_{1}\\right)$, where ${u}_{1} = 3 x$\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\sin {u}_{1}\\right) = \\cos {u}_{1} \\cdot \\frac{d}{\\mathrm{dx}} \\left(3 x\\right)$\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\sin \\left(3 x\\right)\\right) = 3 \\cos \\left(3 x\\right)$\n\nThe second one will be\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\cot {u}_{2}\\right) = \\frac{d}{{\\mathrm{du}}_{2}} \\left(\\cot {u}_{2}\\right) \\cdot \\frac{d}{\\mathrm{dx}} \\left({u}_{2}\\right)$, where ${u}_{2} = {x}^{3}$\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\cot {u}_{2}\\right) = - {\\csc}^{2} {u}_{2} \\cdot \\frac{d}{\\mathrm{dx}} \\left({x}^{3}\\right)$\n\n$\\frac{d}{\\mathrm{dx}} \\left(\\cot {u}_{2}\\right) = - {\\csc}^{2} \\left({x}^{3}\\right) \\cdot 3 {x}^{2}$\n\nPlug these back into your tager derivative to get\n\n${y}^{'} = 8 \\cdot {\\left[\\sin \\left(3 x\\right) + \\cot \\left({x}^{3}\\right)\\right]}^{7} \\cdot \\left(3 \\cos \\left(3 x\\right) - {\\csc}^{2} \\left({x}^{3}\\right) \\cdot 3 {x}^{2}\\right)$\n\n${y}^{'} = \\textcolor{g r e e n}{24 \\cdot {\\left[\\sin \\left(3 x\\right) + \\cot \\left({x}^{3}\\right)\\right]}^{7} \\cdot \\left[\\cos \\left(3 x\\right) - {x}^{2} \\csc \\left({x}^{3}\\right)\\right]}$"
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https://mathematica.stackexchange.com/questions/250503/control-evaluation-for-functional-constraints | [
"# Control evaluation for functional constraints\n\nI'm trying to understand how to use Mathematica to find a solution subject to constraints, where one of the constraints is specified as a predicate function. But I don't know how to control evaluation in order to use the predicate function as a condition.\n\nHere's the problem. I want to find three integers, $$a$$, $$b$$, and $$c$$, subject to these constraints:\n\n1. They sum to 70\n2. Each of the integer is greater than or equal to 15 and less than 30\n3. No digits from 1-9 appears twice if you consider all the digits in the squares of the integers.\n\nSo how do I approach this with Mathematica? I expect I can use FindInstance to find values under a set of constraints.\n\nI can express constraints 1 and 2 by setting variables equal to equations and inequalities:\n\neq = (a + b + c == 70);\ncs = 15 <= a <= 30 && 15 <= b <= 30 && 15 <= c <= 30;\n\n\nIn order to express the third constraint, I have defined this predicate function, which takes a list of numbers and returns true when they do not re-use digits:\n\nUniqueDigitsQ[xss_] := With[\n{nonzeros = Select[Flatten[Map[IntegerDigits,xss]] ,#1!=0&]},\nSortBy[Tally[nonzeros],Last][[-1,-1]] <2];\n\n\nSo I would like to be able to express the third constraint by saying:\n\ncs2 = UniqueDigitsQ[ {a^2,b^2,c^2} ];\n\n\nBut this fails, because the predicate function cannot handle symbolic argument.\n\nIs there a way to fix this problem by defining the function in such a way that it does not evaluate until the arguments are numeric? Or else, what is the right approach?\n\n• Welcome to Mathematica.SE! I hope you will become a regular contributor. To get started, 1) take the introductory tour now, 2) when you see good questions and answers, vote them up by clicking the gray triangles, because the credibility of the system is based on the reputation gained by users sharing their knowledge, 3) remember to accept the answer, if any, that solves your problem, by clicking the checkmark sign, and 4) give help too, by answering questions in your areas of expertise. Jul 3, 2021 at 4:31\n\nClear[\"Global*\"]\n\n\nFind all solutions for the first two criteria then select from those the ones that meet the third criteria.\n\nsol = Select[\nSolve[{a + b + c == 70, 15 <= a < 30, 15 <= b < 30,\n15 <= c < 30}, {a, b, c}, Integers],\n(digits = Flatten[IntegerDigits[{a^2, b^2, c^2}] /. #];\nLength[digits] == Length[Union@digits]) &]\n\n(* {{a -> 19, b -> 23, c -> 28}, {a -> 19, b -> 28, c -> 23}, {a -> 23,\nb -> 19, c -> 28}, {a -> 23, b -> 28, c -> 19}, {a -> 28, b -> 19,\nc -> 23}, {a -> 28, b -> 23, c -> 19}} *)\n\n\nThese are just permutations of {19, 23, 28}\n\nEDIT: A user-defined function must be used in an equation or an inequality. Consequently, modify your function to return a numeric value.\n\nUniqueDigitsQ[xss_?(VectorQ[#, NumericQ] &)] := With[\n{nonzeros = Select[Flatten[Map[IntegerDigits, xss]], #1 != 0 &]},\nBoole[SortBy[Tally[nonzeros], Last][[-1, -1]] < 2]];\n\nSolve[{a + b + c == 70, 15 <= a < 30, 15 <= b < 30, 15 <= c < 30,\nUniqueDigitsQ[{a^2, b^2, c^2}] == 1}, {a, b, c}, Integers]\n\n(* {{a -> 19, b -> 23, c -> 28}, {a -> 19, b -> 28, c -> 23}, {a -> 23, b -> 19,\nc -> 28}, {a -> 23, b -> 28, c -> 19}, {a -> 28, b -> 19,\nc -> 23}, {a -> 28, b -> 23, c -> 19}} *)\n\n• Thanks! Is this a better way because Mathematica’s solvers work only with equations and inequalities, and not user-defined functions? Or is it that it’s dangerous to use substitutions with user-defined functions at all? Functions are obviously a basic form of abstraction, so I’d like to understand how to use them in this sort of case because usually it becomes untenable to express everything in an inline snippet of code. Jul 3, 2021 at 14:58\n• The solvers can work with user-defined functions. I just find the approach that I used simple and straightforward. You could also eliminate the redundancy of the permutations by adding a fourth constraint that the values are ordered, e.g., a < b < c`. Note that the third constraint eliminates any equality. Jul 3, 2021 at 15:07\n• Oh I quite agree your approach is simpler and better! I just remain curious how my kind of approach would work, since sometimes function-defined constraints will be unavoidable, and I wonder if the solver can work with them efficiently or if it can only work analytically with equations and then you have to brute force search over functions. Also, even if the solver could handle UDFs, I think it couldn’t handle mine because mine consumes symbolic arguments eagerly, before substitution rules are applied, unlike IntegerDigits apparently. This is the evaluation behavior I don’t understand. Jul 3, 2021 at 17:12"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8766827,"math_prob":0.9820447,"size":1482,"snap":"2023-40-2023-50","text_gpt3_token_len":374,"char_repetition_ratio":0.11840325,"word_repetition_ratio":0.007633588,"special_character_ratio":0.27530363,"punctuation_ratio":0.117056854,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99621737,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-09-22T12:34:08Z\",\"WARC-Record-ID\":\"<urn:uuid:dc1e7987-3946-422d-a673-44f3bae27cbb>\",\"Content-Length\":\"160592\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:41e94a66-5254-4052-a873-3eed8f546f08>\",\"WARC-Concurrent-To\":\"<urn:uuid:e27b240b-7b1f-4fa7-bad2-1058ec532c0c>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://mathematica.stackexchange.com/questions/250503/control-evaluation-for-functional-constraints\",\"WARC-Payload-Digest\":\"sha1:6FWW3YRNAJ4DFANWUXJ2N6EW4J3PYQGQ\",\"WARC-Block-Digest\":\"sha1:2LVW4PSK6PJ3CGZA55MW7FKU3435YWWN\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-40/CC-MAIN-2023-40_segments_1695233506399.24_warc_CC-MAIN-20230922102329-20230922132329-00630.warc.gz\"}"} |
http://www.ueda.info.waseda.ac.jp/hydla/index.php?cmd=backup&action=nowdiff&page=Examples&age=8 | [
"# Backup diff of Examples vs current(No. 8)\n\n• The added line is THIS COLOR.\n• The deleted line is THIS COLOR.\n#author(\"2017-03-17T11:54:21+09:00\",\"default:Uedalab\",\"Uedalab\")\n#author(\"2017-03-17T17:42:45+09:00\",\"default:Uedalab\",\"Uedalab\")\n#noattach\n* A Bouncing Particle [#p560bc2f]\n>\n* Bouncing particle [#p560bc2f]\n\n// y stands for the height of the ball\nINIT <=> y = 10 & y' = 0. // initial state\nFALL <=> [](y'' = -10). // falling\nBOUNCE <=> [](y- = 0 => y' = -4/5*y'-).\n// if the ball reaches the ground, it bounces\nINIT, FALL << BOUNCE. // FALL is weaker than BOUNCE\n<\n\n&ref(./Bouncing_Particle.png,50%);\n----\n* A Bouncing Particle with a Parameter [#z5246173]\n>\n* Bouncing particle with a parametric initial height [#z5246173]\n\nINIT <=> 5 < y < 15 & y' = 0. // the initial height is uncertain\nFALL <=> [](y'' = -10).\nBOUNCE <=> [](y- = 0 => y' = -4/5 * y'-).\n\nINIT, FALL << BOUNCE.\n<\n\n&ref(./Bouncing_Particle_with_a_Parameter.png,100%);\n----\n* A Bouncing Paticle on a Curve [#j8167ade]\n>\n* Bouncing particle in a parabolic vase [#j8167ade]\n\n/**\n* bouncing particle on a curve of f(x) = (1/2) * x^2\n*/\n\nINIT <=> x = 1/2 & y = 10 & x' = 0 & y' = 0 & [](k = 1).\nA <=> [](x'' = 0 & y'' = -98/10).\n/**\n* sin = f'(x) / (1+f'(x))^(1/2)\n* cos = 1 / (1+f'(x))^(1/2)\n* new x' = (-k * sin^2 + cos^2) * x' + (k+1) * sin * cos * y'\n* new y' = (k+1) * sin * cos * x' + (sin^2 + (-k) * cos^2) * y'\n*/\n\nSC <=> [](s = (x-)/(1+(x-)^2)^(1/2)\n& c = 1 /(1+(x-)^2)^(1/2)).\n\nBOUNCE <=> [](y- = (1/2) * (x-)^2 =>\nx' = ( (-k) * s^2 + c^2 ) * x'- + ( (k+1) * s * c ) * y'-\n& y' = ( (k+1) * s * c ) * x'- + ( s^2 + (-k) * c^2 ) * y'- ).\n\nINIT, SC, A << BOUNCE.\n<\n\n&ref(./Bouncing_Paticle_on_a_Curve.png,70%);\n----\n* A Bouncing Particle in a Circle [#xbf24e18]\n>\n* Bouncing particle in a circle [#xbf24e18]\n\nINIT <=> x = 0 /\\ 0.5 < y < 0.6 /\\ x' = 2 /\\ y' = 1.\n// the initial position is uncertain\nRUN <=> [](x'' = 0 /\\ y'' = 0).\nBOUNCE <=> []((x-)^2 + (y-)^2 = 1 =>\nx' = x'- - (x- * x'- + y- * y'-) * 2 * (x-)\n/\\ y' = y'- - (x- * x'- + y- * y'-) * 2 * (y-)\n).\nINIT, RUN<<BOUNCE.\n<\n\n&ref(./Bouncing_Particle_in_a_Circle.png,70%);\n----\n* A Hot-Air Balloon with multiple parameters [#tf906f5e]\n>\n* Hot-Air Balloon with multiple parameters [#tf906f5e]\n\n/* A program for a hot-air balloon that repeats rising and falling */\n// The initial condition of the balloon and the timer\n// h: height of the balloon\n// timer: timer variable to repeat rising and falling\nINIT <=> h = 10 /\\ h' = 0 /\\ timer = 0.\n\n// parameters\n// duration: duration of falling\n// riseT: duration of rising\nPARAM<=> 1 < fallT < 4 /\\ 1 < riseT < 3\n/\\ [](riseT' = 0 /\\ fallT' = 0).\n\n// increasing of timer\nTIMER <=> [](timer' = 1).\n\n// rising of the balloon\nRISE <=> [](timer- < riseT =>h'' = 1).\n\n// falling of the balloon\nFALL <=> [](timer- >= riseT => h'' = -2).\n\n// reset the timer to repeat rising and falling\nRESET <=> [](timer- >= riseT + fallT => timer=0).\n\n// assertion for bounded model checking\nASSERT(h > 0).\n\n// constraint hierarchies\nINIT, PARAM, FALL, RISE, TIMER<<RESET.\n<\n\n&ref(./Hot-Air_Balloon.png,70%);\n----\n* A Bouncing Particle with Magnetic Force [#a6ea3f5c]\n>\n* Bouncing particle with magnetic force [#a6ea3f5c]\n\nINIT <=> y=10 & y'=0 & mag=0 & timer=0.\nFALL <=> [](y''=-10+mag).\nBOUNCE <=> [](y-=0=>y'=-y'-).\nTRUE <=> [](1=1).\nTIMER <=> [](mag'=0&timer'=1).\nSWITCHON <=> [](timer-=1=>mag=12&timer=0).\n// The magnetic force may be switched on at every one second\nSWITCHOFF <=> [](timer-=1=>mag=0&timer=0).\n// The magnetic force may be switched off at every one second\n\nINIT,TIMER<<(SWITCHOFF,SWITCHON)<<TRUE,FALL<<BOUNCE.\n<\n\n&ref(./Bouncing_Particle_with_Magnetic_Force.png,70%);\n----\n* A Bouncing Particle thrown toward a ceiling [#e682ba1f]\n>\n* Bouncing particle thrown toward a ceiling [#e682ba1f]\n\nINIT <=> 9 < y < 11 & y' = 10.\nFALL <=> [](y'' = -10).\nBOUNCE <=> [](y- = 15 => y' = -(4/5)*y'-).\n\nINIT, FALL << BOUNCE.\n<\n\n#mathjax\n- In this program, the trajectories change qualitatively dependent on the initial height $$y_0$$.\n-- If $$9 < y_0 < 10$$, the ball doesn't reach the ceiling.~\n-- If $$y_0 = 10$$, the ball touches the ceiling, but the velocity remains continuous.~\n-- If $$10 < y_0 < 11$$, the ball bounces on the ceiling.~\n- HyLaGI performs such a case analysis automatically.~\n#norelated\n&ref(./Bouncing_Particle_thrown_toward a_ceiling.png,100%);\n----"
]
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https://wiki-helper.com/determine-wheter-the-values-given-against-the-quadratic-equation-are-the-root-of-the-equation-or-37400899-28/ | [
"# determine wheter the values given against the quadratic equation are the root of the equation or not X2+4x-5=0 ,X=1,-1\n\ndetermine wheter the values given against the quadratic equation are the root of the equation or not X2+4x-5=0 ,X=1,-1\n\n### 1 thought on “determine wheter the values given against the quadratic equation are the root of the equation or not X2+4x-5=0 ,X=1,-1”\n\n1.",
null,
""
]
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"https://wiki-helper.com/wp-content/litespeed/avatar/903550a2f70b936bc3f8a4e89e4a4dc9.jpg",
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https://www.oreilly.com/library/view/2007-microsoft-office/9780735623248/ch14s02.html | [
"With Safari, you learn the way you learn best. Get unlimited access to videos, live online training, learning paths, books, tutorials, and more.\n\nNo credit card required\n\nUsing Functions: A Preview\n\nIn simplest terms, a function is a predefined formula. Many Excel functions are shorthand versions of frequently used formulas. For example, compare the formula =A1+A2+A3+A4+A5+A6+A7+A8+A9+A10 with the formula =SUM(A1:A10). The SUM function makes the formula a lot shorter, easier to read, and easier to create. Some Excel functions perform complex calculations. For example, using the PMT function, you can calculate the payment on a loan at a given interest rate and principal amount.\n\nAll functions consist of a function name followed by a set of arguments enclosed in parentheses. (In the preceding example, A1:A10 is the argument in the SUM function.) If you omit a closing parenthesis when you enter a function, Excel adds ...\n\nWith Safari, you learn the way you learn best. Get unlimited access to videos, live online training, learning paths, books, interactive tutorials, and more.\n\nNo credit card required"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.76730806,"math_prob":0.925256,"size":755,"snap":"2019-43-2019-47","text_gpt3_token_len":165,"char_repetition_ratio":0.15579228,"word_repetition_ratio":0.0,"special_character_ratio":0.22649007,"punctuation_ratio":0.13907285,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99414414,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-10-14T04:05:57Z\",\"WARC-Record-ID\":\"<urn:uuid:b5d667e0-957f-4b0c-a9b6-74104885abf3>\",\"Content-Length\":\"34267\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:4d7ae794-c9cc-4ad8-82b6-b84756d8e972>\",\"WARC-Concurrent-To\":\"<urn:uuid:f68fc27d-d1fc-46d0-96bb-f1e2bcaa8e58>\",\"WARC-IP-Address\":\"104.80.31.164\",\"WARC-Target-URI\":\"https://www.oreilly.com/library/view/2007-microsoft-office/9780735623248/ch14s02.html\",\"WARC-Payload-Digest\":\"sha1:R3KEFOAG4PX4HZAWDBY2WYVLNE2HL7SX\",\"WARC-Block-Digest\":\"sha1:7LFUUYLGFDRIBBQ7SZAOOIRRLUPWZXPF\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-43/CC-MAIN-2019-43_segments_1570986649035.4_warc_CC-MAIN-20191014025508-20191014052508-00090.warc.gz\"}"} |
http://jarnoralli.com/code/optical-flow-code | [
"# Optical Flow Code\n\nOne complete chapter of my thesis is devoted to explaining how the variational optical flow, disparity and level-set models can be solved. In this chapter I show, step by step, how these models can be solved using different kinds of solvers (Jacobi, Gauss Seidel, Alternating Line Relaxation and Additive Operator Splitting scheme). Related to this chapter, I release the optical flow and disparity codes on this page...these codes are quite similar to the ones that I have used for generating the videos on this site. However, they are not 100% the same...there have been some slight modifications. For anyone interested in the actual code, I suggest first to have a look at the thesis in order to better understand the code itself! The codes are released under LGPL license. If you use the codes, please reference my papers...in my papers, on the other hand, I reference those papers upon which my work is based on. Thanx!!\n\nThe optical flow codes are as follows:\n\n1. Late linerisation optical-flow for large displacements.\n2. Early linearisation optical-flow method for small displacements (basically Horn&Schunck type of formulation).\n3. Late linearisation method for disparity.\n\nPseudo Code\n\nBelow you can see pseudo codes for early- and late-linearization versions of the optical flow. I decided to include these here in order to give a better idea how the different codes actually work. However, all the details are explained in my phd thesis. Therefore, I recommend that you have a look at Chapter 5, Solving Equations.\n\n### Early Linearization\n\n• //----------------------------------------------------------------------------------------------------------------\n• //-COARSE-TO-FINE ALGORITHM FOR CALCULATING OPTICAL FLOW\n• //-Early linearisation (i.e. no warping)\n• //-Quadratic smoothness term (i.e. Tikhonov regulariser)\n• //-Inputs are $$I_0$$ and $$I_1$$, number of scales $$scl$$, and scaling factor $$sclFactor$$\n• //----------------------------------------------------------------------------------------------------------------\n• $$\\mathbf{INPUT:} \\, I_0, \\, I_1, \\, scl, \\, sclFactor$$\n• $$\\mathbf{OUTPUT:} \\, (u,\\, v)$$\n• //Set $$u$$ and $$v$$ to zero\n• $$u=0$$, $$v=0$$\n• //Create image pyramid\n• $$[ Iscl_0\\{\\}, \\, Iscl_1\\{\\} ] = pyramid(I_0, \\, I_1, \\, scl, \\, sclFactor)$$\n• //This is the coarse-to-fine loop\n• WHILE( $$s=scl:-1:1$$ )\n• $$I_0 = Iscl_0\\{s\\}, \\, I_1 = Iscl_1\\{s\\}$$\n• Approximate derivatives for $$I_0$$ and $$I_1$$: $$\\dfrac{\\partial I_k}{\\partial t}$$, $$\\dfrac{\\partial I_{k,0}}{\\partial x}$$, $$\\dfrac{\\partial I_{k,0}}{\\partial y}$$\n• //Solve for new $$u$$ and $$v$$\n• $$[u, \\, v] = SOLVER ( u, \\, v, \\, nLoops, \\, \\dfrac{\\partial I_k}{\\partial t}, \\, \\dfrac{\\partial I_{k,0}}{\\partial x}, \\, \\dfrac{\\partial I_{k,0}}{\\partial y} )$$\n• //Interpolate (prolongate) solution\n• IF ( $$s-1>0$$ )\n• $$[u, \\, v] = prolongate( u, \\, v, \\,sclFactor )$$\n• ENDIF\n• ENDWHILE\n\n### Late Linearization\n\n• //----------------------------------------------------------------------------------------------------------------\n• //-COARSE-TO-FINE ALGORITHM FOR CALCULATING OPTICAL FLOW\n• //-Late linearisation (i.e. uses warping)\n• //-Robust error functions in both the data and the smoothness terms\n• //-Inputs are $$I_0$$ and $$I_1$$, number of scales $$scl$$, and scaling factor $$sclFactor$$\n• //----------------------------------------------------------------------------------------------------------------\n• $$\\mathbf{INPUT:} \\, I_0, \\, I_1, \\, scl, \\, sclFactor$$\n• $$\\mathbf{OUTPUT:} \\, (u,\\, v)$$\n• //Set $$u$$ and $$v$$ to zero\n• $$u=0$$, $$v=0;$$\n• //Create image pyramid\n• $$[ Iscl_0\\{\\} \\, Iscl_1\\{\\} ] = pyramid(I_0, \\, I_1, \\, scl, \\, sclFactor);$$\n• //Coarse-to-fine loop\n• WHILE( $$s=scl:-1:1$$ )\n• $$I_0 =Iscl_0\\{s\\}$$, $$I_1 =Iscl_1\\{s\\};$$\n• //Warping loop\n• WHILE( $$fstLoop$$)\n• //Warp image as per $$u$$ and $$v$$\n• $$I_{k,0}^w = warp( I_{k,0}, u, v );$$\n• Approximate derivatives for $$I_0^w$$ and $$I_1$$: $$\\dfrac{\\partial I_k}{\\partial t} = I_{k,1} - I_{k,0}^w$$, $$\\dfrac{\\partial I_{k,0}^w}{\\partial x}$$, $$\\dfrac{\\partial I_{k,0}^w}{\\partial y}$$\n• //Reset $$du$$ and $$dv$$\n• $$du=0$$, $$dv=0$$\n• //Fixed-point loop due to the robust error functions\n• WHILE( $$sndLoop$$)\n• //Calculate penalizer function values for data\n• $$\\Psi{\\prime} \\Big( (E_k)_D \\Big)$$, where $$\\left( E_k \\right)_D = \\left( \\dfrac{ \\partial I_k }{\\partial t} - \\dfrac{ \\partial I_{k,0}^{w} }{\\partial x}du - \\dfrac{ \\partial I_{k,0}^{w} }{\\partial y}dv \\right)^2 ;$$\n• //Calculate the diffusion weights\n• $$\\Big[ \\Psi{\\prime} \\big( E_R^{l,m} \\big)_W \\, \\Psi{\\prime} \\big( E_R^{l,m} \\big)_N \\, \\Psi{\\prime} \\big( E_R^{l,m} \\big)_E \\, \\Psi{\\prime} \\big( E_R^{l,m} \\big)_S \\Big] = weights(u+du, v+dv);$$\n• //Solve for new $$du$$ and $$dv$$\n• $$\\begin{matrix} [du \\, dv] = SOLVER ( & u, \\, v, \\, du, \\, dv, \\, nLoops, \\, \\dfrac{\\partial I_k}{\\partial t}, \\, \\dfrac{\\partial I_{k,0}^w}{\\partial x}, \\, \\dfrac{\\partial I_{k,0}^w}{\\partial y}, \\, \\Psi{\\prime} \\Big( (E_k)_D \\Big), &\\\\ & \\Psi{\\prime} \\big( E_R^{l,m} \\big)_W, \\, \\Psi{\\prime} \\big( E_R^{l,m} \\big)_N, &\\\\ & \\Psi{\\prime} \\big( E_R^{l,m} \\big)_S, \\, \\Psi{\\prime} \\big( E_R^{l,m} \\big)_E & ); \\end{matrix}$$\n• ENDWHILE\n• //Update $$u$$ and $$v$$\n• $$u=u+du$$, $$v=v+dv;$$\n• ENDWHILE\n• //Interpolate (prolongate) solution\n• IF( $$s-1>0$$ )\n• $$[u \\, v] = prolongate( u, \\, v, \\,sclFactor );$$\n• ENDIF\n• ENDWHILE",
null,
"Author: Jarno Ralli\nJarno Ralli is a computer vision scientist and a programmer.",
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"http://jarnoralli.com/component/jcomments/captcha/97261",
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"http://jarnoralli.com/modules/mod_nice_social_bookmark/icons/facebook_aqu_48.png",
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"http://jarnoralli.com/modules/mod_nice_social_bookmark/icons/twitter_aqu_48.png",
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"http://jarnoralli.com/modules/mod_nice_social_bookmark/icons/google_aqu_48.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.649838,"math_prob":0.9998425,"size":5426,"snap":"2020-10-2020-16","text_gpt3_token_len":1810,"char_repetition_ratio":0.22150499,"word_repetition_ratio":0.16981132,"special_character_ratio":0.4493181,"punctuation_ratio":0.20042194,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":1.0000046,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12],"im_url_duplicate_count":[null,null,null,1,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-02-17T14:31:36Z\",\"WARC-Record-ID\":\"<urn:uuid:46c968ae-1aa7-4e50-bd1d-4f6eea42fc95>\",\"Content-Length\":\"30291\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:74baf3ea-75e3-43a7-9613-f1f25c4cda8c>\",\"WARC-Concurrent-To\":\"<urn:uuid:72f7f3fa-0a66-401e-a1f3-edda4e6b85af>\",\"WARC-IP-Address\":\"87.98.255.3\",\"WARC-Target-URI\":\"http://jarnoralli.com/code/optical-flow-code\",\"WARC-Payload-Digest\":\"sha1:LRGBL7BA5DWGEMVBPI7GZLWQBOVPPQUQ\",\"WARC-Block-Digest\":\"sha1:KFPVJYRS5QDC5SZ4AAFOWMUCQNI7SUP6\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-10/CC-MAIN-2020-10_segments_1581875142323.84_warc_CC-MAIN-20200217115308-20200217145308-00306.warc.gz\"}"} |
https://calculator.academy/duct-velocity-calculator/ | [
"Enter the air CFM (cubic feet per minute) and the duct cross-sectional area into the calculator to determine the duct velocity.\n\n## Duct Velocity Formula\n\nThe following formula is used to calculate the linear air velocity through a duct.\n\nV = CFM / A\n\n• Where V is the duct velocity (FPM)\n• CFM is the volumetric flow rate of air through the duct (typically cubic feet per minute)\n• A is the cross-sectional area (ft^2)\n\n## Duct Velocity Definition\n\nWhat is a duct velocity? A duct velocity is defined as the linear speed at which air is moving through the opening of a duct or air vent. This is the average linear speed of the air since normal airflow is not constant across an entire area.\n\n## Example Problem\n\nHow to calculate duct velocity?\n\n1. First, determine the volumetric flow rate.\n\nThe volumetric flow rate, often denoted CFM (cubic feet per minute) is the total volume of air moving through an area per unit of time. For this problem, the flow rate is 1,500 ft^3/min.\n\n2. Next, determine the cross-sectional area.\n\nFor this example, the cross-sectional area of the duct is 5 ft^2.\n\n3. Finally, calculate the duct velocity.\n\nThe air velocity is then calculated using the formula above. V = 1500 / 5 = 300 ft/min = 5 ft/s."
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https://miphonedoctorofaustin.com/qa/what-happens-when-irr-is-negative.html | [
"",
null,
"# What Happens When IRR Is Negative?\n\n## What does negative return mean?\n\nA negative return occurs when a company or business has a financial loss or lackluster returns on an investment during a specific period of time.\n\nSome businesses report a negative return during their early years because of the amount of capital that initially goes into the business to get it off the ground..\n\n## What are the problems with IRR?\n\nThere are some cases in which the cash flow pattern is such that the calculation of IRR actually ends up giving multiple rates. So instead of having one IRR, we would then have multiple IRR’s. Sometimes the IRR number can even go in the negative indicating that the firm is actually losing value.\n\n## Is NPV better than IRR?\n\nBecause the NPV method uses a reinvestment rate close to its current cost of capital, the reinvestment assumptions of the NPV method are more realistic than those associated with the IRR method. … In conclusion, NPV is a better method for evaluating mutually exclusive projects than the IRR method.\n\n## Is a negative IRR bad?\n\nIt is ok to get a negative IRR. Negative IRR indicates that the sum of post-investment cash flows is less than the initial investment; i.e. the non-discounted cash flows add up to a value which is less than the investment.\n\n## What happens when IRR is negative NPV?\n\nIRR of a given series of cash flows is calculated by discounting them at such rate so that the NPV is zero. Therefore higher the IRR (discounting rate), the lower will be the NPV value even falling below zero( both are inversely related). Negative NPV implies a ‘no-go’ investment as expected returns at not delivered.\n\n## Can IRR be negative in Excel?\n\nExcel allows a user to get a negative internal rate of return of an investment using the IRR function."
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http://www.tweetnotebook.com/Pennsylvania/normalised-mean-square-error-formula.html | [
"",
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"Address 7314 W Ridge Rd, Fairview, PA 16415 (814) 474-1202 http://microsupportcenter.com\n\n# normalised mean square error formula Cranesville, Pennsylvania\n\nA proposal is then made to obtain the desired results by the use of different indices.Discover the world's research11+ million members100+ million publications100k+ research projectsJoin for free Full-text (PDF)DOI: ·Available from: It is also shown that in certain situations, that have not to be considered as limit cases, the “best” condition to get the lowest value of the NMSE is completely different The final step is to determine if the performance of the competing models is statistically different. Papers of Interest:- 1) V.\n\nnormalization by Co Considering Co/Cp and Cp/Cp, i.e. The same data filtering for FAa calculation is applied for NMSE calculation. This gives a simple relation between NMSE and relative $\\ell^2$ error. Full-text · Article · Feb 2016 Gilberto Fernandes JrLuiz F.\n\nThe RMSD represents the sample standard deviation of the differences between predicted values and observed values. Hanna (1988,1989) has pioneered a significant number of these statistics. Back to Table of Contents Drop in your comments and suggestions to mailto:[email protected] | The University of Toledo | | College of Engineering | | Department of Civil Engineering The idea is to find out the quality and reliability of the predictions made by a model when compared to real life data.\n\nKumar, \"Evaluation of the ISC Short Term Model in a Large-Scale Multiple Source Region for Different Stability Classes\", Env. For example, when measuring the average difference between two time series x 1 , t {\\displaystyle x_{1,t}} and x 2 , t {\\displaystyle x_{2,t}} , the formula becomes RMSD = ∑ The quality measurements are the percentage of validation and estimation data unfitness, Akaike's Final Prediction Error (FPE) (Jones, 1975), loss function (Berger, 1985) and mean squared normalized error performance function (MSE) So far, estimation and modeling approaches have enabled a comprehensive understanding of repetitive processes in projects at steady-state.\n\nThough there is no consistent means of normalization in the literature, common choices are the mean or the range (defined as the maximum value minus the minimum value) of the measured The first technique to measure the adjustment degree relative to the current analyzed traffic and DSNSF is the Normalized Mean Square Error (NMSE) (Poli & Cirillo, 1993), which evaluates the difference Similar is the case of Kumar et al (1993) who have used statistical tools to evaluate the prediction of lower flammability distances. Thus, results close to zero indicate excellent traffic characterizations while high values demonstrate that DSNSF is distant from the expected results. \"[Show abstract] [Hide abstract] ABSTRACT: Traffic monitoring and anomaly detection\n\nRetrieved 4 February 2015. ^ \"FAQ: What is the coefficient of variation?\". The bootstrap technique has to be used. To determine the reliability of a model the following criteria suggested by Kumar et al. (1993) could be used. The ideal value for the factor of two should be 1 (100%).\n\nAiming to improve its efficiency, a modification of the Ant Colony Optimization metaheuristic is proposed, which through self-organized agents optimizes the analysis of multidimensional flows attributes and allows it to be So, does anyone know how matlab normalizes the MSE?Many thanks in advance!Hugo 0 Comments Show all comments Tags mseneural networksperformancenormalized Products No products are associated with this question. These approaches underestimate the influence of process repetitiveness, the variation of learning curves and the conservation of processes’ properties. signal-processing share|cite|improve this question asked Sep 10 '13 at 0:59 Gummi F 74119 I guess not.\n\nrows or columns)). Pet buying scam Measuring air density - where is my huge error coming from? The system returned: (22) Invalid argument The remote host or network may be down. Generated Fri, 21 Oct 2016 22:00:07 GMT by s_wx1011 (squid/3.5.20)\n\nNote that air quality scientists and engineers do not use all the performance measures mentioned below. Maximal number of regions obtained by joining n points around a circle by straight lines Questions about convolving/deconvolving with a PSF A crime has been committed! ...so here is a riddle On the other hand, high NMSE values do not necessarily mean that a model is completely wrong. These requirements cause the calibration of models to be a very expensive and often time-consuming study.\n\nNevertheless, most estimation, planning, and scheduling approaches overlook the dynamics of project-based systems in construction. Scott Armstrong & Fred Collopy (1992). \"Error Measures For Generalizing About Forecasting Methods: Empirical Comparisons\" (PDF). By using this site, you agree to the Terms of Use and Privacy Policy. An Error Occurred Unable to complete the action because of changes made to the page.\n\nAn internet search however only shows strange definitions like $$\\frac{ \\sum_i (x_i-y_i)^2}{N\\sum_i (x_i)^2} \\quad\\text{or} \\quad \\frac{N \\sum_i (x_i-y_i)^2}{\\sum_i x_i \\sum_i y_i}$$ Is my interpretation not the standard definition? When an 'NA' value is found at the i-th position in obs OR sim, the i-th value of obs AND sim are removed before the computation. It is written in symbolic form as: iii) Normalized Mean Square Error This statistic emphasizes the scatter in the entire data set and is known as Normalized Mean Square Error Not the answer you're looking for?\n\nBesides, there is the possibility to calculate the same MSE normalized setting 'standard' or 'percent'.I have looked for the algorithm to calculate both of them with no success. Old literature in the fields of science and engineering is full of such examples. Later on correlation coefficient between the observed and predicted values became a popular way of looking at the performance of a model. See all ›40 CitationsSee all ›7 ReferencesShare Facebook Twitter Google+ LinkedIn Reddit Download Full-text PDF On the use of the normalized mean square error in evaluating dispersion model performanceArticle (PDF Available) in Atmospheric\n\nBased on your location, we recommend that you select: . Difference measures represent a quantitative estimate of the size of the differences between observed and predicted values. The resulting detection system was tested with real and simulated data, achieving high detection rates while the false alarm rate remains low.Article · Jan 2016 Luiz Fernando CarvalhoSylvio BarbonLeonardo de Souza Full-text · Conference Paper · Jul 2015 · Expert Systems with ApplicationsRicardo Magno Santos AntunesVicente a.\n\nOn the other hand, high NMSE values do not necessarily mean that a model is completely wrong. Apply Today MATLAB Academy New to MATLAB? Ret_type is a switch to select the return output (1= RMSD (default), 2= NRMSD, 3= CV(RMSD)). Aiming an automated management to detect and prevent potential problems, we present and compare two novel anomaly detection mechanisms based on statistical procedure Principal Component Analysis and the Ant Colony Optimization\n\nRMSD is a good measure of accuracy, but only to compare forecasting errors of different models for a particular variable and not between variables, as it is scale-dependent. Contents 1 Formula In equation form it is represented as: v) Geometric Mean Bias The geometric mean bias ( MG ) ig given by: vi) Geometric Mean Variance The geometric mean variance These are NOT standard definitions for regression/curve-fitting or classification/pattern-recognition."
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https://stackoverflow.com/questions/9909038/formatting-hexadecimal-number-to-short-uuid-in-javascript | [
"# Formatting hexadecimal Number to short UUID in JavaScript\n\nI have a hexadecimal number in javascript. For display purposes, I would like to format the string as:\n\n``````ffffffff-ffff-ffff\n00000000-0000-01ff\n``````\n\n`(8 digits)-(4 digits)-(4 digits)` with padded zeros on the front\n\nI've been trying to write my own loop to format an arbitrary hexadecimal number into this format, but this seems like something that should be available in JavaScript already.\n\nIs there a built-in way to format a hexadecimal number in JavaScript?\n\n• There is unfortunately no way to format such hexadecimal numbers in JavaScript. But check out this link, maybe it helps.\n– Neq\nMar 28, 2012 at 14:05\n\nI would do a two-step process:\n\n1) convert number to 16 digit hex with leading zeros:\n\n``````var i = 12345; // your number\nvar h = (\"000000000000000\" + i.toString(16)).substr(-16);\n``````\n\n``````var result = h.substr(0, 8)+'-'+h.substr(8,4)+'-'+h.substr(12,4);\n``````\n\nIf your number is really a full 64 bits long you should be aware that javascript has only doubles, which top out at around 53 bits of precision. E.g.\n\n``````var i = 0x89abcdef01234567; // a 64-bit constant\nvar h = (\"000000000000000\" + i.toString(16)).substr(-16); // \"89abcdef01234800\"\n``````\n\nSo you probably want to split this into two 32-bit numbers, and format them 8 digits at a time. Then the second caveat strikes: javascript performs bitwise ops on signed 32-bit integers, and this formatting code can't handle negative numbers.\n\n``````var i = 0xffd2 << 16; // actually negative\nvar h = (\"0000000\" + i.toString(16)).substr(-8); // \"0-2e0000\"\n``````\n\nSince it's fairly likely that numbers you want formatted in hexadecimal are the result of bitwise manipulations, the code can be tweaked to print in two's complement instead:\n\n``````var i = 0xffd2 << 16; // actually negative\nvar h = (\"0000000\" + ((i|0)+4294967296).toString(16)).substr(-8); // \"ffd20000\"\n``````\n\nThis produces the hex representation of the bottom 32 bits of the integral part of arbitrary positive and negative numbers. This is probably what you want (it's approximately `printf(\"%08x\")`). Some more corner cases:\n\n``````var i = 1.5; // non-integers are rounded\nvar h = (\"0000000\" + ((i|0)+4294967296).toString(16)).substr(-8); // \"00000001\"\n\nvar i = -1.5; // rounding is towards zero\nvar h = (\"0000000\" + ((i|0)+4294967296).toString(16)).substr(-8); // \"ffffffff\"\n\nvar i = NaN; // not actually a number\nvar h = (\"0000000\" + ((i|0)+4294967296).toString(16)).substr(-8); // \"00000000\"\n``````\n• While `(i|0)+4294967296` will adequately force the number to be in range and unsigned, `i >>> 0` achieves this purpose as well, and it's a lot clearer too. Oct 2, 2020 at 17:15\n\nES6 Version\n\n``````function toPaddedHexString(num, len) {\nstr = num.toString(16);\nreturn \"0\".repeat(len - str.length) + str;\n}\n\n``````\n• This is simplified further by padStart in EMCAScript 2017. `num.toString(16).padStart(len, \"0\")` Dec 4, 2018 at 17:36\n\nThere are two methods for `String` called `padStart` and `padEnd`\n\n``````const num = 15;\n``````\n``````const num = 15;\n``````\n\n## The shortest version as conclusion\n\nFor ID like `00000000-0000-01ff`\n\n``````function createID_8_4_4(s)\n{\nreturn(1e16+s).slice(-16).replace(/^.{8}|.{4}(?!\\$)/g,'\\$&-')\n/*\nOR the version for easy understanding:\nreturn(1e16+s).slice(-16).match(/..../g).join('-').replace('-','')\nreplace on the end replaces only first '-'\n*/\n}\n\nconsole.log(createID_8_4_4('01ff')); //00000000-0000-01ff``````\n\nFor ID like `0000-0000-0000-01ff`\n\n``````function createID_4_4_4_4(s)\n{\nreturn(1e16+s).slice(-16).match(/..../g).join('-')\n}\n\nconsole.log(createID_4_4_4_4('01ff')); //0000-0000-0000-01ff``````\n\ni don't think there is anything related to that in pure javascript, but frameworks provide this method, in ExtJS 3 it is implemented this way\n\n`````` /**\n* Pads the left side of a string with a specified character. This is especially useful\n* for normalizing number and date strings. Example usage:\n* <pre><code>\nvar s = String.leftPad('123', 5, '0');\n// s now contains the string: '00123'\n* </code></pre>\n* @param {String} string The original string\n* @param {Number} size The total length of the output string\n* @param {String} char (optional) The character with which to pad the original string (defaults to empty string \" \")\n* @return {String} The padded string\n* @static\n*/\nleftPad : function (val, size, ch) {\nvar result = String(val);\nif(!ch) {\nch = \" \";\n}\nwhile (result.length < size) {\nresult = ch + result;\n}\nreturn result;\n}\n``````\n• This is just a padding function, what about the hex formatting and the dashes? Mar 28, 2012 at 14:06\n\nI assume the number is already in the form of a string due to the limitations described in hexwab's answer. If it isn't, start the process by getting it into a hex string of arbitrary length (called `str`) using whatever mechanism is appropriate for your situation. Then:\n\n``````function format(str) {\nreturn (1e15+str).slice(-16).match(/^.{8}|.{4}/g).join('-');\n}\n\nconsole.log(format('723e9f4911'))``````\n\n• Very nice and short solution! (+) I wrote a little bit shorted version from your answer. See my answer. Apr 21, 2020 at 15:59\n• @Bharata I love golf! Let's do this. Amended my answer. Apr 21, 2020 at 18:55"
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http://www.webconversiononline.com/radiation-exposure-conversion.aspx | [
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null,
"Convert Radiation Exposure between Coulomb/Kg, Millicoulomb/Kg, Microcoulomb/Kg, Roentgen, Parker, Rep and other radiation exposure measurement units\n Enter radiation exposure quantity, select units and click 'Convert'\n Quantity From To Coulomb/KgMillicoulomb/KgMicrocoulomb/KgRoentgenParkerRep = ? Coulomb/KgMillicoulomb/KgMicrocoulomb/KgRoentgenParkerRep\n Use Radiation Exposure Conversion Wizard Instead? How to use this calculator...Use current calculator (page) to convert Radiation Exposure from Parker to Coulomb/Kg. Simply enter Radiation Exposure quantity and click ‘Convert’. Both Parker and Coulomb/Kg are Radiation Exposure measurement units.For conversion to different Radiation Exposure units, select required units from the dropdown list (combo), enter quantity and click convertFor very large or very small quantity, enter number in scientific notation, Accepted format are 3.142E12 or 3.142E-12 or 3.142x10**12 or 3.142x10^12 or 3.142*10**12 or 3.142*10^12 and like wise\n\n Related ... » Radiation Conversion » Radiation Activity Conversion » Radiation Absorbed Dose Conversion » Isotopes of different elements » Half-life period of different element » Properties of different element » Atomic symbols of different element » Trigonometry Calculator » Logarithm Calculator » Distance between Cities (or Town) » Molecular Weight Calculator » World Time - Find time at different places » BMI Calculator (Body Mass Index) » Body Fat Calculator » BMR Calculator (Find daily calorie requirement) » Waist to Hip Ratio Calculator » Calculate Calories Burned in different activities » Calculate Your Ideal Weight » Weight Management » Due Date Calculator (Pregnancy) » When is Ovulation (Ovulation Calculator) » Pregnancy Calculator » Safe Period Calculator » Birth Control Methods » Find Definition of different Units » List of different measurement Units\n\n Supported Conversion Types ... Acceleration Angle Angular Acceleration Angular Velocity Area Blood Sugar Clothing Size Computer Storage Unit Cooking Volume Cooking Weight Data Transfer Rate Date Density Dynamic Viscosity Electric Capacitance Electric Charge Electric Conductance Electric Conductivity Electric Current Electric Field Strength Electric Potential Electric Resistance Electric Resistivity Energy Energy Density Energy Mass Euro Currency Fluid Concentration Fluid Flow Rate Fluid Mass Flow Rate Force Frequency Fuel Economy Heat Capacity Heat Density Heat Flux Density Heat Transfer Coefficient Illumination Image Resolution Inductance Kinematic Viscosity Length Luminance (Light) Light Intensity Linear Charge Density Linear Current Density Magnetic Field Strength Magnetic Flux Magnetic Flux Density Magnetomotive Force Mass Flux Density Molar Concentration Molar Flow Rate Moment of Inertia Number Permeability Power Prefix Pressure Radiation Radiation Absorbed Radiation Exposure Radioactivity Shoe Size Sound Specific Volume Speed Surface Charge Density Surface Current Density Surface Tension Temperature Thermal Conductivity Thermal Expansion Thermal Resistance Time Torque Volume Volume Charge Density Water Oil Viscosity Weight\n\n Topic of Interest ... Area Astrology Baby Names Banking Birth Control Chemistry Chinese Astrology City Info Electricity Finance Fluids Geography Health Length Magnetism Pregnancy Radiation Scientific Speed Technology Telephone Temperature Time & Date Train Info Volume Weight World Clock Zodiac Astrology Other\n\n Are you looking for ... List of Supported Conversion Types (sorted) Quick Info - Lookup and Reference List of Metric, English & Local Units Definition of different measurement units Conversion Wizards Calculators"
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https://answers.everydaycalculation.com/add-fractions/15-42-plus-8-20 | [
"Solutions by everydaycalculation.com\n\n15/42 + 8/20 is 53/70.\n\n1. Find the least common denominator or LCM of the two denominators:\nLCM of 42 and 20 is 420\n2. For the 1st fraction, since 42 × 10 = 420,\n15/42 = 15 × 10/42 × 10 = 150/420\n3. Likewise, for the 2nd fraction, since 20 × 21 = 420,\n8/20 = 8 × 21/20 × 21 = 168/420",
null,
"Download our mobile app and learn to work with fractions in your own time:"
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https://support.bioconductor.org/p/62039/ | [
"exporting limma log2 data\n1\n0\nEntering edit mode\nJahn Davik ▴ 110\n@jahn-davik-5747\nLast seen 8.0 years ago\n\nDear all,\n\nI am quite new to limma and need to ask how to export the normalized data. I want to use them in graphical data exploration and presenatation. So, I do something like this (following the Mattick Lab post):\n\nlibrary(limma)\n\nx <- read.maimages(targets, path = 'mydirectory', source = 'agilent', green.only =T)\n\ny <- backgroundCorrection(x,method = 'normexp')\n\ny <- normalizeBetweenArrays(y, method = 'quantile')\n\nSo I guess 'y' now contains the log2 expression data.\n\nQuestion: how can I get them out of R and into a, say, tab-delimited text file?\n\nI would be much obliged.\n\nThank you.\n\njd\n\nlimma export log2 data agilent • 2.5k views\n2\nEntering edit mode\n@james-w-macdonald-5106\nLast seen 32 minutes ago\nUnited States\n\nThe object you are calling 'y' is an EList, and y$E contains the normalized data. So you could hypothetically use write.table() to output to a file. But I would recommend that you resist this temptation. There are any number of Bioconductor packages (one of which is limma, the package you are currently using) that are useful for exploration and presentation of your data. In fact I would argue that the easiest and most productive way for you to proceed from here is to keep your data in R and finish the analysis using limma. I can't imagine what you would do with those data that you couldn't do (probably more efficiently) with Bioconductor. If you say what exactly you are trying to do, I am sure we can come up with some pointers. ADD COMMENT 0 Entering edit mode Dear MacDonald, Thanks for the reply. I wanted to extract the data in order to do boxplots of probes of my interest. But if that is possible within limma, advice is greatly appreciated. jd ADD REPLY 0 Entering edit mode I am not sure exactly what you mean by 'boxplots of probes'. I could interpret that to mean that you want to make boxplots for individual probes, across (some or all) samples. Or I could interpret that to mean that you want to make boxplots for each sample, restricted to a set of probes. There isn't any functionality in limma that I know of to make boxplots, but that's because it would be duplication of existing functionality elsewhere in R. Since I don't know exactly what you want, here are some suggestions. In these examples, I will use 'y' as the EList input object. Boxplot of individual probes, all samples: probevec <- <character vector of probe IDs of interest> boxplot(t(y$E[probevec,]), xaxt = \"none\")\naxis(1, seq_len(length(probevec)), probevec, las = 2)\n\nBoxplot of individual probes, separated by groups of samples:\n\nlibrary(lattice)\ngroupfac <- <factor of groups>\n## this can be any vector that has the same value for each sample of a given type. As an example:\ngroupfac <- factor(c(\"Control\",\"Control\",\"Treated\",\"Control\",\"Treated\",\"Treated\"))\nprobes <- t(y$E[probevec,]) forlattice <- data.frame(groupfac = rep(groupfac, length(probevec), probes = colnames(probes)[col(probes)], vals = as.vector(probes)) bwplot(vals~probes|groupfac, forlattice) Boxplot of individual samples, subsetted by a set of probes: boxplot(y$E[probevec,])\n\nDoes that help?\n\n0\nEntering edit mode\n\nIt helps. Thank you so much for the feedback.\n\njd"
]
| [
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https://www.aimsciences.org/article/doi/10.3934/dcds.2017187 | [
"",
null,
"",
null,
"",
null,
"",
null,
"August 2017, 37(8): 4379-4390. doi: 10.3934/dcds.2017187\n\n## Livšic theorem for banach rings\n\n 1 Dept. of Math & Computer Science, St. John's University, Queens, NY, USA 2 Deptartment of Mathematics, The Pennsilvania State University, University Park, PA, USA\n\nReceived November 2016 Revised May 2017 Published April 2017\n\nThe Livšic Theorem for Hölder continuous cocycles with values in Banach rings is proved. We consider a transitive homeomorphism ${\\sigma :X\\to X}$ that satisfies the Anosov Closing Lemma and a Hölder continuous map ${a:X\\to B^\\times}$ from a compact metric space $X$ to the set of invertible elements of some Banach ring $B$. The map $a(x)$ is a coboundary with a Hölder continuous transition function if and only if $a(\\sigma^{n-1}p)\\ldots a(\\sigma p)a(p)$ is the identity for each periodic point $p=\\sigma^n p$.\n\nCitation: Genady Ya. Grabarnik, Misha Guysinsky. Livšic theorem for banach rings. Discrete & Continuous Dynamical Systems - A, 2017, 37 (8) : 4379-4390. doi: 10.3934/dcds.2017187\n##### References:\n H. Bercovici and V. Nitica, A Banach algebra version of the Livšic theorem, Discr. Contin. Dyn. Syst., 4 (1998), 523-534. doi: 10.3934/dcds.1998.4.523.",
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null,
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"Google Scholar\n Habibulla Akhadkulov, Akhtam Dzhalilov, Konstantin Khanin. Notes on a theorem of Katznelson and Ornstein. Discrete & Continuous Dynamical Systems - A, 2017, 37 (9) : 4587-4609. doi: 10.3934/dcds.2017197 Stefano Bianchini, Daniela Tonon. A decomposition theorem for $BV$ functions. Communications on Pure & Applied Analysis, 2011, 10 (6) : 1549-1566. doi: 10.3934/cpaa.2011.10.1549 Henk Broer, Konstantinos Efstathiou, Olga Lukina. A geometric fractional monodromy theorem. Discrete & Continuous Dynamical Systems - S, 2010, 3 (4) : 517-532. doi: 10.3934/dcdss.2010.3.517 John Hubbard, Yulij Ilyashenko. A proof of Kolmogorov's theorem. Discrete & Continuous Dynamical Systems - A, 2004, 10 (1&2) : 367-385. doi: 10.3934/dcds.2004.10.367 Rabah Amir, Igor V. Evstigneev. On Zermelo's theorem. Journal of Dynamics & Games, 2017, 4 (3) : 191-194. doi: 10.3934/jdg.2017011 Cristina Stoica. An approximation theorem in classical mechanics. Journal of Geometric Mechanics, 2016, 8 (3) : 359-374. doi: 10.3934/jgm.2016011 Fabrizio Colombo, Irene Sabadini, Frank Sommen. The inverse Fueter mapping theorem. Communications on Pure & Applied Analysis, 2011, 10 (4) : 1165-1181. doi: 10.3934/cpaa.2011.10.1165 Hahng-Yun Chu, Se-Hyun Ku, Jong-Suh Park. Conley's theorem for dispersive systems. Discrete & Continuous Dynamical Systems - S, 2015, 8 (2) : 313-321. doi: 10.3934/dcdss.2015.8.313 Viktor L. Ginzburg and Basak Z. Gurel. The Generalized Weinstein--Moser Theorem. Electronic Research Announcements, 2007, 14: 20-29. doi: 10.3934/era.2007.14.20 Jinxin Xue. Continuous averaging proof of the Nekhoroshev theorem. Discrete & Continuous Dynamical Systems - A, 2015, 35 (8) : 3827-3855. doi: 10.3934/dcds.2015.35.3827 Dezhong Chen, Li Ma. A Liouville type Theorem for an integral system. Communications on Pure & Applied Analysis, 2006, 5 (4) : 855-859. doi: 10.3934/cpaa.2006.5.855 Sergei Ivanov. On Helly's theorem in geodesic spaces. Electronic Research Announcements, 2014, 21: 109-112. doi: 10.3934/era.2014.21.109 William Clark, Anthony Bloch, Leonardo Colombo. A Poincaré-Bendixson theorem for hybrid systems. Mathematical Control & Related Fields, 2020, 10 (1) : 27-45. doi: 10.3934/mcrf.2019028 Mathias Staudigl. A limit theorem for Markov decision processes. Journal of Dynamics & Games, 2014, 1 (4) : 639-659. doi: 10.3934/jdg.2014.1.639 Oliver Knill. A deterministic displacement theorem for Poisson processes. Electronic Research Announcements, 1997, 3: 110-113. Abdon E. Choque-Rivero, Iván Area. A Favard type theorem for Hurwitz polynomials. Discrete & Continuous Dynamical Systems - B, 2020, 25 (2) : 529-544. doi: 10.3934/dcdsb.2019252 Hans Wilhelm Alt. An abstract existence theorem for parabolic systems. Communications on Pure & Applied Analysis, 2012, 11 (5) : 2079-2123. doi: 10.3934/cpaa.2012.11.2079 Hari Bercovici, Viorel Niţică. A Banach algebra version of the Livsic theorem. Discrete & Continuous Dynamical Systems - A, 1998, 4 (3) : 523-534. doi: 10.3934/dcds.1998.4.523 Mario Jorge Dias Carneiro, Rafael O. Ruggiero. On the graph theorem for Lagrangian minimizing tori. Discrete & Continuous Dynamical Systems - A, 2018, 38 (12) : 6029-6045. doi: 10.3934/dcds.2018260 Yukie Goto, Danielle Hilhorst, Ehud Meron, Roger Temam. Existence theorem for a model of dryland vegetation. Discrete & Continuous Dynamical Systems - B, 2011, 16 (1) : 197-224. doi: 10.3934/dcdsb.2011.16.197\n\n2019 Impact Factor: 1.338"
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https://encyclopediaofmath.org/wiki/Dickman_function | [
"# Dickman function\n\nThe function",
null,
"defined on",
null,
"by the initial condition",
null,
"for",
null,
"and by the differential-delay equation",
null,
"for",
null,
". Interest attaches to this function because of its connection to \"smooth\" numbers, i.e. numbers that are the product of many small prime numbers. Let",
null,
"denote the number of positive integers less than or equal to",
null,
"and free of prime divisors greater than",
null,
". When",
null,
"is much larger than",
null,
", it is a simple matter of inclusion-and-exclusion counting (cf. also Inclusion-exclusion formula) to show that",
null,
", where",
null,
"denotes a prime number. But the error terms grow rapidly, and the \"main\" term gives the wrong answer in the ranges of greatest interest, including the case when",
null,
"is comparable to a fixed fractional power of",
null,
". For this case, K. Dickman found that",
null,
". If, in place of the restriction",
null,
"for",
null,
"one takes the condition",
null,
", the resulting",
null,
"is approximated by",
null,
", where",
null,
"is the Buchstab function, defined by",
null,
",",
null,
", and",
null,
",",
null,
", where for",
null,
"the right-hand derivative has to be taken, [a1]. Unlike",
null,
",",
null,
"oscillates and tends to a positive limit, equal to",
null,
".\n\nThere are two combinatorial identities linking the Dickman function to",
null,
". Early work is based on the Buchstab identity: With",
null,
"denoting a prime number, for",
null,
",",
null,
"The usual heuristic device of replacing a sum over prime numbers by an integral with \"prime density\"",
null,
"and replacing",
null,
"with",
null,
"leads to an identity which, when",
null,
"and",
null,
", simplifies to an integral equivalent to the definition of",
null,
". N.G. de Bruijn carried this idea to its limits in [a2], but accuracy suffers when large and comparable estimated quantities must be subtracted. The more recent Hildebrand identity involves only additions and has the further advantage that the second input is the same",
null,
"throughout:",
null,
"Applications require estimates uniform in",
null,
"; the best known estimate along these lines, due to A. Hildebrand and based on the identity above, is",
null,
"uniformly in",
null,
"and",
null,
". There are similar results for algebraic integers, [a3].\n\nThere are also results concerning the number of smooth integers in an interval, and concerning the distribution of smooth integers into congruence classes [a4], [a5].\n\nThe Riemann hypothesis (cf. Riemann hypotheses) implies",
null,
"[a8].\n\nThe analytical properties of",
null,
"are reasonably well understood; calculus, analysis of the Laplace transform, and the saddle-point method are the key tools. The first extensive analysis is due to De Bruijn, and the function",
null,
"is sometimes termed the Dickman–De Bruijn function. One has [a10]:\n\na)",
null,
"for",
null,
"(so that",
null,
"is positive for all positive",
null,
", and hence, from the definition, decreasing);\n\nb)",
null,
"is log-concave, that is,",
null,
"for",
null,
"and",
null,
"(K. Alladi);\n\nc) The Laplace transform",
null,
"",
null,
"d)",
null,
"as",
null,
".\n\nThe Dickman function is one of a parameterized family of related functions",
null,
", [a12], and a wider class of similar delay-differential equations has been studied in [a7]. A quick and simple bit of Mathematica code suffices to calculate",
null,
"to reasonable accuracy in the interval",
null,
"using step-size",
null,
". This code calculates a table of values of",
null,
"at intervals of length",
null,
", working back recursively into",
null,
":\n\n<tbody> </tbody>",
null,
"",
null,
",",
null,
";",
null,
";",
null,
"",
null,
"How to Cite This Entry:\nDickman function. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Dickman_function&oldid=41921\nThis article was adapted from an original article by D. Hensley (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article"
]
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https://metanumbers.com/16649 | [
"## 16649\n\n16,649 (sixteen thousand six hundred forty-nine) is an odd five-digits prime number following 16648 and preceding 16650. In scientific notation, it is written as 1.6649 × 104. The sum of its digits is 26. It has a total of 1 prime factor and 2 positive divisors. There are 16,648 positive integers (up to 16649) that are relatively prime to 16649.\n\n## Basic properties\n\n• Is Prime? Yes\n• Number parity Odd\n• Number length 5\n• Sum of Digits 26\n• Digital Root 8\n\n## Name\n\nShort name 16 thousand 649 sixteen thousand six hundred forty-nine\n\n## Notation\n\nScientific notation 1.6649 × 104 16.649 × 103\n\n## Prime Factorization of 16649\n\nPrime Factorization 16649\n\nPrime number\nDistinct Factors Total Factors Radical ω(n) 1 Total number of distinct prime factors Ω(n) 1 Total number of prime factors rad(n) 16649 Product of the distinct prime numbers λ(n) -1 Returns the parity of Ω(n), such that λ(n) = (-1)Ω(n) μ(n) -1 Returns: 1, if n has an even number of prime factors (and is square free) −1, if n has an odd number of prime factors (and is square free) 0, if n has a squared prime factor Λ(n) 9.72011 Returns log(p) if n is a power pk of any prime p (for any k >= 1), else returns 0\n\nThe prime factorization of 16,649 is 16649. Since it has a total of 1 prime factor, 16,649 is a prime number.\n\n## Divisors of 16649\n\n2 divisors\n\n Even divisors 0 2 2 0\nTotal Divisors Sum of Divisors Aliquot Sum τ(n) 2 Total number of the positive divisors of n σ(n) 16650 Sum of all the positive divisors of n s(n) 1 Sum of the proper positive divisors of n A(n) 8325 Returns the sum of divisors (σ(n)) divided by the total number of divisors (τ(n)) G(n) 129.031 Returns the nth root of the product of n divisors H(n) 1.99988 Returns the total number of divisors (τ(n)) divided by the sum of the reciprocal of each divisors\n\nThe number 16,649 can be divided by 2 positive divisors (out of which 0 are even, and 2 are odd). The sum of these divisors (counting 16,649) is 16,650, the average is 8,325.\n\n## Other Arithmetic Functions (n = 16649)\n\n1 φ(n) n\nEuler Totient Carmichael Lambda Prime Pi φ(n) 16648 Total number of positive integers not greater than n that are coprime to n λ(n) 16648 Smallest positive number such that aλ(n) ≡ 1 (mod n) for all a coprime to n π(n) ≈ 1927 Total number of primes less than or equal to n r2(n) 8 The number of ways n can be represented as the sum of 2 squares\n\nThere are 16,648 positive integers (less than 16,649) that are coprime with 16,649. And there are approximately 1,927 prime numbers less than or equal to 16,649.\n\n## Divisibility of 16649\n\n m n mod m 2 3 4 5 6 7 8 9 1 2 1 4 5 3 1 8\n\n16,649 is not divisible by any number less than or equal to 9.\n\n• Arithmetic\n• Prime\n• Deficient\n\n• Polite\n\n• Prime Power\n• Square Free\n\n## Base conversion (16649)\n\nBase System Value\n2 Binary 100000100001001\n3 Ternary 211211122\n4 Quaternary 10010021\n5 Quinary 1013044\n6 Senary 205025\n8 Octal 40411\n10 Decimal 16649\n12 Duodecimal 9775\n20 Vigesimal 21c9\n36 Base36 cuh\n\n## Basic calculations (n = 16649)\n\n### Multiplication\n\nn×i\n n×2 33298 49947 66596 83245\n\n### Division\n\nni\n n⁄2 8324.5 5549.67 4162.25 3329.8\n\n### Exponentiation\n\nni\n n2 277189201 4614923007449 76833853151018401 1279206821111305358249\n\n### Nth Root\n\ni√n\n 2√n 129.031 25.5346 11.3592 6.98679\n\n## 16649 as geometric shapes\n\n### Circle\n\n Diameter 33298 104609 8.70816e+08\n\n### Sphere\n\n Volume 1.93309e+13 3.48326e+09 104609\n\n### Square\n\nLength = n\n Perimeter 66596 2.77189e+08 23545.2\n\n### Cube\n\nLength = n\n Surface area 1.66314e+09 4.61492e+12 28836.9\n\n### Equilateral Triangle\n\nLength = n\n Perimeter 49947 1.20026e+08 14418.5\n\n### Triangular Pyramid\n\nLength = n\n Surface area 4.80106e+08 5.43874e+11 13593.9\n\n## Cryptographic Hash Functions\n\nmd5 bd896f3dbc16b0042625fbf0a8ab8b3a 74e0468cab3eff3280ec3bd2316121e29878476a b856aac2f8db97177fc96cdb7c7df3c1913ac76a9ee41240a1df79d40951512b f2d58d9e44c936d1dfeaa34b7abb3e3506bd267484748d09545c794d1a84d84b3195c24d9d50afdfed9bd5fcbd1d55ad3111a3ebf4f8df3fd5afa837bf86dd8f e80beee40e81aae44105cb9c7df9817a813b929a"
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https://www.dml.cz/handle/10338.dmlcz/703068 | [
"# Article\n\nKeywords:\ngeneralized Newtonian fluids; Navier-Stokes equations; OpenFOAM; bypass\nSummary:\nThe aim of this work is to present numerical results of non-Newtonian fluid flow in a model of bypass. Different angle of a connection between narrowed channel and the bypass graft is considered. Several rheology viscosity models were used for the non-Newtonian fluid, namely the modified Cross model and the Carreau-Yasuda model. The results of non-Newtonian fluid flow are compared to the results of Newtonian fluid. The fundamental system of equations is the generalized system of Navier-Stokes equations for incompressible laminar flow. Generalized Newtonian fluids flow in the bypass is numerically simulated by using an open source CFD tool, OpenFOAM."
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http://mathcentral.uregina.ca/QandQ/topics/pick%20a%20number | [
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"Pick a number greater than 1 2004-06-25",
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"From A student:I understand that when you pick a number greater than 1 and less than 10; multiply it by 7 and add 23, then add the digits of that number until you get a one digit number. Then multiply that number by 9, add the digits of that number until you get a one digit number, subtract 3 from that number and divide the difference by 3; that this process will always give you the result of 2. Does this have a name or theory for it as to why the answer will always be 2?Answered by Penny Nom.",
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https://ncatlab.org/schreiber/show/Rational+parameterized+stable+homotopy+theory | [
"# Schreiber Rational parameterized stable homotopy theory\n\nReferences\n\nAn article that we are writing:\n\n• Rational parameterized stable homotopy theory\n\nAbstract We combine Quillen-Sullivan’s classical rational homotopy theory with Schwede-Shipley’s stable homotopy theory of HR-module spectra to prove that rational parameterized spectra over a rational parameter space are equivalently modeled by the homotopy theory of dg(co-)modules over the Quillen-Sullivan dg(co-)algebras that models the parameter spaces. This implies also that rational parameterized spectra form a full subcategory of the slice homotopy theory of unbounded $L_\\infty$-algebras, thereby extending Hinich‘s embedding of rational homotopy theory in $L_\\infty$-algebras from non-negative to undounded degrees. Minimal models of augmented Sulllivan algebras regarded just as minimal dg-modules over the base algebra have been studied before by A. Roig, and our result shows that these are models for the fiberwise suspension spectra of the corresponding rational fibration.\n\nAn interesting example is the fiberwise suspension spectrum over the 3-sphere of the homotopy quotient of the 4-sphere $S^4 \\simeq S(\\mathbb{R} \\oplus \\mathbb{H})$ by the circle action: this turns out to contain a copy of twisted K-theory, rationally: $\\Sigma^\\infty_{S^3} (S^4/S^1) \\underset{\\mathbb{Q}}{\\simeq} ku/BU(1) \\oplus \\cdots$.\n\n$\\,$"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.851294,"math_prob":0.98472875,"size":1308,"snap":"2022-05-2022-21","text_gpt3_token_len":293,"char_repetition_ratio":0.15260737,"word_repetition_ratio":0.0,"special_character_ratio":0.18425076,"punctuation_ratio":0.075555556,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9881253,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-05-24T19:46:12Z\",\"WARC-Record-ID\":\"<urn:uuid:142a28f4-225c-4359-a2f2-8725f01203a3>\",\"Content-Length\":\"17233\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ac9e679d-6018-4f2d-88a9-bd1adf1c6d1a>\",\"WARC-Concurrent-To\":\"<urn:uuid:7b509c9a-9ddb-4811-a468-e10bd23ac68b>\",\"WARC-IP-Address\":\"172.67.177.13\",\"WARC-Target-URI\":\"https://ncatlab.org/schreiber/show/Rational+parameterized+stable+homotopy+theory\",\"WARC-Payload-Digest\":\"sha1:ZERPXC5YM4X5FLBOVQIU5DSJH7GXBHEO\",\"WARC-Block-Digest\":\"sha1:4RQWRISZZBAHRPSKFVEBTG63Q7HOZ77Z\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-21/CC-MAIN-2022-21_segments_1652662573189.78_warc_CC-MAIN-20220524173011-20220524203011-00146.warc.gz\"}"} |
https://www.colorhexa.com/b2220c | [
"#b2220c Color Information\n\nIn a RGB color space, hex #b2220c is composed of 69.8% red, 13.3% green and 4.7% blue. Whereas in a CMYK color space, it is composed of 0% cyan, 80.9% magenta, 93.3% yellow and 30.2% black. It has a hue angle of 8 degrees, a saturation of 87.4% and a lightness of 37.3%. #b2220c color hex could be obtained by blending #ff4418 with #650000. Closest websafe color is: #993300.\n\n• R 70\n• G 13\n• B 5\nRGB color chart\n• C 0\n• M 81\n• Y 93\n• K 30\nCMYK color chart\n\n#b2220c color description : Dark red.\n\n#b2220c Color Conversion\n\nThe hexadecimal color #b2220c has RGB values of R:178, G:34, B:12 and CMYK values of C:0, M:0.81, Y:0.93, K:0.3. Its decimal value is 11674124.\n\nHex triplet RGB Decimal b2220c `#b2220c` 178, 34, 12 `rgb(178,34,12)` 69.8, 13.3, 4.7 `rgb(69.8%,13.3%,4.7%)` 0, 81, 93, 30 8°, 87.4, 37.3 `hsl(8,87.4%,37.3%)` 8°, 93.3, 69.8 993300 `#993300`\nCIE-LAB 38.964, 55.437, 47.902 19, 10.638, 1.401 0.612, 0.343, 10.638 38.964, 73.266, 40.829 38.964, 110.408, 28.111 32.616, 46.902, 20.285 10110010, 00100010, 00001100\n\nColor Schemes with #b2220c\n\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #0c9cb2\n``#0c9cb2` `rgb(12,156,178)``\nComplementary Color\n• #b20c49\n``#b20c49` `rgb(178,12,73)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #b2750c\n``#b2750c` `rgb(178,117,12)``\nAnalogous Color\n• #0c49b2\n``#0c49b2` `rgb(12,73,178)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #0cb275\n``#0cb275` `rgb(12,178,117)``\nSplit Complementary Color\n• #220cb2\n``#220cb2` `rgb(34,12,178)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #0cb222\n``#0cb222` `rgb(12,178,34)``\n• #b20c9c\n``#b20c9c` `rgb(178,12,156)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #0cb222\n``#0cb222` `rgb(12,178,34)``\n• #0c9cb2\n``#0c9cb2` `rgb(12,156,178)``\n• #6a1407\n``#6a1407` `rgb(106,20,7)``\n• #821909\n``#821909` `rgb(130,25,9)``\n• #9a1d0a\n``#9a1d0a` `rgb(154,29,10)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #ca270e\n``#ca270e` `rgb(202,39,14)``\n• #e22b0f\n``#e22b0f` `rgb(226,43,15)``\n• #f0371b\n``#f0371b` `rgb(240,55,27)``\nMonochromatic Color\n\nAlternatives to #b2220c\n\nBelow, you can see some colors close to #b2220c. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #b20c1f\n``#b20c1f` `rgb(178,12,31)``\n• #b20c12\n``#b20c12` `rgb(178,12,18)``\n• #b2140c\n``#b2140c` `rgb(178,20,12)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #b2300c\n``#b2300c` `rgb(178,48,12)``\n• #b23e0c\n``#b23e0c` `rgb(178,62,12)``\n• #b24c0c\n``#b24c0c` `rgb(178,76,12)``\nSimilar Colors\n\n#b2220c Preview\n\nThis text has a font color of #b2220c.\n\n``<span style=\"color:#b2220c;\">Text here</span>``\n#b2220c background color\n\nThis paragraph has a background color of #b2220c.\n\n``<p style=\"background-color:#b2220c;\">Content here</p>``\n#b2220c border color\n\nThis element has a border color of #b2220c.\n\n``<div style=\"border:1px solid #b2220c;\">Content here</div>``\nCSS codes\n``.text {color:#b2220c;}``\n``.background {background-color:#b2220c;}``\n``.border {border:1px solid #b2220c;}``\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, #0d0201 is the darkest color, while #fffaf9 is the lightest one.\n\n• #0d0201\n``#0d0201` `rgb(13,2,1)``\n• #1f0602\n``#1f0602` `rgb(31,6,2)``\n• #310903\n``#310903` `rgb(49,9,3)``\n• #440d05\n``#440d05` `rgb(68,13,5)``\n• #561006\n``#561006` `rgb(86,16,6)``\n• #681407\n``#681407` `rgb(104,20,7)``\n• #7b1708\n``#7b1708` `rgb(123,23,8)``\n• #8d1b0a\n``#8d1b0a` `rgb(141,27,10)``\n• #a01e0b\n``#a01e0b` `rgb(160,30,11)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #c4260d\n``#c4260d` `rgb(196,38,13)``\n• #d7290e\n``#d7290e` `rgb(215,41,14)``\n• #e92d10\n``#e92d10` `rgb(233,45,16)``\n• #f0391d\n``#f0391d` `rgb(240,57,29)``\n• #f1492f\n``#f1492f` `rgb(241,73,47)``\n• #f25941\n``#f25941` `rgb(242,89,65)``\n• #f36954\n``#f36954` `rgb(243,105,84)``\n• #f57966\n``#f57966` `rgb(245,121,102)``\n• #f68979\n``#f68979` `rgb(246,137,121)``\n• #f7998b\n``#f7998b` `rgb(247,153,139)``\n• #f8a99d\n``#f8a99d` `rgb(248,169,157)``\n• #fabab0\n``#fabab0` `rgb(250,186,176)``\n• #fbcac2\n``#fbcac2` `rgb(251,202,194)``\n``#fcdad4` `rgb(252,218,212)``\n• #fdeae7\n``#fdeae7` `rgb(253,234,231)``\n• #fffaf9\n``#fffaf9` `rgb(255,250,249)``\nTint Color Variation\n\nTones of #b2220c\n\nA tone is produced by adding gray to any pure hue. In this case, #625d5c is the less saturated color, while #b91d05 is the most saturated one.\n\n• #625d5c\n``#625d5c` `rgb(98,93,92)``\n• #695855\n``#695855` `rgb(105,88,85)``\n• #70524e\n``#70524e` `rgb(112,82,78)``\n• #784d46\n``#784d46` `rgb(120,77,70)``\n• #7f483f\n``#7f483f` `rgb(127,72,63)``\n• #864238\n``#864238` `rgb(134,66,56)``\n• #8d3d31\n``#8d3d31` `rgb(141,61,49)``\n• #953729\n``#953729` `rgb(149,55,41)``\n• #9c3222\n``#9c3222` `rgb(156,50,34)``\n• #a32d1b\n``#a32d1b` `rgb(163,45,27)``\n• #ab2713\n``#ab2713` `rgb(171,39,19)``\n• #b2220c\n``#b2220c` `rgb(178,34,12)``\n• #b91d05\n``#b91d05` `rgb(185,29,5)``\nTone Color Variation\n\nColor Blindness Simulator\n\nBelow, you can see how #b2220c 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"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.51380366,"math_prob":0.706406,"size":3652,"snap":"2019-26-2019-30","text_gpt3_token_len":1647,"char_repetition_ratio":0.12746711,"word_repetition_ratio":0.011111111,"special_character_ratio":0.5605148,"punctuation_ratio":0.23516238,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9867699,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-06-25T20:43:16Z\",\"WARC-Record-ID\":\"<urn:uuid:efb469bc-7db6-4fd5-bc85-6d8cbf932957>\",\"Content-Length\":\"36366\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:b7c933fb-c95b-4dc3-a210-5d8e5e7964a6>\",\"WARC-Concurrent-To\":\"<urn:uuid:631661b8-f51f-45a0-939d-b2716636eea3>\",\"WARC-IP-Address\":\"178.32.117.56\",\"WARC-Target-URI\":\"https://www.colorhexa.com/b2220c\",\"WARC-Payload-Digest\":\"sha1:W5T2OGYMJ2TT7KJWZ6SWD667YQ4PDUFK\",\"WARC-Block-Digest\":\"sha1:ZQB3PN37LTKU4DJ5WOXZVROXD7HVRH7D\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-26/CC-MAIN-2019-26_segments_1560627999946.25_warc_CC-MAIN-20190625192953-20190625214953-00109.warc.gz\"}"} |
https://www.tradingmasters.io/cfd-course/moving-average | [
"Another function that can be used in charts for online trading is the moving average, which is widely used for the analysis of story series and especially for technical analysis. On the trading platforms (we recommend this one) you can set this type of graphic function and usually find three types: simple, exponential, and weighted.\n\nIn this lesson we will detail what these three types of moving averages are and how they differ, without going too far into technical details that you can explore personally later depending on your needs.\n\n## Simple Moving Average\n\nThe simple moving average (SMA) is also called arithmetic average and is in fact the most widely used by analysts and by those who trade online. The data of a given period is used and the average is calculated simply by adding it together and dividing the total by the number of values (e.g., 3 + 5 + 6 + 8 and divided by 4). However, the simple moving average is subject to criticism because it assigns the same importance (or weight) to each value. In practice, if we had a 10-period moving average, the same weight would be given to every single value (each of the 10 periods is 10%).\n\n## Weighted Moving Average\n\nThe weighted moving average (WMA) is used to address the previously highlighted problem with the simple moving average. Greater weight is given to the last values of a series. As for the final calculation, this remains unchanged: all the values of the same series are added together. For example, if we had 10 periods we would associate “weight” 1 to the first value, “weight” 2 to the second, and so on. These “weights” must be multiplied by the value of the data. For example, if the first period has a value of 3, we will multiply it by weight 1 and it will ultimately have a value of 3. If the fifth period is 7, we will multiply it by 5 and obtain a last value of 35. In the end, we add up the final values and divide them by the sum of the weights used. Example with three periods (5-6-7): the result will be [(5 × 1) + (6 × 2) + (7 × 3) / (1 + 2 + 3)] or 38/6 = 6.3333.\n\nEven this is subject to criticism because it fails to instantaneously provide an idea of what is happening on the market.\n\n## Exponential Moving Average\n\nThe exponential moving average (EMA) is much more complex than the averages described above and is therefore used by more experienced users. As in the weighted average, a different weight is assigned to the various prices (or values) being considered, greater for the most recent and lesser for the oldest, with the major difference being that it takes into account much more data (e.g., many “older” values).\n\nBeing a very difficult calculation medium, it is practically impossible to generate except through the use of a computer. By the way, we can get a perfect EMA with a single mouse clic, on the trading platform.\n\nHowever, to calculate the exponential moving average two values are taken into consideration:\n\n• The arithmetic mean (seen previously)\n• The Alpha coefficient, which will make the average more reactive.\n\nTo calculate Alpha, use this formula:\n\nAlpha = 2/(n + 1) where n is the number of periods.\n\nThe exponential moving average is obtained by:\n\nEMA (exp. M.) = (Close – previous EMA) * Alpha + previous EMA\n\nWith respect to the weighted average, the weighting coefficients are assigned with an exponential and non-linear progressive value. The difference in “weight” between the different values, therefore, varies exponentially.\n\nGo to lesson 15 – Alligator indicator"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9408227,"math_prob":0.99077666,"size":3480,"snap":"2019-35-2019-39","text_gpt3_token_len":774,"char_repetition_ratio":0.13636364,"word_repetition_ratio":0.009803922,"special_character_ratio":0.23103449,"punctuation_ratio":0.09985097,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9977535,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-09-21T11:51:11Z\",\"WARC-Record-ID\":\"<urn:uuid:934b67ae-5e6c-408a-a70a-119cc4b06879>\",\"Content-Length\":\"91094\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:247b1d12-d1ed-4ca3-9ea2-dee5085b47a0>\",\"WARC-Concurrent-To\":\"<urn:uuid:47331dac-d4de-40ff-89ed-a388a7f8b372>\",\"WARC-IP-Address\":\"104.18.55.123\",\"WARC-Target-URI\":\"https://www.tradingmasters.io/cfd-course/moving-average\",\"WARC-Payload-Digest\":\"sha1:DPBWSHWUEEU5YEDBFS72DFF52AOHSNVS\",\"WARC-Block-Digest\":\"sha1:4Q7TBVDQ3DWFETKDUUSGRBBYKFADAEGS\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-39/CC-MAIN-2019-39_segments_1568514574409.16_warc_CC-MAIN-20190921104758-20190921130758-00068.warc.gz\"}"} |
https://www.cuemath.com/ncert-solutions/direct-and-inverse-proportions-class-8-maths/ | [
"# NCERT Class 8 Maths Direct and Inverse Proportions\n\nThe chapter 13 begins with an introduction to Direct and Inverse Proportions by citing situations in our day-to-day life, where variation in one quantity bringing in variation in the other to delve into the subject of interest.After this , Direct Proportion is explained by stating some real-life scenario and there are some related examples to dig deep into it.Similarly, Inverse Proportion i.e if one quantity increases, the other quantity decreases and vice versa, is also discussed in the same manner with some real-life examples and both of them have some exercise problems to work on.\n\nDownload FREE PDF of Chapter-13 Direct and Inverse Proportions\n\n## Chapter 13 Ex.13.1 Question 1\n\nFollowing are the car parking charges near a railway station up to:\n\n$$4$$ hours ₹$$60$$\n\n$$8$$ hours ₹$$100$$\n\n$$12$$ hours ₹$$140$$\n\n$$24$$ hours ₹$$180$$\n\nCheck if the parking charges are in direct proportion to the parking time.\n\n### Solution\n\nWhat is Known?\n\nParking charges for different hours.\n\nWhat is Unknown?\n\nParking charges are direct proportion to the parking time or not.\n\nReasoning:\n\nIf two quantities are related in such a way that an increase in one lead to a corresponding proportional increase in the other, then such a variation is called direct variation.\n\nSteps:\n\nThe parking charge for $$1$$ hour in all the four cases then the variation is direct.\n\nWe have:\n\n\\begin{align}\\frac{{60}}{4}&=\\frac{{15}}{1}\\\\&=15\\\\ \\\\ \\frac{{100}}{8}&=\\frac{{25}}{2}\\\\ &= 12.5\\\\ \\\\ \\frac{{140}}{{12}} &=\\frac{{35}}{3}\\\\&=11.67 \\\\ \\\\\\frac{{180}}{{24}}&=\\frac{{15}}{2}\\\\&= 7.50\\end{align}\n\nSince all the values are not the same, the parking charges are not in direct proportion to parking times.\n\n## Chapter 13 Ex.13.1 Question 2\n\nA mixture of paint is prepared by mixing $$1$$ part of red pigments with $$8$$ parts of base. In the following table find the parts of base that needed to be added.\n\n Parts of red pigment 1 4 7 12 20 Parts of base 8 ... ... ... ...\n\n### Solution\n\nWhat is Known?\n\nParts of red pigments used.\n\nWhat is Unknown?\n\nParts of base used.\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said to vary in direct proportion if\n\n$\\frac{x}{y} = k,x = yk$\n\nWhere, $$k$$ is a constant.\n\nSteps:\n\nLet the parts of red pigments used be $$x$$ and parts of base used be $$y.$$\n\n\\begin{align}\\therefore \\frac{{{x_1}}}{{{y_1}}} = \\frac{{{x_2}}}{{{y_2}}}\\end{align}\n\nHere\n\n\\begin{align} \\quad{x_1} &= 1, \\qquad {x_2} = 4 \\\\ {y_1} &= 8,\\qquad {y_2} = ?\\\\ \\frac{{{x_1}}}{{{y_1}}} &= \\frac{{{x_2}}}{{{y_2}}} \\\\ \\frac{1}{8} &= \\frac{4}{{y2}}\\\\ \\,{y_2} &= 8 \\times 4 \\\\ &= 32{\\text{ parts }}\\end{align}\n\n$$32$$ parts of base is needed for $$4$$ parts of red pigment.\n\nHere\n\n\\begin{align} {{x}_{1}}&=1,\\quad \\ {{x}_{2}}=7 \\\\ {{y}_{1}}&=8,\\quad{{y}_{2}}=? \\\\ \\frac{{{x}_{1}}}{{{y}_{1}}}&=\\frac{{{x}_{2}}}{{{y}_{2}}} \\\\ \\,\\,\\frac{1}{8}&=\\frac{7}{{{y}^{2}}} \\\\ {{y}_{2}}&=8\\times 7 \\\\ \\,\\,\\,\\,\\,\\,&=56\\,\\ \\text{parts} \\end{align}\n\n$$56$$ parts of base is needed for $$7$$ parts of red pigment.\n\nHere\n\n\\begin{align} \\,\\,\\,\\,\\,\\,\\,\\,{{x}_{1}}&=1,\\quad{{x}_{2}}=12 \\\\ {{y}_{1}}&=8,\\quad{{y}_{2}}=? \\\\ \\frac{{{x}_{1}}}{{{y}_{1}}}&=\\frac{{{x}_{2}}}{{{y}_{2}}} \\\\ \\frac{1}{8}&=\\frac{12}{{{y}_{2}}} \\\\ {{y}_{2}}&=8\\times 12\\quad \\\\ &=96 \\end{align}\n\n$$96$$ parts of base is needed for $$12$$ parts of red pigment.\n\nHere\n\n\\begin{align} {{x}_{1}}&=1,\\quad{{x}_{2}}=20 \\\\ {{y}_{1}}&=8,\\quad{{y}_{2}}=? \\\\ \\frac{{{x}_{1}}}{{{y}_{1}}}&=\\frac{{{x}_{2}}}{{{y}_{2}}} \\\\ \\frac{1}{8}&=\\frac{20}{{{y}_{2}}} \\\\ {{y}_{2}}&=8\\times 20 \\\\ &=160 \\end{align}\n\n$$160$$ parts of base are needed for $$20$$ parts of red pigment.\n\n## Chapter 13 Ex.13.1 Question 3\n\nIn question ($$2$$), above if $$1$$ part of red pigment requires $$75\\,\\rm{ml}$$ of base, how much red pigment should we mix with $$1800\\,\\rm{ml}$$ of base?\n\n### Solution\n\nWhat is Known?\n\n$$1$$ part of red pigment requires $$75\\,\\rm{ml}$$ of base.\n\nWhat is Unknown?\n\n$$1800$$ mL of base needed how much red pigment?\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said to vary in direct proportion if,\n\n\\begin{align}\\frac{x}{y} = k, \\qquad x = y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\nLet the number of parts of red pigment be $$x$$\n\nAs the number of parts of red pigment increases, amount of base also increases in the same ratio. So it is a case of direct proportion.\n\nHere,\n\n\\begin{align} \\frac{{{x}_{1}}}{{{y}_{1}}}&=\\frac{{{x}_{2}}}{{{y}_{2}}} \\\\ {{x}_{1}}&=1,\\qquad {{x}_{2}}=? \\\\ {{y}_{1}}&=8,\\qquad{{y}_{2}}=1800 \\\\ \\frac{1}{75}&=\\frac{{{x}_{2}}}{1800} \\\\ {{x}_{2}}&=\\frac{1\\ \\times \\ 1800}{75} \\\\ {{x}_{2}}&=24 \\end{align}\n\n$$24$$ parts of red pigment should be mixed with $$1800\\,\\rm{ml}$$ of base.\n\n## Chapter 13 Ex.13.1 Question 4\n\nA machine in a soft drink factory fills $$840$$ bottles in $$6$$ hours. How many bottles it will fill in five hours?\n\n### Solution\n\nWhat is Known?\n\n$$840$$ bottles can be filled in $$6$$ hours.\n\nWhat is Unknown?\n\nBottles filled in $$5$$ hours.\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said to be in direct proportion, if\n\n\\begin{align}\\frac{x}{y}=k,\\quad x=y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\n No of bottles Time in hours $${x}_{1}=840$$ $${y}_{1}=6$$ $${x}_{2}=?$$ $${y}_{2}=5$$\n\nSo, the number of bottles filled, and numbers of hours are directly proportional to each other.\n\n\\begin{align} \\frac{{{x}_{1}}}{{{y}_{1}}}&=\\frac{{{x}_{2}}}{{{y}_{2}}} \\\\ \\frac{840}{6}&=\\frac{{{x}_{2}}}{5} \\\\ 6{{x}_{2}}&=840\\,\\times \\,5 \\\\ {{x}_{2}}&=\\frac{840\\times 5}{6} \\\\ {{x}_{2}}&=700 \\end{align}\n\n$$700$$ bottles will be filled in $$5$$ hours.\n\n## Chapter 13 Ex.13.1 Question 5\n\nA photograph of a bacteria is enlarged $$50,000$$ times attains a length of $$5 \\rm{cm}$$ as shown in the diagram. What is the actual length of the bacteria? If the photograph is enlarged $$20,000$$ times only, what would be its enlarged length?\n\n### Solution\n\nWhat is Known?\n\nBacteria enlarged $$50,000$$ times attain a length of $$5 \\,\\rm{cm.}$$\n\nWhat is Unknown?\n\nActual length of the bacteria\n\nif $$20,000$$ times enlarged what will be the length of the bacteria?\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if,\n\n\\begin{align}\\frac{x}{y}=k,\\quad x=y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\n\\begin{align} \\text{Actual length,}\\ l&=\\frac{{{y}_{1}}}{{{x}_{1}}} \\\\ l&=\\frac{5}{50000} \\\\ l&=0.0001\\ \\rm{cm} \\\\ \\end{align}\n\n Number of times enlarged Length attained ${{x_1} = {\\rm{50,000}}}$ ${{y_{\\rm{1}}} = {\\rm{5}}}$ ${{x_2} = {\\rm{20,000}}}$ ${{y_{\\rm{2}}} = {\\rm{?}}}$\n\nThe number of times enlarged is directly proportional to the length attained.\n\nActual length $$= 0.0001 \\,\\rm{cm}$$\n\nEnlarged length will be $$2 \\,\\rm{cm.}$$\n\n## Chapter 13 Ex.13.1 Question 6\n\nIn a model of a ship, the mast is $$9 \\,\\rm{cm}$$ high, while the mast of the actual ship is $$12\\, \\rm{cm}$$ high. If the length of the actual ship is $$28\\;\\rm{m}$$, how long is the model ship?\n\n### Solution\n\nWhat is Known?\n\nThe mast is $$9 \\,\\rm{cm}$$ high while the mast of actual ships is $$12\\, \\rm{cm}$$ high.\n\nWhat is Unknown?\n\nIf the length of the ship is $$28\\;\\rm{m}$$ How long is the model ship?\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if,\n\n\\begin{align}\\frac{x}{y} = k,\\quad x = y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\n Actual ship Model ship $${y}_{1}=12\\;\\rm{m}$$ $${y}_{2}=9\\;\\rm{cm}$$ $${x}_{1}=28\\rm{m}$$ $${x}_{2}=?$$\n\nMore the length of the ship more would be the length of its mast. Hence, this is a direct proportion.\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}} &= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{{28}}{{12}} &= \\frac{{{x_2}}}{9}\\\\12 \\times {x_2} &= 28 \\times 9\\\\{x_2} &= \\frac{{28 \\times 9}}{{12}}\\\\{x_2} &= 21\\;{\\rm{m}}\\end{align}\n\nLength of the model ship is $$21\\;\\rm{ m.}$$\n\n## Chapter 13 Ex.13.1 Question 7\n\nSuppose $$2\\,\\rm{kg}$$ of sugar contains $$9 \\times {10^6}$$ crystals. How many sugar crystals are there in\n\n(1) $$5\\,\\rm{kg}$$ of sugar?\n\n(2) $$1.2\\,\\rm{kg}$$ of sugar?\n\n### Solution\n\n(i) How many crystals are there in $$5\\, \\rm{kg}$$ of crystals?\n\nWhat is Known?\n\n$$2\\,\\rm{kg}$$ of sugar contains $$9 × 10^6$$ crystals.\n\nWhat is Unknown?\n\n(i) $$5\\,\\rm{kg}$$ of sugar contains how many crystals?\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if,\n\n\\begin{align}\\frac{x}{y} = k,\\quad\\;\\; x = yk\\,\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps (i):\n\n Amount of sugar No. of crystals $$2$$ $${9 \\times 10^6}$$ $$5$$ ?\n\nMore the amount of sugar more will be the number of crystals. Hence this is a direct proportion.\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}} &= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{2}{{9 \\times {{10}^6}}}&= \\frac{5}{{{y_2}}}\\\\2 \\times y_2 &= 9 \\times {10^6} \\times 5\\\\ y_2 &= \\frac{{9 \\times {{10}^6} \\times 5}}{2}\\\\{y_2} &= 22.5 \\times {10^6}\\\\{y_2} &= 2.25 \\times {10^7}\\end{align}\n\nHence there are $$2.25 \\times {10^7}$$ crystals.\n\n(ii) How many crystals are there in $$1.2\\,\\rm{kg}$$ of crystals?\n\nWhat is Known?\n\n$$2\\,\\rm{kg}$$ of sugar contains $$9 × 10^6$$ crystals.\n\nWhat is UnKnown?\n\nHow many crystals are there in $$1.2\\,\\rm{kg}$$ of crystals?\n\nSteps (ii):\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}} &= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{2}{{9 \\times {{10}^6}}} &= \\frac{{1.2}}{{{y_2}}}\\\\2 \\times y_2 &= 9 \\times {10^6} \\times 1.2\\\\ y_2 &=\\frac{{9 \\times {{10}^6} \\times 5}}{2}\\\\{y_2} &= 5.4 \\times {10^6}\\end{align}\n\nHence there are $$5.4 \\times {10^6}$$ crystals.\n\n## Chapter 13 Ex.13.1 Question 8\n\nRashmi has a road map with a scale of $$1 \\;\\rm{cm}$$ representing $$18 \\,\\rm{km}$$. She drives on a road for $$72 \\,\\rm{km}$$. What would be her distance covered in the map?\n\n### Solution\n\nWhat is Known:\n\nThe scale of representing $$1\\; \\rm{cm}$$ $$=$$ $$18 \\,\\rm{km}$$\n\nWhat is Unknown:\n\nThe distance covered in map when the distance on road is $$72 \\,\\rm{km.}$$\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if\n\n\\begin{align}\\frac{x}{y} = k,\\, \\qquad x = y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nThe map is a representation of very large region. The scale shows the representation of the actual length and the length represented in map.\n\nSteps:\n\n$$1\\,\\rm{cm}$$ on map represents $$18 \\,\\rm{km}$$ of actual distance then $$2\\, \\rm{cm}$$ on the map represents $$36 \\,\\rm{km}$$. Hence the scale is based on the concept of direct proportion.\n\n\\begin{align}1:18 &= x:72\\\\\\frac{{1}}{18} &= \\frac{x}{{72}}\\\\18 \\times x &= 72 \\times 1\\\\x &= \\frac{{72}}{{18}}\\\\x &= 4\\end{align}\n\nThe distance covered in the map would be $$4 \\,\\rm{cm}$$.\n\n## Chapter 13 Ex.13.1 Question 9\n\nA $$5\\,\\rm{m}$$ $$60\\,\\rm {cm}$$ high vertical pole casts a shadow $$3\\;\\rm{m}$$ $$20 \\;\\rm{cm}$$ long. Find at the same time\n\n(i) Length of the shadow cast by another pole $$10 \\;\\rm{m}$$ $$50 \\;\\rm{cm}$$ high.\n\n(ii) The height of the pole which casts a shadow of $$5\\;\\rm{m}$$ long.\n\n### Solution\n\n(i) Length of the shadow cast by another pole $$10\\; \\rm{m}$$ $$50 \\;\\rm{cm}$$ high.\n\nWaht is Known?\n\n$$5.6\\, \\rm{m}$$ vertical pole casts a shadow of $$3.2\\; \\rm{m}$$ long.\n\nWaht is Unknown?\n\nThe length of a shadow cast by a pole $$10.5\\; \\rm{m}$$ high.\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if\n\n\\begin{align}\\frac{x}{y} = k,\\quad x= y\\,k\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\n Height of the pole Length of the shadow $${5.6{\\rm{m}}}$$ $${3.2{\\rm{m}}}$$ $${10.5{\\rm{m}}}$$ $$?$$\n\nAs the height of the pole increases the length of the shadow also increases. So, it is a direct proportion.\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}}&= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{{5.6}}{{3.2}}&= \\frac{{10.5}}{{{y_2}}}\\\\\\,\\,5.6\\,\\, \\times &= 10.5 \\times 3.2\\\\{y_2}&= \\frac{{10.5 \\times 3.2}}{{5.6}}\\\\ y_2 & = 6\\end{align}\n\nIf the height of the pole is $$10.5\\; \\rm{m}$$, then length of the shadow is $$6\\;\\rm{m}$$.\n\n(ii) The height of the pole which casts a shadow of $$5\\,\\rm{m}$$ long.\n\nWaht is Known?\n\n$$5.6 \\,\\rm{m}$$ vertical pole casts a shadow of $$3.2\\,\\rm{m}$$ long.\n\nWaht is Unknown?\n\nThe height of the pole when the length of the shadow is $$5\\,\\rm{m}$$ long.\n\nSteps:\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}}&= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{{5.6}}{{3.2}}&= \\frac{{{x_2}}}{5}\\\\3.2x &= 5 \\times 5.6\\\\{x_2}&= \\frac{{5 \\times 5.6}}{{3.2}}\\\\{x_2}&= 8.75\\end{align}\n\nIf the height of the pole is $$5\\,\\rm{m}$$, then length of the shadow is $$8.75\\, \\rm{m.}$$\n\n## Chapter 13 Ex.13.1 Question 10\n\nA loaded truck travels $$14\\,\\rm{km}$$ in $$25$$ minutes. If the speed remains the same, how far it travels in $$5$$ hours?\n\n### Solution\n\nWhat is Known?\n\nTruck travels $$14\\,\\rm{km}$$ in $$25$$ minutes.\n\nWhat is Unknown?\n\nDistance travelled in $$5$$ hours.\n\nReasoning:\n\nTwo numbers $$x$$ and $$y$$ are said in direct proportion if,\n\n\\begin{align}\\frac{x}{y} = k,\\quad x = k\\,y\\end{align}\n\nWhere $$k$$ is a constant.\n\nSteps:\n\nIn $$25$$ minutes, it travels $$14 \\,\\rm{km}$$. In $$5$$ hours, it will travel more distance. So, it is a case of direct proportion.\n\n Distance Time in minutes $${{\\rm{14}}}$$ $${{\\rm{25}}}$$ $${\\,{\\rm{?}}}$$ $$5 \\times 60$$ ($$1$$ hour $$=$$ $$60$$ minutes)\n\n[For comparison the unit should be same]\n\n\\begin{align}\\frac{{{x_1}}}{{{y_1}}} &= \\frac{{{x_2}}}{{{y_2}}}\\\\\\frac{{14}}{{25}} &= \\frac{{{x_2}}}{{5 \\times 60}}\\\\25\\,{x_2} &= 5 \\times 60 \\times 14\\\\{x_2} &= \\frac{{5 \\times 60 \\times 14}}{{25}}\\\\{x_2} &= 168\\;{\\rm{km}}\\end{align}\n\nHence the truck can travel $$168 \\,\\rm{km}$$ in $$5$$ hours.\n\nDownload FREE PDF of Chapter-13 Direct and Inverse Proportions\nDirect and Inverse Proportions | NCERT Solutions\nLearn from the best math teachers and top your exams\n\n• Live one on one classroom and doubt clearing\n• Practice worksheets in and after class for conceptual clarity\n• Personalized curriculum to keep up with school"
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https://financetrainingcourse.com/education/tag/var-calculations/ | [
"",
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"# VaR calculations",
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"## Calculating Value at Risk Excel\n\n2 mins read time Calculating Value at Risk Excel Our second course on Risk […]\n\n## Calculating Value at Risk – Approach Specific Steps\n\n5 mins read time Calculating Variance-Covariance (VCV) Value at Risk (VaR) This method assumes […]\n\n## Calculating Value at Risk – Data & Return Series\n\n1 Comment\n\n4 mins read time Methodology Setting the Scene Sample Portfolio Our sample portfolio that […]\n\n## Calculating Value at Risk – Introduction\n\n1 Comment\n\n2 mins read time One of the most pertinent questions in risk management has […]"
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https://www.hindawi.com/journals/amp/2019/4364108/ | [
"/ / Article\n\nResearch Article | Open Access\n\nVolume 2019 |Article ID 4364108 | 6 pages | https://doi.org/10.1155/2019/4364108\n\n# Symmetry, Pulson Solution, and Conservation Laws of the Holm-Hone Equation\n\nRevised06 Jan 2019\nAccepted13 Jan 2019\nPublished03 Feb 2019\n\n#### Abstract\n\nIn this paper, we focus on the Holm-Hone equation which is a fifth-order generalization of the Camassa-Holm equation. It was shown that this equation is not integrable due to the nonexistence of a suitable Lagrangian or bi-Hamiltonian structure and negative results from Painlevé analysis and the Wahlquist-Estabrook method. We mainly study its symmetry properties, travelling wave solutions, and conservation laws. The symmetry group and its one-dimensional optimal system are given. Furthermore, preliminary classifications of its symmetry reductions are investigated. Also we derive some solitary pattern solutions and nonanalytic first-order pulson solution via the ansatz-based method. Finally, some conservation laws for the fifth-order equation are presented.\n\n#### 1. Introduction\n\nIn the study of shallow water waves, Camassa and Holm derived a nonlinear dispersive shallow water wave equation which is called Camassa-Holm (CH) equation now. The here denotes the fluid velocity at time in the direction . Eq. (1) admits bi-Hamiltonian structure and it is completely integrable [3, 4]. What is more, the equation has infinite conservation laws as well as a spike solitary wave solution where is an arbitrary constant. The solitary wave curve of the solution has a cusp at the peak, and the first derivative of the cusp is not continuous. Accordingly, it is called a peakon [6, 7].\n\nWith the further researches on the CH equation, a lot of findings about the equation have been obtained and it is impossible to give a comprehensive overview here. For example, Eq. (1) represents the equation for geodesics on the Bott-Virasoro group and owns the geometric interpretation . The CH equation possesses both global solutions and solutions developing singularities in finite time and the blow-up happens in a way which resembles wave breaking to some extent [9, 10]. The well-developed inverse scattering theory can also be used to integrate the CH flow . In , it was shown that the well-known CH equation is included in the negative order CH hierarchy and a class of new algebro-geometric solutions of the CH equation was presented. Moreover, the time evolution of traveling-wave solutions and the interaction of peaked and cusped waves were numerically studied .\n\nRecently, one of the latest trends is that researchers are trying to generalize the CH equation to higher order, which is also the subject of this paper. In fact, some higher-order CH equations are well considered. For example, Wazwaz studied the nonlinear fourth-order dispersive variants of the generalized CH equation by using sine-cosine method . The existence of global weak solutions was established for a higher-order CH equation describing exponential curves of the manifold of smooth orientation-preserving diffeomorphisms of the unit circle in the plane . Nonsmooth travelling wave solutions of a generalized fourth-order nonlinear CH equation were studied in . In , the CH model was extended to fifth order and some interesting solutions were obtained including explicit single pseudo-peakons, two-peakon, and -peakon solutions.\n\nEspecially, Holm and Hone discussed a fifth-order partial differential equation (PDE)which is a generalization of the integrable CH equation . We will call it the Holm-Hone equation in the following. This fifth-order PDE admits exact solutions in terms of an arbitrary number of superposed pulsons. The pulsons of Eq. (3) are weak solutions with discontinuous second derivatives at isolated points. Numerical simulations show that the pulsons are stable and they dominate the initial value problem and scatter elastically . These characteristics are reminiscent of solitons in integrable systems. However, after demonstrating the nonexistence of a suitable Lagrangian or bi-Hamiltonian structure and obtaining negative results from Painlevé analysis and the Wahlquist-Estabrook method , they asserted that the Holm-Hone equation is not integrable. Consequently, most effective methods for integrable systems are not applicable to this equation. However, the Lie symmetry approach originated from Norwegian mathematician Sophus Lie systematically unifies and extends well-known ad hoc techniques to construct explicit solutions for differential equations, no matter the equations are integrable or not.\n\nActually, there are several important applications of symmetry analysis in the investigation of differential equations . Since some solutions of partial differential equations asymptotically tend to solutions of lower-dimensional equations obtained by symmetry reduction, some of these special solutions illustrate important physical phenomena. In particular, the exact solutions arising from symmetry methods can often be used effectively to study properties such as asymptotics and blow-up. Besides, the explicit solutions found by symmetry methods can play important roles in the design and testing of numerical integrators, and these solutions provide an important practical check on the accuracy and reliability of such integrators.\n\nThis paper is organized as follows. We first present the common form of the infinitesimal generators of the Holm-Hone equation. Then we establish the optimal system of one-dimensional subalgebras and consider the similarity reductions of the equation. Furthermore, the travelling wave solutions are investigated. At last, some conservation laws of the equation are also derived.\n\n#### 2. Lie Symmetries for the Holm-Hone Equation\n\nIn this section, we investigate the Lie symmetries and similarity reductions of the Holm-Hone equation through the classical methods. The infinitesimal generators corresponding to the one-parameter transformation group are presented. Furthermore, the one-dimensional optimal system of the group is derived with the help of the adjoint representation among the vector fields. Finally, the reduced equations are given through the similarity transformation.\n\n##### 2.1. Infinitesimal Generators\n\nWe introduce the infinitesimal form of the single parameter transformation groupwhere is the infinitesimal group parameter and , , are the infinitesimals of the transformation for the independent and dependent variables, respectively. The vector field associated with the above group of transformations can be written as Using the software package GeM , we obtainwhere , , are arbitrary constants. The infinitesimal generators of the corresponding Lie algebra are given by\n\nIn order to obtain the group transformation which is generated by the infinitesimal generators for , we need to solve the first-order ordinary differential equations Exponentiating the infinitesimal symmetries we get the one-parameter groups generated by for as Accordingly, if is a solution of the Holm-Hone equation, so are the functions\n\n##### 2.2. One-Dimensional Optimal System\n\nIn general, the Lie group has infinite subgroups; it is not usually feasible to list all possible group invariant solutions to the system. We need an effective systematic approach to classify these solutions, so the optimal 1-dimensional subalgebras of group invariant solutions can be derived. In this section, the optimal system is obtained by computing the adjoint representation of the vector fields . We use the Lie series where is the commutator for the Lie algebra, is a parameter, and . The commutator table of the Lie point symmetries for Eq. (3) and the adjoint representation of the symmetry group on its Lie algebra are presented in Tables 1 and 2, respectively.\n\n 0 0 0 0 0 0 0\n\nGiven a nonzero vector our task is to simplify as many of the coefficients as possible through judicious applications of adjoint maps to .\n\nFirstly, we suppose that . Scaling if necessary, we can assume that . Referring to Table 2, if we act on such a by , we can make the coefficient of vanish and the coefficients of cannot be eliminated further, so we can make the coefficient of either , , or . Thus any one-dimensional subalgebra spanned by with is equivalent to one spanned by either , , or .\n\nThe remaining one-dimensional subalgebras are spanned by vectors of the above form with . If , we scale to make , and then no coefficient vanishes by any action on , so that is equivalent to .\n\nThe remaining case, , is equivalent to . And it is impossible to make further simplification.\n\nUntil now, we have found the optimal system of one-dimensional subalgebras spanned by\n\nThe list can be reduced slightly if we admit the discrete symmetry , which maps to , and thereby the number of inequivalent subalgebras is reduced to four.\n\n##### 2.3. Similarity Reductions\n\nThe Holm-Hone equation is expressed in the coordinates , so we try to reduce this equation in order to search for its form in specific coordinates which can be constructed by solving the characteristic equationBased on the optimal system presented before, we obtain the following four kinds of reductions:\n\nReduction 1. For , we get the reduction\n\nReduction 2. For , we get the traveling wave reduction , , where satisfies\n\nReduction 3. For , we get the reduction , where satisfies\n\nReduction 4. For , we get the reduction , where satisfies\n\n#### 3. Travelling Wave Solutions of the Holm-Hone Equation\n\nThe appearance of nonanalytic peakon-type solutions has increased the menagerie of solutions appearing in nonlinear partial differential equations, both integrable and nonintegrable. The pulson solutions for Eq. (3) have a finite jump in second derivative of the solutions. In a series of papers, Wazwaz proposed some schemes to determine new sets of soliton solutions, in addition to the peakon solutions obtained before, for the family of CH equations [29, 30]. The method rests mainly on some ansatzes that use one hyperbolic function or combine two hyperbolic functions as follows:\n\n(1) A sinh-cosh Ansatz I\n\n(2) A sinh-cosh Ansatz II\n\n(3) A tanh Ansatz or a coth Ansatz or\n\n(4) The Exponential Peakon Ansatz where , and are parameters that will be determined. By this method, solitons, solitary patterns solutions, periodic solutions, compactons, and peakons solutions for a family of CH equations with distinct parameters are obtained. However, we should modify the first ansatz and combine it into the second one since and . In what follows, we try to describe some specific travelling wave solutions for the Holm-Hone equation via this modified method.\n\nFirstly, we obtain the travelling wave solutions with or and are arbitrary constants. Moreover, it can be easily verified that there is no effective result for the third ansatz for the Holm-Hone equation. And in order to take the last exponential peakon ansatz, we are advised to rewrite Eq. (3) aswith\n\nSupposing that , then Eq. (24) becomeswhereLet us find all possible nonconstant solutions satisfying and . Since , the corresponding characteristic equation is . Then the characteristic values are and , which yield It is easy to see that if and only if Nevertheless, when Then the solution can be reduced to Considering the continuity of solution at , we look for a solution of the following form:where , are arbitrary constants. Next we explore the relationship between the coefficients and . Substituting Eq. (32) into Eq. (27) and using the property we get the travelling wave solution of the original equation This solution is called the first-order pulson solution which is different from the peakons of CH equation. Its first derivative is continuous and the second derivative of the cusp is not continuous.\n\n#### 4. Conservation Laws for the Holm-Hone Equation\n\nConservation laws are widely applied in the analysis of PDEs, particularly in the study of existence, uniqueness, and stability of solutions. The concept of conservation laws and the relationship between symmetries and conservation laws arise in a wide variety of applications and contexts [25, 26].\n\nA conservation law for (3) is of the form where and denote the total derivatives as and the subscripts denote partial derivatives. The vector is a conserved vector for the partial differential equation. It was shown that Eq. (3) has the conservation law where and it does not own bi-Hamiltonian structure . In this section, we mainly solve the conservation laws of the Holm-Hone equation by multiplier method .\n\nA multiplier has the property thatfor all solutions . Generally speaking, each multiplier is a function as , where denotes all th order derivatives of with respect to all independent variables . Here we only consider multipliers of the form , although multipliers which depend on the first-order and higher-order partial derivatives of could also be considered, but the calculations become more complicated and we fail to find any result.\n\nThe right-hand side of (38) is a divergence expression which leads to the determining equation for the multiplier aswhere is the standard Euler operator.\n\nFrom the system (39), we can obtain the solutionwhere and are arbitrary constants. Therefore we get that any conserved vector of the Holm-Hone equation with multiplier of the form is a linear combination of the two conserved vectors\n\n#### 5. Conclusions\n\nIn summary, we have found the most general Lie point symmetries group for the nonintegrable Holm-Hone equation which is a fifth-order generalization of the CH equation. Meanwhile, we constructed the optimal system of one-dimensional subalgebras. Afterwards, we created the preliminary classifications of similarity reductions. The Lie invariants and similarity reduced equations corresponding to infinitesimal symmetries have been obtained. In order to obtain the traveling wave solutions of the equation, we adopted the method of ansatz. We also found some conservation laws from the multiplier method.\n\n#### Data Availability\n\nNo data were used to support this study.\n\n#### Conflicts of Interest\n\nThe authors declare that they have no conflicts of interest.\n\n#### Acknowledgments\n\nThis work is supported by the 13th Five-Year National Key Research and Development Program of China with Grant No. 2016YFC0401407.\n\n1. R. Camassa and D. D. Holm, “An integrable shallow water equation with peaked solitons,” Physical Review Letters, vol. 71, no. 11, pp. 1661–1664, 1993. View at: Publisher Site | Google Scholar | MathSciNet\n2. R. Camassa, D. D. Holm, and J. M. Hyman, “A new integrable shallow water equation,” Advances in Applied Mechanics, vol. 31, pp. 1–33, 1994. View at: Publisher Site | Google Scholar\n3. 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Olver, Applications of Lie Groups to Differential Equations, vol. 107, Springer, New York, NY, USA, 2nd edition, 1993. View at: MathSciNet\n26. G. W. Bluman, A. F. Cheviakov, and S. C. Anco, Applications of Symmetry Methods to Partial Differential Equations, vol. 168 of Applied Mathematical Sciences, Springer, New York, NY, USA, 2010. View at: Publisher Site | MathSciNet\n27. N. H. Ibragimov, Transformation Groups Applied to Mathematical Physics, Higher Education Press, Beijing, China, 2013.\n28. A. F. Cheviakov, “GeM software package for computation of symmetries and conservation laws of differential equations,” Computer Physics Communications, vol. 176, no. 1, pp. 48–61, 2007. View at: Publisher Site | Google Scholar | MathSciNet\n29. A.-M. Wazwaz, “New compact and noncompact solutions for two variants of a modified Camassa-Holm equation,” Applied Mathematics and Computation, vol. 163, no. 3, pp. 1165–1179, 2005. View at: Publisher Site | Google Scholar | MathSciNet\n30. A. M. Wazwaz, “Peakons, kinks, compactons and solitary patterns solutions for a family of Camassa-Holm equations by using new hyperbolic schemes,” Applied Mathematics and Computation, vol. 182, no. 1, pp. 412–424, 2006. View at: Publisher Site | Google Scholar | MathSciNet\n31. S. C. Anco and G. Bluman, “Direct construction of conservation laws from field equations,” Physical Review Letters, vol. 78, no. 15, pp. 2869–2873, 1997. View at: Publisher Site | Google Scholar | MathSciNet\n32. S. C. Anco and G. Bluman, “Direct construction method for conservation laws of partial differential equations part II: general treatment,” European Journal of Applied Mathematics, vol. 13, no. 5, pp. 567–585, 2002. View at: Publisher Site | Google Scholar | MathSciNet\n33. S. C. Anco, “Generalization of Noether’s theorem in modern form to non-variational partial differential equations,” in Recent progress and Modern Challenges in Applied Mathematics, Modeling and Computational Science, vol. 79, pp. 119–182, Fields Institute Communications, 2017. View at: Google Scholar\n\n#### More related articles\n\nWe are committed to sharing findings related to COVID-19 as quickly and safely as possible. Any author submitting a COVID-19 paper should notify us at [email protected] to ensure their research is fast-tracked and made available on a preprint server as soon as possible. We will be providing unlimited waivers of publication charges for accepted articles related to COVID-19. Sign up here as a reviewer to help fast-track new submissions."
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https://jwcn-eurasipjournals.springeropen.com/articles/10.1186/s13638-018-1149-7 | [
"# Random forests for resource allocation in 5G cloud radio access networks based on position information\n\n## Abstract\n\nNext generation 5G cellular networks are envisioned to accommodate an unprecedented massive amount of Internet of things (IoT) and user devices while providing high aggregate multi-user sum rates and low latencies. To this end, cloud radio access networks (CRAN), which operate at short radio frames and coordinate dense sets of spatially distributed radio heads, have been proposed. However, coordination of spatially and temporally denser resources for larger sets of user population implies considerable resource allocation complexity and significant system signalling overhead when associated with channel state information (CSI)-based resource allocation (RA) schemes. In this paper, we propose a novel solution that utilizes random forests as supervised machine learning approach to determine the resource allocation in multi-antenna CRAN systems based primarily on the position information of user terminals. Our simulation studies show that the proposed learning based RA scheme performs comparably to a CSI-based scheme in terms of spectral efficiency and is a promising approach to master the complexity in future cellular networks. When taking the system overhead into account, the proposed learning-based RA scheme, which utilizes position information, outperforms legacy CSI-based scheme by up to 100%. The most important factor influencing the performance of the proposed learning-based RA scheme is antenna orientation randomness and position inaccuracies. While the proposed random forests scheme is robust against position inaccuracies and changes in the propagation scenario, we complement our scheme with three approaches that restore most of the original performance when facing random antenna orientations of the user terminal.\n\n## Introduction\n\nOne of the key challenges with the fifth generation (5G) cellular networking technology is to ensure high data rate provision to all users, irrespective of their location and time of network access. Typically, the service requirements on 5G systems include a 1000 × increase in system capacity compared to Long Term Evolution-Advanced (LTE-A) systems , an end-to-end latency reduction of at least 10 × compared to LTE-A systems , and support for medium- to high-mobility users, with high throughput and always-on connectivity requirements .\n\nDensification of the radio access network (RAN) toward network deployments of high access node density has been suggested to massively increase the system capacity of mobile radio networks. However, a massive densification of the radio access network resources implies high coordination requirements that the existing LTE system architecture cannot meet. For this reason, new network architectures had been proposed, among which the cloud radio access network (CRAN) architecture constitutes a promising solution for implementing dense networks that can achieve fast coordination at relatively moderate costs. In CRAN, the radio access units, which are formed from distributed antenna systems, are separated from the central processing units, that handle all the baseband processing. The central processing units, essentially being small cloud-like data processing units, are also connected to each other through a backbone supporting fast coordination among them. A single unit of the distributed antenna systems is called remote radio head (RRH), which when densely placed with other RRHs in an area of interest forms an antenna domain, and this set up is formally known as ultra-dense network (UDN) deployment . Such UDN deployments allow for tight interference coordination between RRHs, and consequently result in higher system capacity, and thus can achieve the aforementioned targets for 5G communication systems.\n\nServing an unprecedented massive amount of terminals in 5G, comprising Internet-of-things (IoT) and user devices, with five times smaller frame duration than in LTE requires an extensive overhead for the channel state information (CSI) acquisition. Comparing with traditional resource allocation (RA) schemes [7, 8], this overhead becomes excessive for moderate to high speeds of the user terminals, where the channel states fluctuate intensely . On the other hand, the densification implies more terminal connections in line-of-sight (LOS) positions, leading to lower statistical channel variability. This motivates the consideration of alternative non-CSI based RA approaches that utilize pure position information of the terminals in the antenna domain. In , it is shown that RA based on CSI is much more expensive in terms of system overhead compared to location-based RA in the context of device-to-device (D2D) communications. Although position estimation based on, e.g., uplink (UL) pilot reference signals, or beacons, requires a much lower overhead than CSI acquisition, it remains an open research question how such schemes perform in terms of network key performance indicators (KPIs) when benchmarked with CSI-based schemes. Furthermore, it remains to be studied how accurate and complex a realization of a position-based RA is, and how robust it is to the changes in the propagation scenario or to terminal position information inaccuracies.\n\nIn order to address these research issues, we propose the usage of a supervised machine learning approach based on the random forests algorithm. The random forests algorithm is well known for its inherent robustness and superiority over other known supervised learning techniques in case of missing data values [11, 12]. In this article, we model and devise a learning-based RA scheme as centralized solution for resource allocation in 5G systems by using random forests as multi-class classifier. Our solution essentially aims at predicting the modulation and coding scheme (MCS) to be used for a given terminal position. Through numerical evaluations, we study the basic efficiency of the approach which achieves a spectral efficiency performance comparable to CSI-based schemes. By considering the corresponding overhead, we also show that the learning-based approach outperforms CSI-based approaches significantly. We demonstrate the robustness of the proposed scheme with respect to different variations of users’ position accuracy, showing that even for quite large variations the learning-based approach can still provide good performance. In addition we show the increasing accuracy on the system performance that can be achieved by an increasing number of training and test samples. Finally, we study the impact of a random orientation of the user antennas, which may lead to significant performance deterioration, and discuss several compensation schemes, which successfully addresses this challenge.\n\nThe remaining paper is structured in the following manner: Section 2 presents relevant prior art research, while Section 3 presents the system model and the detailed problem statement. Some background information on machine learning and random forests algorithm is presented in Section 4, along with the details for the design of learning-based RA scheme. The performance evaluation of the proposed scheme is then elaborated in Section 5. Finally, Section 6 concludes the article accompanied by a discussion of the future work.\n\n## Related work\n\nOptimizing resource allocation based on terminals’ CSI for multi-antenna systems has been extensively used and studied in the prior art literature where both centralized and distributed solutions have been suggested . To this end, CRAN defines a suitable platform for resource allocation in 5G that may allow for both centralized and distributed control of a common pool of resources belonging to multiple operators or multiple service providers . Despite the recent CRAN advances, related work with respect to machine learning for resource allocation within the context of CRAN is still quite sparse. In , the authors propose a resource allocation scheme based on linearisation of mixed integer non-linear program for mobile users present in 5G CRAN systems, where they formulate the problem as maximization of network throughput, with a constraint on maximum network capacity. The authors in have shown that resource allocation based on CSI is much expensive in terms of system overhead compared to location-based resource allocation scheme in the context of device-to-device (D2D) communications, which are an integral part of 5G system design. In such case, when perfect CSI is used for resource allocation, the system overhead can be as large as about 25% of the system capacity. The authors in use the reinforcement learning, a machine learning technique, for adaptive modulation and coding in orthogonal frequency division multiplex-multiple input, multiple output (OFDM-MIMO) based 5G systems. In our previous work , we used the random forests algorithm as a binary classifier for allocating resources to users present in CRAN-based 5G system. In that case, the random forests classifier was coupled with a system scheduler, which validated the prediction provided by the random forests, and then the appropriate resources were allocated to serve the given set of users in the system. Though we evaluated the robustness of the RA scheme based on the binary random forests classifier for different system parametrization, but the scope of such investigations was quite limited. We thus conclude that all of our above addressed challenges are still open, some of which are investigated in this work.\n\n## System model\n\n### General system components and assumptions\n\nFigure 1 presents the CRAN system, consisting of the following essential components:\n\n• N terminals spread out across the entire CRAN system;\n\n• A number of R remote radio heads (RRHs) serving the terminals; and\n\n• A baseband unit (denoted by ‘BBU’ in Fig. 1) that performs baseband processing in the entire system, and to which all RRHs are connected to by a fast back-haul.\n\nFor simplicity, we consider the case where each RRH is serving only one terminal in the downlink (DL) in a given time frame. It is further assumed that the CRAN system operates in time division duplex (TDD), where time frames of duration Tf are used for a communication link. Each time frame consists of a number of L sub-frames, each of duration Tsub. Orthogonal frequency-division multiplexing (OFDM) waveform is considered, and therefore, each sub-frame consists of a number of symbols Stotal and fsc OFDM sub-carriers. The operating frequency of the system is fc, with a system bandwidth W. Dense deployment of RRHs is considered within the given CRAN system; an example could be placing distributed antenna systems on top of street lights . Terminals are roaming freely within the area with varying velocities and directions. Each RRH and terminal is equipped with ATx and ARx antennas, respectively.\n\nFinally, the following notations are followed in the description of the 5G CRAN system model and throughout the rest of this paper. Bold-faced capital letter, e.g. A, denotes a matrix, whereas bold-faced small letter, e.g., a, denotes a vector. $$\\mathbb {A}$$ denotes a set, whereas A or a denote scalars. (.) denotes the Hermitian of a vector or a matrix, while the transpose of a vector or a matrix is denoted by (.)T.\n\n### Resource allocation and channel model\n\nIn the considered CRAN system, the baseband unit is the central RA unit, which allocates resources on a per-frame basis. First, it performs the assignment of each RRH to the terminals present in the system. Let Xt denote the binary assignment matrix, where each element $$x_{r,n}^{t}$$ denotes the assignment of nth terminals to rth RRH at time t. The assignment of the terminals to RRH, is in the literature referred to as user assignment. Once the user assignment is determined, the baseband unit decides on the selection of a transmit beam $$\\pmb {v}_{r,n}^{t}$$ to be used by the assigned RRH, and also the receive filter $$\\pmb {u}_{r,n}^{t}$$ at the terminal. The transmit beams and receive filters belong to the pre-defined sets of beams, i.e., $$\\pmb {v}_{r,n}^{t}\\in \\mathbb {V}$$ and $$\\pmb {u}_{r,n}^{t}\\in \\mathbb {U}$$, that are available at each RRH and terminal, respectively. Finally, the baseband unit selects a modulation and coding scheme (MCS), $$m_{r,n}^{t}$$ from the set $$\\mathbb {M}$$, for data transmission between each RRH-terminal link. The resource allocation is done by the baseband unit on per-frame basis, where the objective is to maximize the system goodput.\n\nThe propagation scenario is interference-limited, having densely deployed RRHs within the area of interest. Given a certain allocation of terminals to RRHs in the system, combined with the selection of transmit beams and receive filters for each allocation, the signal-to-interference-and-noise ratio (SINR) of a terminal n for a given time t is given by\n\n$$\\begin{array}{*{20}l} \\gamma_{n}^{t} = \\frac{P_{r, n}^{t}}{ \\sigma^{2} + \\sum\\limits_{\\substack{q=1 \\\\ q \\neq r} }^{R} P_{q, n}^{t}}, \\end{array}$$\n(1)\n\nwhere, $$P_{r, n}^{t}$$ is the signal power received by terminal n, from the rth RRH, at time t, $$P_{q, n}^{t}$$ is the signal power received by terminal n, from the qth RRH (other than the rth RRH), at the same time frame t, and σ2 is the noise power. The received signal power $$P_{r, n}^{t}$$ is given by\n\n$$\\begin{array}{*{20}l} P_{r, n}^{t} = \\ P_{\\text{Tx}} \\cdot \\ | (\\pmb{u}_{r,n}^{t})^{\\dagger} \\pmb{H}_{r, n}^{t} \\pmb{v}_{r,n}^{t} |^{2}. \\end{array}$$\n(2)\n\nIn Eq. (2), PTx denotes the transmit power allocated per RRH, and $$\\pmb {H}_{r, n}^{t}$$ is the channel matrix for the time frame t between RRH r and terminal n. Throughout the duration of a frame we assume that the SINR remains constant in both time and frequency.\n\nEach element of the channel matrix $$\\pmb {H}_{r, n}^{t}$$ represents the complex polarimetric channel impulse response between each transmitter antenna element aTx and receiver antenna element aRx, and is denoted by $$H_{a_{\\text {Rx}}, a_{\\text {Tx}}} (t, \\tau)$$. In reality, this channel response is the combination of different path components, i.e., reflection, diffraction, and scattering, which can be modeled as k different multipath components. The channel impulse response is the sum of the impulse responses from k different multipath components, between aTx and aRx antenna elements and is given by\n\n$$\\begin{array}{*{20}l} H_{a_{\\text{Rx}}, a_{\\text{Tx}}} (t, \\tau) = & \\sum\\limits_{k = 1}^{K} \\tilde{\\pmb{h}}_{k, a_{\\text{Rx}}, a_{\\text{Tx}}}(t) \\cdot \\\\ & \\cdot e^{\\frac {j 2 \\pi d_{k} (t)}{\\lambda}} \\delta \\left(\\tau - \\tau_{k, a_{\\text{Rx}}, a_{\\text{Tx}}}(t)\\right). \\end{array}$$\n(3)\n\nHere, K is the total number of multipath components. $$\\tilde {\\pmb {h}}_{k, a_{\\text {Rx}}, a_{\\text {Tx}}}(t)$$ is the impulse response of kth multipath, including the relevant pathloss. λ denotes the wavelength, and d k is the total distance for multipath k at time t. $$\\delta (\\tau - \\tau _{k, a_{\\text {Rx}}, a_{\\text {Tx}}}(t))$$ is the delta function representing the evolution of channel impulse response with respect to different multipath delays $$\\tau _{k, a_{\\text {Rx}}, a_{\\text {Tx}}}$$.\n\nGiven the SINR per time frame, the system utilizes the MCS $$m_{r,n}^{t}$$ chosen by the resource allocation unit, i.e., the baseband unit, to convey backlogged information to the corresponding terminal. This results in a certain spectral efficiency combined with a block error rate $$e_{m_{r,n}^{t}} (\\gamma _{n}^{t})$$. Thus, assuming full-buffer at the baseband unit, the choice of MCS determines a certain payload size $$b_{m_{r,n}^{t}}$$ that can be sent over the channel, and depending on the resulting block error rate, the goodput for the corresponding link at time t can be calculated as\n\n$$\\begin{array}{*{20}l} G_{r,n}^{t} = \\frac{(1 - e_{m_{r,n}^{t}} (\\gamma_{n}^{t})) \\cdot b_{m_{r,n}^{t}}}{T_{\\mathrm{f}}}. \\end{array}$$\n(4)\n\nFor the determination of user assignments and resource allocations, the baseband unit utilizes either the position estimates of the terminals present in the system, or their CSI. Acquisition of either of these comes at a certain signalling expense, which we model as a system overhead. We assume a time frame structure, as shown in Fig. 2, where the frame duration Tf is 1 ms, and it comprises of L = 5 sub-frames, each of duration Tsub. The first few symbols of each sub-frame are used for acquiring terminals’ position estimates or their CSI estimates. Since TDD-based system operation is assumed, channel reciprocity holds and, therefore, the UL pilots can be used for terminals’ positions or CSI estimates in the DL subframe.\n\nThe first symbol of each sub-frame is used for position acquisition, i.e., narrow-band pilots are sufficient for acquiring the terminals’ position estimates. The next four consecutive symbols in each sub-frame are the full-band pilots to be used for CSI acquisition. The number of pilots needed for position or CSI estimation depend on the number of terminals present in the system; the greater the number of terminals, the greater the number of full-band pilots needed for CSI estimation. Typically, the number of narrow-band pilots spans a few time symbols within a frame Tf. To avoid inter-carrier interference, the adjacent CSI-sensing pilots are scheduled based on the cyclic-prefix compensation distance, as explained in . Also, if any of the pilots in the sub-frames within a frame are not used for position or CSI sensing, they can be used for data transmission in downlink.\n\nBased on these parameters, the percentage overhead for position acquisition per frame can be calculated as\n\n$$\\begin{array}{*{20}l} OH_{\\text{pos}} = \\frac{S_{\\text{pos}} \\cdot f_{\\mathrm{sc,pos}} }{S_{\\text{total}} \\cdot f_{\\mathrm{sc,total}}}, \\end{array}$$\n(5)\n\nwhere Spos is the number of OFDM symbols used for position estimation of terminals in the system, fsc,pos denotes the number of sub-carriers used in the positioning beacon, and Stotal and fsc,total are the total number of OFDM symbols and sub-carriers available in the time frame Tf, respectively.\n\nSimilarly, for CSI acquisition per frame, the percentage overhead can be computed as\n\n$$\\begin{array}{*{20}l} OH_{\\text{CSI}} = \\frac{S_{\\text{CSI}} \\cdot f_{\\mathrm{sc,CSI}} }{S_{\\text{total}} \\cdot f_{\\mathrm{sc,total}}}, \\end{array}$$\n(6)\n\nwhere SCSI and fsc,CSI denote the number of OFDM symbols and the number of sub-carriers used for CSI acquisition of terminals present in the system in a transmitted frame, respectively.\n\n### Problem statement\n\nThe objective of this research work is to design an efficient resource allocation scheme that maximizes the sum-goodput of the CRAN based 5G system having medium- to high-speed mobility terminals. The traditional approach utilizes the terminals’ CSI for doing RA in a centralized or distributed fashion for multi-antenna systems [7, 8, 17]. Certainly, the same approach can be applied for a 5G system and combined with the advantage of coordination between RRHs provided by the CRAN architecture; however, the resulting system overhead can lead to deteriorating performance for an increased number of terminals in the system. In addition, the CSI-based RA approach leads to increased computational complexity when the number of terminals requiring service becomes large.\n\nTo alleviate these scalability problems in 5G CRAN system, we propose the usage of acquired terminals’ position estimates as an input to the RA scheme. Specifically, we design a RA scheme using machine learning algorithm to correlate the acquired terminals’ position information with different system parameters and to compare the resulting sum-goodput with that obtained from the traditional CSI-based RA scheme. Our proposed scheme is a centralized solution for resource allocation and is considerably less complex, but leads to other potential issues relevant to the context of using machine learning algorithms, namely, (a) the number of training samples for learning model needed to achieve a comparable system performance, and (b) the robustness of the learned structure to changes in the live environment, which we address in this research study. In the following, we will first discuss a learning-based approach which utilizes the random forests algorithm, and afterwards present a thorough performance evaluation.\n\n## Learning-based resource allocation scheme\n\nMachine learning is a tool used for making a computer program or a machine “develop new knowledge or skill from the existing and non-existing data samples to optimize some performance criteria” . In this work, we use the random forests algorithm , a supervised machine learning technique, for designing the learning-based RA scheme. For a basic understanding of the learning approach and its application to CRAN resource allocation, a brief introduction of the random forests algorithm, followed by the details of the proposed resource allocation scheme, are presented in the remainder of this section.\n\n### Random forests algorithm\n\nAs the name suggests, the algorithm uses a combination of multiple ‘random’ binary decision trees, which make up the forest, for predicting one (or a set of) outcome(s). Being a supervised learning technique, random forests algorithm relies on provision of a training dataset to generate the decision trees. The training dataset D consists of two parts: a set of data characteristics or features F, and a set of output variables Y. Each instance d i of the training dataset is called an input feature vector. The algorithm then constructs Ω t binary random trees, each with a depth Ω d , using the different features (selected randomly) in the training dataset. Each tree typically consists of a root node, one or more interior nodes and terminates at leaf nodes, as shown in the sample tree in Fig. 3. The leaf nodes store the output variable(s), technically called a ‘vote’, and the output variable predicted by the algorithm is the mode of those votes from all trees in the random forest. It is worthy to mention here that the algorithm strives to learn the input-output correlation so as to maximize the overall accuracy of prediction, irrespective of the distribution of individual values of the output variable y. Therefore, care has to be taken that the set of output variables Y is not ‘biased’ toward some particular values in the training data. Once a forest has been trained (during the operational phase), the input features of a new (and potentially unknown) instance is presented to the decision forest, leading to a prediction (through the voting of the trees) of the output variable. More detailed descriptions about the working of the random forests algorithm can be found in .\n\nIn general, random forests are known to be easy-to-use but robust machine learning data structures for noisy data. Furthermore, they can be used to calculate the ‘input variable importance,’ which signifies the influence of an input feature on prediction of the output variable. In this study, we consider system-level simulations modeled according to realistic scenarios, so the collected data may sometimes be noisy which will influence the overall performance of the learning algorithm. Keeping this in view, the aforementioned properties motivated our choice for using random forests algorithm in the design of the proposed RA scheme.\n\n### The proposed scheme\n\nAs already mentioned, the main motivation for designing the proposed approach is to use the acquired terminals’ position estimates for allocating the resources efficiently. The resources include transmit beam, $$\\pmb {v}_{r,n}^{t}$$, per RRH-terminal link, receive filter, $$\\pmb {u}_{r,n}^{t}$$, per terminal, as well as the appropriate MCSs’ selection, $$m_{r,n}^{t}$$, for each RRH-terminal user assignment. We consider the case of fixed user assignments, where each RRH serves only one terminal throughout the operational phase. We apply a simplistic approach for designing the dataset to use for the training of random forests algorithm: we use the acquired terminals’ position estimates in combination with some system resources as input features, and train the algorithm for predicting the MCS as an output variable. Specifically, the input parameters, which constitute the input feature vector, are the following:\n\n• Terminal position estimate $$\\mathcal {P}_{n}^{t}$$ of the dedicated terminal. In reality, this is acquired with certain precision using an extended Kalman filter, along with the direction of arrival and time of arrival estimates of those terminals .\n\n• Transmit beam $$\\pmb {v}_{r,n}^{t}$$ used for serving the dedicated terminal. Essentially, they belong to a set of fixed beams $$\\mathbb {V}$$ based on geometric beamforming, with a certain angular separation.\n\n• Receive filter $$\\pmb {u}_{r,n}^{t}$$ used by the terminal to receive transmitted data in a specific direction. These filters are also geometric beams, with an angular separation dependent on the number of antennas at the terminal.\n\n• Interfering transmit beams $$\\pmb {v}_{q,n}^{t}, q\\neq r$$ used by the interfering RRHs for nth terminal.\n\nRandom forests algorithm is trained on these ‘input features’ to predict the MCS, $$m_{r,n}^{t}$$, such that the sum-goodput is maximized. Essentially, we deploy the random forests as multi-class classifier, where the output variable $$m_{r,n}^{t}$$ has multiple values, or classes.\n\nFigure 3 illustrates an example of a binary decision tree of depth Ω d = 3 from a set of trees comprising a random forest. The root node comprises the input variable corresponding to the user position along the x-axis, while the input features corresponding to transmit beam, receive filter, interference beam for the first interfering terminal, and user position along the y-axis constitute the interior nodes of the tree. A binary decision tree organizes the classification in a set of binary choices about each input in steps, starting at the root node of the tree and progressing down to the leaf nodes which represent the classification decision. At each step of the tree construction, the input feature and its threshold value providing the highest information gain are selected. An input feature and its corresponding threshold value show the highest information gain if they divide the sample training dataset in two (equally large) subsets. Table 1 shows the details of the input variables used for constructing the input feature vector for training the random forests algorithm. Here, ‘Tx_IF1’ refers to the interfering transmit beam for the first interfering terminal, ‘Tx_IF2’ is the interfering transmit beam for the second interferer, and so on. The leaf nodes, which corresponds to the output variable values, comprises the classification decision, i.e., the MCS indices of which only a limited number is shown in Fig. 3 for illustration simplicity (c.f. Table 2).\n\nIt has to be noted that the organization of each trained decision tree of the random forest is determined by the bootstrap sample subset that is extracted from the training dataset during the training phase. For constructing the training dataset, we use ‘exhaustive search’ to determine the optimal allocation of resources, i.e., $$\\pmb {v}_{r,n}^{t}$$, $$\\pmb {u}_{r,n}^{t}$$, and $$m_{r,n}^{t}$$ for a terminal location $$\\mathcal {P}_{n}^{t}$$, to be served by a pre-allocated RRH. In a realistic system, a heuristic approach can be used to determine the optimal resource allocation for the acquired terminal position estimates and construct the training dataset. Upon completion of the training phase, random forests is used as a ‘scheduler’ for predicting the resource variable, MCS $$m_{r,n}^{t}$$, for a newly acquired terminal position estimate and testing its performance. This is done by constructing a test dataset, where the newly acquired position information is compared to the known position estimates used in training dataset. The input features for the closest matching terminal position are then combined with the new position estimate to construct the test data sample, for which a prediction of MCS is obtained from the trained random forests’ data structure. Using the predicted MCS, the sum-goodput is computed by combining all RRH-terminal links’ goodput, calculated using Eq. 4, for evaluating the overall system performance.\n\nDue to the inherent property of the random forests algorithm, this learning-based RA scheme can be expected to be robust to noisy data. Since in reality the acquired terminal position estimates can be inaccurate for some instances, the robustness property of the random forests suggests that this will not have much impact on the overall system performance. Nevertheless, in general, this robustness only holds up to a certain limit. In the performance evaluation section that follows, we determine these limits and discuss remedies.\n\n## Performance evaluation\n\nIn this research study, the performance of the random forests algorithm has been evaluated by means of simulation experiments. In this section, the simulation assumptions and scenarios of our evaluation methodology are first presented. This is followed by a performance analysis of the random forests algorithm providing a basis for the analysis of the performance for system level simulations. Next, a thorough analysis of various sets of performance results of the learning-based RA scheme is given in comparison to a set of benchmark schemes. Finally, various aspects on the robustness and performance limitation of the proposed learning-based RA scheme are discussed in further detail.\n\n### Evaluation methodology\n\nThe performance evaluation of the proposed learning-based RA scheme is done by performing simulations using the discrete event simulator Horizon . Figure 4 shows the simulation scenario, comprising 4 RRHs, each serving a single mobile terminal (MT). This represents a simpler multi-RRH, multi-terminal scenario for 5G CRAN system where only inter-RRH interference exists. The terminal position estimates can either be accurate or can be erroneous, where the error in position is modeled using normal distribution with zero mean and a given standard deviation. A fixed set of transmit beams is designed using geometric beamforming, with an angular separation of 3°. The receive filters are designed in the same way as the transmit beams, but the angular separation is set to 12°. Other parameter settings for the simulation set up are given in Table 3. Assuming DL communication, channel coefficients for each RRH-terminal link are based on TDD-based downlink and are extracted by using the map-based METIS channel model for Madrid grid . A ray-tracer-based channel model was implemented for this purpose, the details for which can be found in . Note that in Table 3, hTx refers to the height of the RRH antennas, while hRx refers to the terminal antenna height from the ground. Finally, v Rx denotes the terminals’ velocity.\n\nDepending on the investigation scenario (c.f., Section 3), the training dataset is constructed next by using the procedure outlined in Section 4. These training datasets are used to construct the multi-class Random forests model, where we rely on the implementation provided by OpenCV . A total of 100 terminal positions, per terminal, are selected randomly from a set of 1000 terminal positions generated by Horizon, per terminal, to create training datasets of 0.25 million samples for each investigation scenario. The output from the random forests model is used to compute the goodput at the terminal, referred to as user goodput, using Eq. (4). The system goodput is computed by taking the sum of the user goodput for each time instance, and its average over all considered 100 terminal positions is used for system-based performance evaluation.\n\n### Performance analysis of random forests algorithm\n\nBefore a forest-based data structure can be applied, it first needs to be learned off-line based on training data. For this, a considerable amount of instances needs to be collected, for instance, from an optimal CSI-based RA scheme. It is important to analyze the collected dataset itself, before constructing the random forest. Table 2 shows the distribution of the output variable, i.e., the considered 8 MCSs, in the training dataset. We notice that the output variables are concentrated more toward lower or higher MCS selection values; this is because the channel gain for a particular terminal is severely influenced by the interference present in the system. Based on this observation, we need to consider an appropriate structure for constructing the random forest, such that the prediction of the output variable is not ‘biased’ toward the output variable value present in the majority of the training data instances in the given dataset.\n\nIn addition to the details of the input variables used for constructing the input feature vector for training the random forests algorithm, Table 1 also shows the variable importance of each input feature obtained by applying the random forests’ property, to observe its dependence on the output variable in the training dataset. From the table, it can be observed that the index of the selected receive filter beam is the most important variable that influences the value of the output variable. This is because the output variable, the MCS selection, is tied to the SINR value of the given terminal n for a given time instance t, which is highly dependent on the receive filter selected to serve the user n. The terminal position is the next most important variable, which itself indicates the expected interference level seen by terminal n when served by a selected transmit beam and receive filter combination by an RRH. The interfering beam indices also considerably influence the output variable, since they are also important in deciding the level of interference seen by terminal n at time t. The assigned terminal ID is the least important parameter, since it only indicates the terminal considered for a given sample instance, and is loosely tied to the output variable, i.e., the MCS selected for serving the indicated terminal.\n\nAfter analyzing the data characteristics, the next step is to construct and train the random forests algorithm. The training of the algorithm essentially optimizes the forest data structure for accuracy. Here, an important aspect relates to the dimensioning of the forest itself, as it impacts the training and test accuracy. Dimensioning relates to the depth of the trees as well as the number of trees to be used in the forest. The number of random features selected for creating a node split in each tree is chosen to be $$\\sqrt {I}$$ according to the analysis study of the random forests algorithm presented in , where I is the number of input features.\n\nThe training accuracy is obtained by using a subset of training data for validation of the constructed random forests model. Once a sufficiently dimensioned random forest structure has been found, a test dataset is then used to compute the test accuracy of the model by passing each instance of the test dataset through each of the random trees in the model. The minimum number of training samples needed to learn a given function (e.g., the resource allocation function in this case) is known as the sample complexity in statistical learning theory. As the problem is open for many functions, determining the number of training samples is usually done empirically. In this work, the number of test samples is the same as that of the training samples, i.e., 0.25 million, with 100 terminal positions drawn randomly from among 1000 terminal positions’ data. In terms of performance evaluation, the accuracy of the data structure built by the random forests algorithm is an important metric; the higher the number of correctly predicted output variables by the model (whether for the validation dataset or the test dataset), the higher the accuracy. However, having a very high training accuracy is not an indicator of an appropriate learned structure. It could be the case that the random forests structure works perfectly for the training dataset, but shows a low accuracy for test dataset. Such a structure is then an over-fit to the training data. For building a robust random forests structure, we need to vary the number of trees Ω t in the forest, as well as the depth of the trees Ω d , in such a way that the model achieves a fairly high training accuracy while it shows good test accuracy for any test dataset with similar input feature vector composition. Hence, for some data collected from a first system set-up (see the next sub-section for details), we study in Table 4 the training and test accuracy obtained for different parametrization of the random forests structure. Based on these investigations, we used the best possible random forests model for the design of the learning-based RA scheme, with 100 trees, each with a maximum depth of 10.\n\nOnce the learned random forests structure achieves an optimal training accuracy, based on different parametrization of the algorithm, it is available for predicting the output variable for the test dataset generated at run-time of the considered CRAN system.\n\n### Evaluation results for the proposed learning-based RA scheme\n\nWe initially start with benchmarking the raw goodput for different schemes based on perfect system status knowledge, i.e., position or CSI. In detail, we consider the following schemes:\n\n• The proposed learning-based RA scheme; where the multi-class random forests algorithm is used for allocating appropriate resources.\n\n• A random MCS allocation scheme; which uses the same input features as used for the learning-based scheme, but assigns a randomly selected MCS to serve a given terminal. This scheme serves as a benchmark to directly determine the value of learning the MCS for a given input feature vector.\n\n• A geometric-based RA scheme; where the terminal position information is used for allocating the transmit beams and receive filters for serving a given terminal, while again selecting the MCS randomly. This scheme benchmarks, in addition, the value of the pre-processing.\n\n• A legacy CSI-based scheme; where for simplicity, we consider a scheme that determines the optimal transmit beam and receive filters based on the given CSI. This serves as an upper bound on the system performance.\n\nTable 5 presents the average system goodput for all the abovementioned comparison schemes. Note that in this investigation, we do not consider the impact from the overhead model. We initially recognize that the learning-based RA scheme achieves a performance quite close to the CSI-based scheme. In contrast, the scheme based on random MCS assignment performs a lot worse than the learning-based RA scheme, because of the spatial selectivity of the system. This also signifies the importance of learning the correlation between different system parameters. The geometric-based RA scheme shows the lowest system goodput compared to the goodput obtained from the CSI-based scheme; the reason being a severely interference-limited system considered for the given case. In general, the transmit beam and receive filter selected purely on the basis of user terminal position are strictly non-optimal in an interference-limited system. Also, since the selection of MCS for serving a given terminal with known position is done at random, therefore, the system goodput degrades even further. From this point onwards, we will provide a comparison of results for the proposed learning-based scheme with the CSI-based RA scheme only, since the random MCS allocation scheme as well as the geometric-based RA scheme reap off very low system goodput.\n\nWe next turn to the evaluation of the different approaches taking the system overhead into account. Since the transmitted frame duration is set to 1 ms, we assume L=5 TDD-frames to be used for position, or CSI, acquisition and data transmission for all terminals present in the system. This serves as basic parametrization for the overhead calculations presented in Eqs. 5 and 6. Our goal is to study the impact of overhead on performance of the learning-based and CSI-based RA schemes as the number of terminals in the system (for which the state information needs to be collected) grows. Note that we consider at this step still all state information to be perfectly accurate (i.e., the position information as well as the CSI).\n\nFigure 5 shows the results of the average system goodput obtained using accurate terminal position information at all RRHs for the learning-based and CSI-based RA schemes. The colored bars show the effective average system goodput, i.e. the system goodput obtained after taking into account the effect of system overhead due to position beaconing or CSI sensing, while the underlying gray bars represent the system performance without taking the overhead into account. Overall, the proposed learning-based RA scheme achieves about 96% of the system goodput achieved by the CSI-based scheme, without considering any overhead. However, if the system overhead is accounted for, we observe that the proposed scheme is either at par or better in performance compared to the CSI-based scheme for all possible number of terminals present in the system. In particular, as we increase the number of terminals in the system, the number of narrow-band beacons for acquiring terminals’ position estimates increases gradually per TTI, and thus the overhead scales up only marginally for the learning-based RA scheme. In contrast, the overhead for the CSI-based scheme grows much stronger with the increase in the number of terminals present in the system, reaching up to 48% of the frame time, showing that effective system performance degrades severely if CSI-based scheme is used for resource allocation in a system with high terminal density.\n\nThese two initial results are quite striking: firstly, with respect to pure spectral efficiency, a learning-based RA scheme using position information can achieve quite a good performance already in comparison to a CSI-based scheme. This holds at least for the considered system scenario, which nevertheless has been designed carefully and contains a typical level of detail for a system-level simulation of a 5G network. Second, if the overhead or the state acquisition is factored in, due to the high cost of the CSI acquisition, the learning-based RA scheme can significantly outperform CSI-based approaches (up to 100% performance improvement).\n\n### Robustness of learning-based RA scheme\n\nThis performance advantage motivates a more thorough study on the robustness of our learning-based RA scheme. We start with considering the most obvious potential source of inaccuracy influencing the learning-based scheme, namely, the accuracy of the position information.\n\nFigure 6 shows the results for the average system goodput obtained when a random error is involved in the position estimation for the terminals being served by RRHs. It can be seen that the classifier trained on perfect terminal position information is enough to guarantee good system performance up to a certain degree of error involved in the position estimation. However, if the error margin in the terminal position estimates exceeds 2 m, the learning-based RA scheme trained on perfect terminal position estimates fails to provide satisfactory system performance. Better system goodput can be obtained by using the learning-based RA scheme trained on inaccurate position estimates, but the traditional CSI-based RA scheme provides still about 10% better effective system performance.\n\nThis shows the robustness of the proposed scheme for small degrees of error involved in acquired terminal position information. However, when the error margin becomes excessively large, the CSI-based RA scheme provides better effective system performance, when the best-case terminal density scenario is considered, i.e., the scenario where the number of terminals present in the system is equal to the number of RRHs serving them.\n\nWe next turn to the question how sensitive the learning-based RA scheme is to a change in the propagation scenario in contrast to the one from which the training data has been acquired. Figure 7 shows the results for changing obstacle/scatterer density when the random forests model is trained only for a fixed system parameterization. We observe that the average system goodput varies only marginally with varying scatterers’ density ranging between 0.01 and 0.2/m2. Overall, the proposed scheme experiences only 7% loss compared to the traditional CSI-based RA scheme in terms of effective system goodput obtained for all considered scenarios.\n\n### Performance accuracy\n\nAn important factor for the design of such a scheme is the quantitative analysis of the dataset, i.e., how many samples are needed to achieve a comparable system performance between the learning-based RA scheme and the traditional CSI-based RA scheme. For this purpose, the system-based performance with an increasing number of total samples has been computed and presented in Fig. 8. More specifically, Fig. 8 represents the system goodput in comparison to the CSI-based scheme for different number of samples used for training and testing the random forests model, without considering any overhead. These results are for the case when perfect position estimates of the users are available at each RRH, and the random forests model is trained (and tested) with the given number of samples. For each case, the learning model has 100 trees, each with a maximum depth of 10.\n\nAs shown in Fig. 8, the performance of the learning-based RA scheme improves with greater number of samples used for training and testing; with more samples comes more information about correlation between the input data features and the output variable, and thus the learning of RF model improves with increasing number of training instances with improved test accuracy. However, the performance saturates after a certain point; this happens for a total of 250,000 instances used for training and testing, in the case shown in Fig. 8. Therefore, we used a total of 250,000 instances for all the abovementioned performance results’ evaluation, which is good enough to guarantee a comparable performance of the learning-based RA scheme to the CSI-based RA scheme.\n\n### Sensitivity to random antenna orientation\n\nIn the learning-based RA scheme, one of the allocated resources includes the receive filter, which is based on beamforming in the direction closest to the direction of the received signal. For this to work perfectly, it is necessary to have the knowledge of the terminal’s antenna orientation at the RRH serving the related terminal. The antenna orientation of the terminal defines the radiation pattern of the receiving antenna, which dictates the selection of the receive filter. However, the terminal antenna orientation is typically random and can therefore be defined in the local coordinate system (LCS), whereas the terminal antenna orientation known at RRH is defined in the global coordinate system (GCS). In order to compute the correct direction of receive filter, the following transformation between GCS and LCS has to be used (based on the discussion given in the METIS channel model documentation ):\n\n$$F_{\\text{GCS}} (\\theta, \\phi) = \\left[ \\begin{array}{ll} cos \\varphi & -sin \\varphi \\\\ sin \\varphi & cos \\varphi\\\\ \\end{array} \\right] \\left[ \\begin{array}{l} F_{\\theta, {\\text{LCS}}} (\\theta ', \\phi ') \\\\ F_{\\phi, {\\text{LCS}}} (\\theta ', \\phi ') \\\\ \\end{array} \\right].$$\n(7)\n\nHere, FGCS represents the antenna radiation pattern in GCS, θ and ϕ are the elevation and azimuth angles in LCS, and Fθ,LCS and Fϕ,LCS denote the radiation patterns of terminal antenna in elevation and azimuth planes, respectively. cosφ and sinφ are the system transformation variables, given by :\n\n$$\\begin{array}{*{20}l} cos \\varphi = \\pmb{e}_{\\theta, {\\text{GCS}}} (\\theta, \\phi)^{T} \\pmb{R}\\: \\pmb{e}_{\\theta, {\\text{LCS}}} (\\theta ', \\phi '), \\end{array}$$\n(8)\n$$\\begin{array}{*{20}l} sin \\varphi = \\pmb{e}_{\\phi, {\\text{GCS}}} (\\theta, \\phi)^{T} \\pmb{R}\\: \\pmb{e}_{\\theta, {\\text{LCS}}} (\\theta ', \\phi '), \\end{array}$$\n(9)\n\nwhere, eθ,GCS and eϕ,GCS are the basis vectors in GCS for elevation and azimuth planes, respectively. R is the rotation matrix applied for correcting the angular orientation in GCS based on the orientation in LCS, and eθ,LCS and eϕ,LCS are the basis vectors in LCS for elevation and azimuth planes, respectively. The derivation of the rotation matrix is given in the Appendix.\n\nIf not known a priori at the serving RRH, the antenna orientation of the user terminal is expected to affect the average system goodput. We therefore study next the impact of such a random orientation of the terminal antenna on the performance of the learning-based RA scheme. Figure 9 shows the effect of misalignment in terminal antenna orientation information in the training and test datasets for the learning-based RA scheme. It can be seen that the average system goodput is adversely affected by the misalignment in antenna orientation at the receiver, with system goodput only being about 27% of that for the traditional CSI-based scheme for resource allocation. This is by far the biggest impact on the performance of the learning-based RA scheme found in our research work. Thus, it is important to investigate approaches to mitigate the performance degradation from random antenna orientation caused by users’ hand movements. One way to mitigate the effect of the misalignment in antenna orientation is to train the classification model for the learning-based approach using random terminal antenna orientation information, and then test it for dataset with random terminal antenna orientation information embedded within. This case is shown as ‘solution 1’ in Fig. 9. In this case, the random terminal antenna orientation helps the classifier learn the correlation between different resources and terminal-related system parameters effectively, thus resulting in the performance gap of only 6% from the system goodput for the CSI-based RA scheme.\n\nAnother option to mitigate the effect of terminal antenna orientation is to apply a rotation matrix to adjust the predicted receive filter settings according to realistic terminal antenna orientation. The mathematical analysis for applying this solution is based on the derivation above. The performance result for this method is shown in Fig. 9 by the bar labeled ‘solution 2.’ In this case, we achieve almost 85% of the average system goodput compared to the CSI-based scheme, which is fairly good but worse than the performance seen for ‘solution 1.’ A possible reason for this performance loss is the interference present in the system, which makes the solution of only rotating the predicted receive filter for good reception at terminal a sub-optimal approach.\n\nYet another solution can be applied to mitigate the effect of unknown terminal antenna orientation, i.e., by making the terminal antenna orientation a part of the input feature vector, exclusively. Note that this would require some additional signalling from the terminal to the baseband unit, for which we do not here account for the overhead. The performance of this approach is shown as ‘solution 3’ in Fig. 9, where we observe that the performance of the proposed technique reaps off almost the same average system goodput as in case of ‘solution 1.’ Since we use the same number of features for random selection in building the decision trees in random forests model, the randomization of trees in the model results in the variation of the obtained system goodput, for the case when terminal antenna orientation is embedded or is exclusively incorporated as an input feature for training the random forests model, i.e., for ‘solution 1’ and ‘solution 3,’ respectively. We conclude with the remarkable observation that the random antenna orientation can basically deteriorate performance strongly; however, especially by including this effect in the training data, more robust MCS selections can be trained to compensate for this randomness.\n\n### Change in channel statistics\n\nA special case for testing the performance of the proposed scheme is when the LOS links are no more existent between the RRHs and the relevant terminals in the system. In this case, the specular component is totally neglected when computing the channel matrix for a given RRH-terminal link, thus resulting in a non-LOS (NLOS) scenario. Figure 10 shows the average system goodput obtained from the proposed learning-based, as well as the traditional CSI-based RA schemes, for different inaccuracy ranges involved in the acquired terminal position estimates. We kept the range of terminal position inaccuracy fairly small in this case, since NLOS consideration is already enough to result in performance degradation using only terminal-position estimates for resource allocation in the system. Overall, for perfect terminal position information availability, the proposed scheme still performs fairly well, reaping off almost 90% of the system goodput obtained using CSI-based RA scheme. The effects on average system performance for different variation in terminal position inaccuracies do not show a specific trend, because of the changing channel statistics in NLOS scenario. However, training on inaccurate terminal position estimates proves to be beneficial in improving the system goodput, in contrast to the effect seen in LOS case, where the learning-based scheme trained only on perfect terminal position information is enough to guarantee a system performance comparable to the traditional CSI-based RA scheme, when lower accuracy is involved in the terminals’ position estimates.\n\n## Conclusions\n\nWe presented the design of a learning-based RA scheme which has much lower system overhead, as well as lower complexity, than the traditionally used CSI-based RA scheme, because of its dependence on only the acquired terminal position estimates. Random forests algorithm is used for designing learning-based RA scheme, that works as a scheduler for appropriate resource allocation in 5G CRAN system, serving the different terminals using only their position information. A comparison analysis was done for the RA scheme based on random forests model and the CSI-based RA scheme, in different contexts. The proposed scheme shows either comparable or significantly better effective system performance compared to the CSI-based RA scheme for different terminal densities in the system. In terms of the design parameter variations, the proposed scheme is fairly robust to the inaccuracy involved in the terminal position estimation. Training the random forests model on the dataset involving variation in either the system metrics or the design parameters for the learning-based scheme is very beneficial in case when the same model trained on fixed system parametrization shows degraded system performance. In general, for LOS or NLOS cases, the proposed scheme is robust to small error margin involved in the acquired terminal position information, as well as to the variation in system characterization (such as changing scatterers’ density). The change in terminal antenna orientation affects the performance of the proposed scheme most severely, but the effect can be mitigated by training on top of the terminal antenna orientation information, either embedded or provided explicitly in the training data for constructing the random forest. The performance limitations of the learning-based scheme for extreme channel characterization variation is still an open question, which will be a part of the future work. Also, the scope of the proposed scheme is limited to a centralized solution for resource allocation in CRAN-based 5G systems. Designing a similar learning-based RA scheme as a distributed solution for CRAN architecture, with the interference coordination between the baseband units, is a potential topic for future research.\n\n## Appendix\n\nThis appendix presents a derivation for the rotation matrix. The basic rotation matrices for rotating the vectors by an angle in x-, y-, or z-axes using the right-hand rule are given as follows :\n\n$$\\pmb{R}_{x} (\\theta) = \\left[ \\begin{array}{lll} 1 & 0 & 0 \\\\ 0 & cos \\theta & -sin \\theta\\\\ 0 & sin \\theta & cos \\theta \\end{array} \\right],$$\n(10)\n$$\\pmb{R}_{y} (\\theta) = \\left[ \\begin{array}{lll} cos \\theta & 0 & sin \\theta\\\\ 0 & 1 & 0\\\\ -sin \\theta & 0 & cos \\theta \\end{array} \\right],$$\n(11)\n$$\\pmb{R}_{z} (\\theta) = \\left[ \\begin{array}{lll} cos \\theta & -sin \\theta & 0\\\\ sin \\theta & cos \\theta & 0\\\\ 0 & 0 & 1 \\end{array} \\right],$$\n(12)\n\nFor the pre-defined orientation angles of the receive filter for a terminal, the rotation matrix can be computed as:\n\n$$\\begin{array}{*{20}l} \\pmb{R} = \\pmb{R}_{z}(\\phi_{0}) \\pmb{R}_{y}(\\theta_{0}). \\end{array}$$\n(13)\n\nExpanding the above expression, we get the following form:\n\n$$\\pmb{R} = \\left[ \\begin{array}{lll} cos \\phi_{0} & -sin \\phi_{0} & 0\\\\ sin \\phi_{0} & cos \\phi_{0} & 0\\\\ 0 & 0 & 1 \\end{array} \\right] \\left[ \\begin{array}{lll} cos \\theta_{0} & 0 & sin \\theta_{0}\\\\ 0 & 1 & 0\\\\ -sin \\theta_{0} & 0 & cos \\theta_{0} \\end{array} \\right]$$\n(14)\n$$\\pmb{R} = \\left[ \\begin{array}{lll} cos \\phi_{0}\\:cos \\theta_{0} & -sin \\phi_{0} & cos \\phi_{0} \\:sin \\theta_{0}\\\\ sin \\phi_{0} \\:cos \\theta_{0} & cos \\phi_{0} & sin \\phi_{0} \\:sin \\theta_{0}\\\\ -sin \\theta_{0} & 0 & cos \\theta_{0} \\end{array} \\right]$$\n(15)\n\nInserting this rotation matrix expression in Eq. 8 results in the following expressions for cosφ and sinφ:\n\n$${}cos \\varphi\\! =\\! \\left[ \\begin{array}{lll} \\!cos \\theta\\:cos \\phi & \\!cos \\theta\\: sin \\phi & -sin\\theta \\end{array} \\right] \\pmb{R} \\left[\\! \\begin{array}{lll} cos \\theta'\\:cos \\phi'\\\\ cos \\theta'\\:sin \\phi'\\\\ -sin \\theta' \\end{array} \\!\\right],$$\n(16)\n$$sin \\varphi = \\left[ \\begin{array}{lll} -sin \\phi & cos \\phi & 0 \\end{array} \\right] \\pmb{R} \\left[ \\begin{array}{lll} cos \\theta'\\:cos \\phi'\\\\ cos \\theta'\\:sin \\phi'\\\\ -sin \\theta' \\end{array} \\right].$$\n(17)\n\nSimplifying these matrix multiplications gives\n\n$$\\begin{array}{*{20}l} cos \\varphi = & \\: (cos\\theta \\: cos \\theta_{0} \\: cos\\phi'\\: +\\:sin \\theta \\:sin \\theta_{0}) cos \\theta'\\:cos \\phi'\\: \\\\ & + cos\\theta\\:sin \\phi'\\:cos\\theta'\\:sin\\phi' \\\\ & - sin\\theta' (cos\\theta\\:sin\\theta_{0}\\:cos\\phi'\\: - sin\\theta\\:cos\\theta_{0}), \\end{array}$$\n(18)\n\nand\n\n$$\\begin{array}{*{20}l} sin \\varphi = & -cos\\theta_{0}\\, \\: sin \\phi'\\: cos\\theta'\\:cos \\phi' +\\:cos \\phi' \\:cos \\theta'\\:sin\\phi' \\\\ & -\\:sin\\theta_{0}\\, \\:sin\\phi'\\:sin\\theta' . \\end{array}$$\n(19)\n\n## Abbreviations\n\n5G:\n\n5th generation\n\nBBU:\n\nBaseband unit\n\nCRAN:\n\nCSI:\n\nChannel state information\n\nD2D:\n\nDevice-to-device\n\nDL:\n\nGCS:\n\nGlobal coordinate system\n\nIoT:\n\nInternet of things\n\nKPI:\n\nKey performance indicator\n\nLCS:\n\nLocal coordinate system\n\nLOS:\n\nLine-of-sight\n\nLTE:\n\nLong-term evolution\n\nLTE-A:\n\nMIMO:\n\nMultiple-input multiple-output\n\nMCS:\n\nModulation and coding scheme\n\nMT:\n\nMobile terminal\n\nNLOS:\n\nNon-line-of-sight\n\nOFDM:\n\nOrthogonal frequency-division multiplexing\n\nRA:\n\nResource allocation\n\nRAN:\n\nRRH:\n\nSINR:\n\nSignal-to-interference-and-noise ratio\n\nTDD:\n\nTime division duplex\n\nTTI:\n\nTime transmission interval\n\nUDN:\n\nUltra-dense network\n\nUL:\n\n## References\n\n1. 1\n\nQC Li, H Niu, AT Papathanassiou, G Wu, 5G Network capacity: key elements and technologies. IEEE Veh. Technol. Mag.9(1), 71–78 (2014). https://doi.org/10.1109/MVT.2013.2295070.\n\n2. 2\n\nP Kela, J Turkka, M Costa, Borderless mobility in 5G outdoor ultra-dense networks. IEEE Access. 3:, 1462–1476 (2015). https://doi.org/10.1109/ACCESS.2015.2470532.\n\n3. 3\n\nS Imtiaz, H Ghauch, MMU Rahman, G Koudouridis, J Gross, in Learning-Based Resource Allocation Scheme for TDD-Based 5G CRAN System. Proceedings of the 19th ACM International Conference on Modeling, Analysis and Simulation of Wireless and Mobile Systems. MSWiM ’16 (ACMNew York, 2016), pp. 176–185. https://doi.org/10.1145/2988287.2989158.\n\n4. 4\n\nJG Andrews, S Buzzi, W Choi, SV Hanly, A Lozano, ACK Soong, JG Zhang, What will 5G be?. IEEE J. Sel. Areas Commun.32(6), 1065–1082 (2014).\n\n5. 5\n\nM Hadzialic, B Dosenovic, M Dzaferagic, J Musovic, in Cloud-RAN: Innovative Radio Access Network Architecture. Proceedings ELMAR-2013 (IEEE, 2013), pp. 115–120.\n\n6. 6\n\n7. 7\n\nTE Bogale, L Vandendorpe, Weighted sum rate optimization for downlink multiuser mimo coordinated base station systems: Centralized and distributed algorithms. IEEE Trans. Sign. Process.60(4), 1876–1889 (2012). https://doi.org/10.1109/TSP.2011.2179538.\n\n8. 8\n\nA Chiumento, C Desset, S Pollin, LV der Perre, R Lauwereins, Impact of CSI Feedback Strategies on LTE Downlink and Reinforcement Learning Solutions for Optimal Allocation. IEEE Trans. Veh. Technol.66(1), 550–562 (2017). https://doi.org/10.1109/TVT.2016.2531291.\n\n9. 9\n\nJC Shen, J Zhang, KC Chen, KB Letaief, High-dimensional CSI acquisition in massive MIMO: sparsity-inspired approaches. IEEE Systems Journal. 11(1), 32–40 (2017). http://dx.doi.org/10.1109/JSYST.2015.2448661.\n\n10. 10\n\nM Botsov, S Stańczak, P Fertl, in Comparison of Location-based and CSI-based Resource Allocation in D2D-Enabled Cellular Networks. 2015 IEEE International Conference on Communications (ICC), (2015), pp. 2529–2534. https://doi.org/10.1109/ICC.2015.7248705.\n\n11. 11\n\nL Breiman, Random forests. Mach. Learn.45(1), 5–32 (2001).\n\n12. 12\n\nHZ O. Punal, J Gross, in RFRA: Random Forests Rate Adaptation for Vehicular Networks. Proc. of the 13th IEEE International Symposium on a World of Wireless, Mobile and Multimedia Networks 2013 (WoWMoM 2013) (IEEE, 2013).\n\n13. 13\n\nM Vincenzi, A Antonopoulos, E Kartsakli, J Vardakas, L Alonso, C Verikoukis, Multi-tenant slicing for spectrum management on the road to 5g. IEEE Wirel. Commun.24(5), 118–125 (2017). https://doi.org/10.1109/MWC.2017.1700138 8088538.\n\n14. 14\n\nE Datsika, A Antonopoulos, N Zorba, C Verikoukis, Software defined network service chaining for ott service providers in 5g networks. IEEE Wirel. Commun.55(11), 124–131 (2017). https://doi.org/10.1109/MCOM.2017.1700108. 8114562.\n\n15. 15\n\nMY Lyazidi, N Aitsaadi, R Langar, in Resource Allocation and Admission Control in OFDMA-Based Cloud-RAN. 2016 IEEE Global Communications Conference (GLOBECOM), (2016), pp. 1–6. https://doi.org/10.1109/GLOCOM.2016.7842217.\n\n16. 16\n\nJP Leite, PHP de Carvalho, RD Vieira, in A flexible framework based on reinforcement learning for adaptive modulation and coding in OFDM Wireless Systems. 2012 IEEE Wireless Communications and Networking Conference (WCNC), (2012), pp. 809–814. https://doi.org/10.1109/WCNC.2012.6214482.\n\n17. 17\n\nX Wang, P Zhu, FC Zheng, C Meng, X You, in Energy-efficient resource allocation in multi-cell OFDMA systems with imperfect CSI. 2015 IEEE 82nd Vehicular Technology Conference (VTC2015-Fall), (2015), pp. 1–5. https://doi.org/10.1109/VTCFall.2015.7390923.\n\n18. 18\n\nE Alpaydin, Introduction to machine learning (MIT press, Cambridge, 2014).\n\n19. 19\n\nJ Werner, M Costa, A Hakkarainen, K Leppänen, M Valkama, in Joint User Node Positioning and Clock Offset Estimation in 5G Ultra-Dense Networks. 2015 IEEE Global Communications Conference (GLOBECOM), (2015), pp. 1–7. https://doi.org/10.1109/GLOCOM.2015.7417360.\n\n20. 20\n\nG Kunz, O Landsiedel, S Götz, K Wehrle, J Gross, F Naghibi, in Expanding the Event Horizon in Parallelized Network Simulations. Modeling, Analysis & Simulation of Computer and Telecommunication Systems (MASCOTS), 2010 IEEE International Symposium On (IEEE, 2010), pp. 172–181.\n\n21. 21\n\nV Nurmela, A Karttunen, A Roivainen, L Raschkowski, T Imai, J Järveläinen, J Medbo, J Vihriälä, J Meinilä, J Kyröläinen, K Haneda, V Hovinen, J Ylitalo, N Omaki, V-M Kolmonen, T Jämsä, P Kyösti, K Kusume, METIS D1.2: Initial channel models based on measurements, (2014).\n\n22. 22\n\nP Kela, et al, in Location Based Beamforming in 5G Ultra-Dense Networks. Proc. Vehicular Technology Conference (VTC Fall), 2016 IEEE 84th (IEEE, 2016). accepted for publication.\n\n23. 23\n\nK Pulli, A Baksheev, K Kornyakov, V Eruhimov, Real-time Computer Vision with OpenCV. Commun. ACM. 55(6), 61–69 (2012). http://doi.acm.org/10.1145/2184319.2184337.\n\n24. 24\n\nEW Swokowski, Calculus With Analytic Geometry (Prindle, Weber, and Schmidt, Boston, 1979).\n\n## Acknowledgements\n\nThe authors would like to thank Mr. Christer Qvarfordt and Dr. Kari Leppänen both with Huawei Technologies for valuable discussions.\n\n## Author information\n\nAuthors\n\n### Corresponding author\n\nCorrespondence to Georgios P. Koudouridis.\n\n## Ethics declarations\n\n### Competing interests\n\nThe authors declare that they have no competing interests.\n\n### Publisher’s Note\n\nSpringer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.\n\n## Rights and permissions",
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https://physics.stackexchange.com/questions/242437/throwing-a-football-is-it-truly-parabolic | [
"Throwing a Football. Is it truly parabolic?\n\nDriving into work, I started thinking about the arc of something being thrown and was puzzled about how gravity's affect is squared per second for falling bodies. Intuitively that implies the shape would be \"like\" a parabolic shape. But I'm curious if it truly is parabolic. Doing some googling, I've found some rudimentary explanations that remind me of explanations I received in algebra as a kid (such as http://entertainment.howstuffworks.com/physics-of-football1.htm)\n\nMy confusion is around the idea that gravity's effect on falling bodies (reference http://en.wikipedia.org/wiki/Equations_for_a_falling_body) is increased over time. If this is the case, then wouldn't this affect the arc in such a way that it's longer on the release end and curves downward faster at the end? This might not be as noticeable for short distances, but intuitively it could play an important role in longer distances.\n\nIn other words, my question is pretty simple, as soon as something is thrown (shot, projected, etc) is it considered a falling body. Either way, is the arc or path truly parabolic, or is the path elongated on the throwing end and curve downward faster at the end? If it is truly parabolic, can you please give a clean explanation as to why the effect of gravity over time doesn't apply? If my intuition is correct about it being elongated, can you please share a useful reference as well?\n\nA couple of assumptions:\n\n1. What is being thrown is small and close to a large body. Like throwing a football 1,000 miles across to the earth's surface.\n2. Ignore air resistance or other factors for simplicity sake.",
null,
"Update:\n\nThe Newton cannon illustration in @HariPrasad's answer shows us the flight path is elliptical not parabolic. It shows how modifying the initial vector's magnitude, when the angle is tangent to the earth effects the ellipse. It however does not show how changes to the initial vector's angle affects the ellipse.\n\nCan we formulate an equation for the path (Reference: https://en.wikipedia.org/wiki/Ellipse)? I'm hoping for an answer that explains how the foci positions, and sum of red and blue line (need editor to give technical name) change in relation to changes in the direction and magnitude of the initial vector.",
null,
"• Given your assumptions, yes, it is parabolic. Gravity's effect isn't increased over time, it is a constant force $\\vec{f} = m \\vec{g}$. – Dimitri Mar 9 '16 at 13:59\n• Doing some more googling, it does look like things drop faster at the end for bullets/artillery (en.wikipedia.org/wiki/External_ballistics) however, what you are saying is this is due to air/wind resistance or other factors? – VenomFangs Mar 9 '16 at 14:03\n• Okay, I see what you mean. The trajectory of any object (pointlike or of finite size) will always be parabolic in a constant force field if there is no friction. In the case of a football some shape effects coupled to air resistance might indeed modify the trajectory. – Dimitri Mar 9 '16 at 14:10\n• For something like a football, you can not neglect air resistance and that's why, indeed, the path is elongated on the throwing end and curved downward faster at the end. You also need to consider the Magnus effect, which allows football players to “bend” a shot in different ways. – leftaroundabout Mar 9 '16 at 15:00\n• The faster drop at the end of a bullet's trajectory is caused by the bullet beginning to tumble instead of pointing directly forward. This is indeed caused by air resistance and loss of spin imparted by the barrel of the gun. A bullet fired in a friction-less environment would not have these issues. – Darrel Hoffman Mar 9 '16 at 19:52\n\nMany sources may tell you, that the path of a trajectory is a parabola. Indeed, all of the mathematical formula and calculations dealing with trajectories of objects falling, thrown or propelled support that interpretation. But when dealing with earth satellites and ballistic missiles, the truth is that their orbits are portions of ellipses.\n\nThe Newton's canon on a Mountain\n\nNewton's cannonball was a thought experiment by Isaac Newton used to hypothesize that the force of gravity was universal, and it was the key force for planetary motion.",
null,
"Here is an interactive version of it: Newton's Cannon on a Mountain\n\nIf an object has less than escape velocity (For earth it is 11.2 km/s), its path is an ellipse. If the object has velocity equal to escape velocity, it has a parabolic trajectory. If it is greater than escape velocity, it is hyperbolic.\n\nNormally when we throw an object the actual path of the object is a part of a larger ellipse as the below image shows but since the velocity is not enough the object hits the ground before completing a full elliptical path which seems to be a parabola",
null,
"The parabolic paths become flatter and flatter as the cannon is fired faster. Newton imagined that the mountain was so high that air resistance could be ignored, and the canon was sufficiently powerful.\n\nPS: Newton's mountain was impossibly high but he realized that the moon's circular path around the earth could be caused by the same gravitational force that pulls cannonball in its orbit, in other words, the same force that causes objects to fall.\n\nThe answer to your question is that the path of football is truly \"elliptical\" since its velocity is way less than escape velocity. But to us, we \"approximate its path to a parabola\".\n\nWe can use equations of projectile motion as follows.",
null,
"Equation for the trajectory of a projectile motion:\n\n$\\displaystyle y= x\\tan\\theta -{\\frac{g}{2u^2\\cos^2\\theta}}x^2$\n\n(yes it is an equation of parabola but I have mentioned earlier that the mathematical formula and calculations dealing with trajectories of object are approximated to parabola)\n\nNow from your question we can have to situations:\n\nCASE-1: When the object is thrown inclined at an angle $\\theta_1$ with a velocity $u$\n\nThen the maximum height the object will reach is given by:\n\n$\\displaystyle h=\\frac{u^2\\sin^2\\theta_1}{2g}$\n\nNow if $\\theta_1= 30^\\circ$ and initial velocity $u= 100\\ \\mathrm{m/s}$ (just for consideration)\n\nThen the maximum Height the object will reach is equal to:\n\n$h= 127.55$ meters\n\nNow using the same angle and velocity, if we calculate the maximum distance traveled(called the range of projectile) we have\n\n$\\displaystyle R_\\text{max}=\\frac{u^2\\sin2\\theta_1}{g}$\n\nNow by plugging in the values, we have $R=883.69$ meters\n\nCASE-2: When the object is thrown at a higher angle than before but with same velocity.\n\nNow say the angle $\\theta_2=60^\\circ$ (Higher angle than before) and $u=100\\ \\mathrm{m/s}$\n\nThen by using the same equation used before we have\n\n$h= 382.65$ meters and $R= 441.83$ meters\n\nRESULT:\n\nWe can clearly see that the maximum height in case-1 is less than that of case-2 and the maximum range in case-1 is higher than that of case-2\n\nWhich means the path in case-1 is less high and more far. But the path in case-2 is higher and less far. See the below image for more clarification.",
null,
"(Sorry for the funky colors :P)\n\n• @VenomFangs \"The velocity is more important than the angle considering the type of path(parabolic, elliptical or hyperbolic)\". But since you asked about on earth phenomenon i would say that if the cannon was angled up slightly, the portion of the ellipse will look like \"elongated at the start and curving down faster at the end\" – hxri Mar 9 '16 at 14:49\n• This is a lovely answer. The only thing you could add (if you felt like it) is the calculation of the difference between the elliptical curve, and the parabolic approximation. This is something that would best be done numerically; I expect the difference is tiny (certainly much smaller than the difference due to ignoring effects of air drag and, in the case of a football, lift). – Floris Mar 9 '16 at 16:51\n• On the \"parabola vs. ellipse\" bit, if the Earth were flat, the football would, in fact, follow a parabolic trajectory. Since, on the scale of kicked footballs, the Earth looks flat, we can use the easier-to-calculate parabolic approximation rather than the exact elliptical solution. – Mark Mar 9 '16 at 21:36\n• 'The answer to your question is that the path of football is truly \"elliptical\" since its velocity is way less than escape velocity.' This is itself a weak gravity approximation. The real path of the object is to very high orders elliptical, but even neglecting air resistance etc., it is still not exact. – Zorawar Mar 9 '16 at 22:00\n• Absolutely right! Not many people aware of this fact. And we are all brainwashed in Physics 101 to believe the misconception of a parabolic flight path. Great presentation of the answer BTW. – docscience Mar 10 '16 at 15:35\n\nTo build up a little bit on our comments, do you mean that you expect the trajectory to be of different shape at the end than at the beginning ? This is again only possible with friction. If there is no friction, your Newton's equation of motion reads\n\n$m \\frac{d^2 \\vec{r}}{dt^2} = m \\vec{g}$\n\nand is invariant under the transformation $t \\mapsto -t$ (it is said to have time reversal symmetry). The practical consequence is that your trajectory must have some axis of symmetry : the football cannot move differently flying upwards than falling downwards because each of these movements map eachother through the time-reversal transformation.\n\nHowever, if you add a friction term like\n\n$m \\frac{d^2 \\vec{r}}{dt^2} = m \\vec{g} - k \\frac{d \\vec{r}}{dt}$\n\n(with $k >0$)\n\nthen you break time-reversal symmetry because $\\vec{v}$ becomes $- \\vec{v}$ under this transformation. Thus, as @leftaroundabout pointed out, you need a friction term to get the trajectory distorsion you described in your question."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9533185,"math_prob":0.96690404,"size":2234,"snap":"2019-43-2019-47","text_gpt3_token_len":476,"char_repetition_ratio":0.09372197,"word_repetition_ratio":0.005586592,"special_character_ratio":0.20411818,"punctuation_ratio":0.108490564,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9955253,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12],"im_url_duplicate_count":[null,5,null,5,null,5,null,5,null,5,null,5,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-10-17T00:08:11Z\",\"WARC-Record-ID\":\"<urn:uuid:f7809b8d-54d8-4e50-a7f6-fca6066c53f3>\",\"Content-Length\":\"162057\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:32f7c5ee-14ec-42d8-ab5c-368c25a7f456>\",\"WARC-Concurrent-To\":\"<urn:uuid:bbea5f70-9824-4f5c-9bee-060c3c3a41eb>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://physics.stackexchange.com/questions/242437/throwing-a-football-is-it-truly-parabolic\",\"WARC-Payload-Digest\":\"sha1:WL7DFK5E4IUSMHLJTLVSPKK6OB5TH7RH\",\"WARC-Block-Digest\":\"sha1:OENVNPDF6SJMW4MDJHLZD72TU7JEVJ4J\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-43/CC-MAIN-2019-43_segments_1570986672431.45_warc_CC-MAIN-20191016235542-20191017023042-00097.warc.gz\"}"} |
https://www.800score.com/gmat-prep/prep-guide/independent-events/ | [
"## Independent Events\n\nTwo outcomes are independent if the occurrence of one outcome has no effect on the occurrence of the other. For example, if a coin is tossed twice, the first outcome (H or T) has no effect on the second outcome (H or T).\n\nThere are two ways multiple events can take place in a single probability problem: either they can each occur separately (A or B) or they must occur together (A and B).\n\n## “Or”\n\nIn some scenarios, the events do not have to occur together to have the desired result. One of the events is enough.\n\nI will be happy today if I win the lottery OR have email.\n\n“Or” means that either outcome is desired. With more possible desired outcomes, the probability is greater than for one event alone.\n\nFor independent events with “or,” add the probabilities of the events.\n\nA fair six-sided die is rolled once. What is the probability of rolling a 5 or a 6?\n\n### Solution\n\nFirst, notice the word “or” in the question. There are 6 possible outcomes, and either a 5 or a 6 is wanted. There is a 1 in 6 probability of a 5 and a 1 in 6 probability of a 6.\n\nBottom: 6 outcomes are possible\nTop: 2 possible desired outcomes\nProbability: \\dfrac{2}{6} = \\dfrac{1}{3}\n\nA deck of 52 cards contains cards numbered 1 through 13 in each of 4 different colors. John will win $100 if he pulls a card numbered either 7 or 9 from the deck. What is the probability that John will win$100?\n\n### Solution\n\nJohn can win by pulling out either a 7 or a 9. His chance of doing this is higher than if he could only win by pulling out a 7. In that case, he’d only have 4 cards that would win, in this case there are 8 winning cards.\n\nMethod 1\n\nTo find the total probability, figure out the probability of each event and then add probabilities.\n\nPulling a 7\nBottom: 52 outcomes are possible\nTop: 4 possible desired outcomes\nProbability: \\dfrac{4}{52} = \\dfrac{1}{13}\n\nPulling a 9\nBottom: 52 outcomes are possible\nTop: 4 possible desired outcomes\nProbability: \\dfrac{4}{52} = \\dfrac{1}{13}\n\nProbability of pulling a 7 or a 9:\n\\dfrac{1}{13} + \\dfrac{1}{13} = \\dfrac{2}{13}\n\nMethod 2\n\nBecause the total possible outcomes are the same for both events, there is no need to calculate their probabilities separately.\nBottom: 52 outcomes are possible\nTop: 8 possible desired outcomes\nProbability: \\dfrac{8}{52} = \\dfrac{2}{13}\n\nA fair coin is flipped 3 times. What is the probability that heads will come up only once?\n\n### Solution\n\nThis is an “or” question, even though the word “or” isn’t written. The probability is independent. Think about what it means to have heads come up only once. Be careful to recognize that the desired outcome is heads only once, not at least once. Write the possible desired scenarios.\n\nH T T or T H T or T T H\n\nThere are three outcomes that would achieve the desired result.\n\nProbability of H T T = \\dfrac{1}{2} × \\dfrac{1}{2} × \\dfrac{1}{2} = \\dfrac{1}{8}\n\nProbability of T H T = \\dfrac{1}{2} × \\dfrac{1}{2} × \\dfrac{1}{2} = \\dfrac{1}{8}\n\nProbability of T T H = \\dfrac{1}{2} × \\dfrac{1}{2} × \\dfrac{1}{2} = \\dfrac{1}{8}\n\nSince these are independent events, add.\n\n\\dfrac{1}{8} × \\dfrac{1}{8} × \\dfrac{1}{8} = \\dfrac{3}{8}\nA fair coin is flipped once. A fair six-sided die is rolled once. What is the probability of getting a heads or rolling a 3?\n\n### Solution\n\nThe probabilities are independent. Each event has a different number of possible outcomes. The only way to solve this type of problem, where the events have a different number of possible outcomes, is to add the separate probabilities.\n\nBottom: 2 outcomes are possible\nTop: 1 possible desired outcome\nProbability: \\dfrac{1}{2}\n\nRolling a 3\nBottom: 6 outcomes are possible\nTop: 1 possible desired outcome\nProbability: \\dfrac{1}{6}\n\nProbability of getting a heads or rolling a 3: \\dfrac{1}{2} + \\dfrac{1}{6} = \\dfrac{3}{6} + \\dfrac{1}{6}\n= \\dfrac{4}{6} = \\dfrac{2}{3}\n\n## “And”\n\nIn some scenarios, all the events have to occur in order to attain the desired result.\n\nI will be happy today if I win the lottery AND have email.\n\n“And” means that both outcomes are needed. With more outcomes required, the probability is less.\n\nFor independent events with “and,” multiply the probabilities of the events.\n\n#### 800score Tip\n\nIn general, the probability of many events occurring is less than just one event occurring.\n\nProbability is expressed as a fraction between 0 and 1. When you multiply these fractions, you get smaller fractions, as in “AND” scenarios. When you add these fractions you get greater fractions, as in “OR” scenarios.\n\nIf a coin is tossed twice, what is the probability that the first toss is heads and the second toss is tails?\n\n### Solution\n\nFirst, notice the word “and” in the question. That means both events must occur. So the desired coin toss is H T.\n\nThe probability that the coin will land on heads is \\dfrac{1}{2}. The probability that the coin will land on tails is also \\dfrac{1}{2}.\n\nSince both must happen, multiply the individual probabilities.\n\n\\dfrac{1}{2} × \\dfrac{1}{2} = \\dfrac{1}{4}\n\nAs expected, the probability of both events occurring is less than the probabilities of either individual event occurring.\n\nNot all “and” questions will include the word “and.” It may say “then” or “both” or it may just be implied.\n\nTwo fair six-sided die are rolled once. What is the probability of rolling two fives?\n\n### Solution\n\nIn this case, the first die must be a 5 and the second die must also be a 5. This is an implied “and.”\n\nProbability of a 5 on the first die is \\dfrac{1}{6}\n\nProbability of a 5 on the second die is \\dfrac{1}{6}\n\nProbability both are 5 is \\dfrac{1}{6} × \\dfrac{1}{6}\n= \\dfrac{1}{36}\n\n## With Replacement\n\nSometimes independent event questions use the term “with replacement.” This means that the first card or marble that is chosen is put back or replaced, so it could be chosen again and not affect the probability of subsequent events (i.e., all the events are independent).\n\nTwo tokens are pulled from a bag that contains 52 tokens, an equal number of which are red, blue, green and white. After the first token is pulled it is placed back in the bag, then the second token is pulled. What is the probability that both tokens are red?\n\n### Solution\n\nSince both tokens must be red, this is an “and” question. Since the events are the same and the first token is replaced, they will each have the same probability. Calculate the probability then multiply.\n\nBottom: 52 outcomes are possible\nTop: 13 tokens are red\nProbability: \\dfrac{13}{52} = \\dfrac{1}{4}\n\nProbability of pulling 2 reds:\n\\dfrac{1}{4} × \\dfrac{1}{4} = \\dfrac{1}{16}\n\nA bag contains 3 white marbles, 2 blue marbles and 5 red marbles. What is the probability of drawing a red marble then a blue marble if the first marble is replaced after it is pulled?\n\n### Solution\n\nThe “then” in the question implies “and.” Since both outcomes must occur, and there is replacement, these are independent events. Multiply the probabilities.\n\nProbability of a red marble\nBottom: 10 outcomes are possible\nTop: 5 marbles are red\nProbability: \\dfrac{5}{10} = \\dfrac{1}{2}\n\nProbability of a blue marble\nBottom: 10 outcomes are possible\nTop: 2 marbles are blue\nProbability: \\dfrac{2}{10} = \\dfrac{1}{5}\n\nProbability of red then blue:\n\\dfrac{1}{2} × \\dfrac{1}{5} = \\dfrac{1}{10}\n\n#### Independent Events\n\nBest viewed in landscape mode\n\n2 questions with video explanations\n\n100 seconds per question",
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https://www.nagwa.com/en/videos/369162172531/ | [
"Question Video: Dividing Two-Digit Numbers by Eight Mathematics • 3rd Grade\n\nThe robot divides any number by 8 and gives a result. In this case, the number 16 gives a result of 2 as 16 ÷ 8 = 2. What will the result be in the following case? 40 ÷ 8 = _ What will the result be in the following case? 64 ÷ 8 = _\n\n03:15\n\nVideo Transcript\n\nThis robot divides any number by eight and gives a result. In this case, the number 16 gives a result of two as 16 divided by eight equals two. What will the result be in the following case? 40 divided by eight equals what. And what will the result be in the following case? 64 divided by eight equals what.\n\nIn the first part of this question, we have to help the robot calculate 40 divided by eight. And in the second part of the question, we have to help the robot calculate 64 divided by eight. Did you notice that in all of the calculations we’re dividing by eight? How could we calculate 40 divided by eight? We could use an array and our knowledge of the eight times table to help.\n\nWhen we’re dividing by eight, we can think of this as dividing a number into equal groups of eight. Here’s one group of eight, which gives us a total of eight. Two eights make 16. Three eights make 24. Eight, 16, 24. Four eights are 32, and five eights make 40. Eight, 16, 24, 32, 40. So, if the number 40 goes in and the robot divides it by eight, the result will be five. There are five eights in 40. 40 divided by eight equals five.\n\nNow, we just need to answer the second part of the question. What is 64 divided by eight? How many eights are there in 64? Let’s keep on counting in eights. We already know that five groups of eight makes 40, so let’s just keep counting forward in eights. Five eights are 40, six eights are 48, seven eights are 56, and eight eights are 64. There are eight eights in 64. If we put the number 64 into the robot and he divides it by eight, the result will be eight because 64 divided by eight equals eight.\n\n40 divided by eight equals five and 64 divided by eight equals eight. We found the results using arrays and our knowledge of the eight times table."
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https://math.stackexchange.com/questions/793754/let-f-n-n-in-mathbbn-rightarrow-f-on-0-infty-true-or-false-lim/793792 | [
"# Let $(f_n)_{n\\in\\mathbb{N}} \\rightarrow f$ on $[0,\\infty)$. True or false: $\\lim_{n\\to\\infty}\\int_0^{\\infty}f_n(x) \\ dx = \\int_0^{\\infty}f(x) \\ dx.$\n\nThe Assignment:\n\nLet $(f_n)_{n\\in\\mathbb{N}}$ converge uniformly to $f$ on $[0,\\infty)$ and let the improper integrals of $f_n$ and $f$ exist on $[0,\\infty)$. True or false: $$\\lim_{n\\to\\infty}\\int_0^{\\infty}f_n(x) \\ dx = \\int_0^{\\infty}f(x) \\ dx$$ Prove it.\n\nSince I know that under certain circumstances (if $f_n$ is integrable $\\forall n≥1$) on the closed interval $[a,b]$: $$\\lim_{n\\to\\infty} \\int_a^bf_n(x) \\ dx = \\int_a^bf(x) \\ dx$$ I have the tendency to say that the statement above is false, since these \"safe\" conditions (compact interval) are substituted by others.\n\nAny help would be appreciated\n\n## 3 Answers\n\nHint:\n\nFill a rubber square aquarium with water until it's completely filled. Now, take the right edge of the aquarium and stretch it to the right. The amount of water never changes, even though the height of the water decreases. What happens when you keep stretching it farther and farther to the right, without restriction?\n\nEdit:\n\nSince I answered your question with a riddle, I'll add a useful tip that might seem more math-like:\n\nWhenever you encounter the question\n\nDoes condition XYZ guarantee $\\displaystyle \\lim_{n\\to\\infty} \\int f_n = \\int \\lim_{n\\to\\infty} f_n$ ?\n\nit is helpful to make the following observation:\n\nIf it is true in the special case that $f_n \\to 0$, then it is true anyway.\n\nThis observation helps you in that you only really need to prove this case, or to find a counterexample of this sort.\n\nProof: Suppose it is true in the special case $f_n \\to 0$. Consider another case, where $f_n \\to f \\ne 0$. Define the sequence $g_n = f_n - f$. Then $g_n \\to 0$, and condition XYZ probably holds for $g_n$ as well as it does for $f_n$, so you can get $\\lim \\int (f_n - f) = 0$, which is exactly what you want.\n\n• I'm still trying to figure out what you're trying to say. Basically you're comparing a definite integral from $0$ to $b$ with water in an rubber square aquarium. Stretching the right edge farther to the right without restriction lets $b \\to \\infty$. While it makes sense in your scenario, why would the integral \"even out\" when one bound is $\\infty$? Edit: I'll read through your edit now. – Nhat May 13 '14 at 22:30\n• The integral is the amount of water. Since the amount of water doesn't change, the integral of $f_n$ is always $1$. However, the integral of $f$ is $0$. (What are $f_n$ and $f$?) – Yoni Rozenshein May 13 '14 at 22:33\n• Firstly, I liked that riddle, haha. Also it hasn't come to my mind to only prove / disprove the special case for $f_n \\rightarrow f = 0$. ... So I'm looking for an $f_n$ such that $\\forall n \\in \\mathbb{N}$ $\\int_0^{\\infty}f_n \\ dx = 1$ and $f_n \\rightarrow 0$ uniformly? – Nhat May 13 '14 at 22:44\n• Yes, exactly. – Yoni Rozenshein May 13 '14 at 22:48\n• Can you help me or give me a hint? – Nhat May 13 '14 at 23:33\n\nConsider $f_n:=\\frac{1}{n}\\chi_{[n,2n]}$ where $\\chi$ denotes the indicator function. Obviously $||f_n||_\\infty\\to 0$, but $\\int_0^\\infty f_n=1~\\forall n\\in\\mathbb{N}$.\n\nConsider the flattening mountain of constant integral\n\n$\\begin{array}{ccccc} f_n & : & R^+ & \\to & R^+\\\\ & & x & \\mapsto &\\frac{x}{n^2}-1+\\frac{1}{n} \\; \\text{when} \\; n^2-n<x\\leq n^2\\\\ && x & \\mapsto & \\frac{-x}{n^2}+1+\\frac{1}{n} \\; \\text{when} \\; n^2<x<n^2 +n\\\\ && x & \\mapsto & 0\\text{when} \\; n^2-n>x \\; \\text{or} \\; x>n^2 +n \\\\ \\end{array}$\n\nEach $f_n$ has integral $1$ but the sequence converges uniformly to $0$."
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.76077694,"math_prob":0.99967253,"size":604,"snap":"2021-04-2021-17","text_gpt3_token_len":206,"char_repetition_ratio":0.115,"word_repetition_ratio":0.0,"special_character_ratio":0.33278146,"punctuation_ratio":0.08547009,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99984837,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-04-11T10:10:29Z\",\"WARC-Record-ID\":\"<urn:uuid:1effcebd-68b9-4888-9be0-8493a64069f2>\",\"Content-Length\":\"185481\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:d22f487d-f424-4ea9-8a52-f4754d20e1de>\",\"WARC-Concurrent-To\":\"<urn:uuid:67bc636b-bea1-4539-875a-0b9e7f97a2b0>\",\"WARC-IP-Address\":\"151.101.193.69\",\"WARC-Target-URI\":\"https://math.stackexchange.com/questions/793754/let-f-n-n-in-mathbbn-rightarrow-f-on-0-infty-true-or-false-lim/793792\",\"WARC-Payload-Digest\":\"sha1:3GDYLRTOBTCOEAVCCL2S4GFTXJD4Q5M6\",\"WARC-Block-Digest\":\"sha1:HQKYQ7GQUJNTPUOL24JVIGQRZ452XBMB\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-17/CC-MAIN-2021-17_segments_1618038061820.19_warc_CC-MAIN-20210411085610-20210411115610-00245.warc.gz\"}"} |
https://brainmass.com/economics/principles-of-mathematical-economics/mathematical-economics-price-output-determination-613736 | [
"Explore BrainMass\nShare\n\n# Mathematical Economics-Price and output determination\n\nThis content was COPIED from BrainMass.com - View the original, and get the already-completed solution here!\n\n1. Assume you are the manager of a firm that holds a patent that makes it the exclusive manufacturer of a unique SD card. Based on the estimates provided by a consultant, you know that the relevant demand and cost functions for this SD card are Q = 120 - 2P; C = 20 + 2.5Q2.\n\nWhat are the levels of quantity and price when you are maximizing profits? Show your work.\n\nWhat are the levels of quantity and price when you are maximizing profits? Show your work.\n\n2. Continuing from the previous question where you are a manager of a firm that holds a patent that makes it the exclusive manufacturer of a unique SD card with demand and cost functions for this SD card that are Q = 120 - 2P; C = 20 + 2.5Q2.\nCalculate the deadweight loss caused by the firm in this market. (Give the number only with no \\$, you will show your work on the next page.)\n\n3. Continuing from the previous question where you are a manager of a firm that holds a patent that makes it the exclusive manufacturer of a unique SD card with demand and cost functions for this SD card that are Q = 120 - 2P; C = 20 + 2.5Q2.\nCalculate the deadweight loss caused by the firm in this market.\n(On the previous page you input the numerical answer. Show your work here the best you can. No need to draw a graph, just give the key equations.)\n4. Continuing from the previous questions where you are a manager of a firm that holds a patent that makes it the exclusive manufacturer of a unique SD card with demand and cost functions for this SD card that are Q = 120 - 2P; C = 20 + 2.5Q2.\nNow assume that the firm incurs a one time cost of \\$10 for a zoning violation. What is the price that the manager should now charge to maximize profits? (Just give the number, no need to include \"\\$\")\n5. Assume a firm selling wine faces the following inverse demand curve: P = 30 − 2Q. The total cost function is TC= 10 + 1.5Q2. A local regulation states that wine must be sold for at least \\$20 per bottle. The firm plans to start a wine club and utilize 2-part pricing. Calculate the membership fee the firm will charge in order to maximize profits and comply with the regulation.\n(Give only the numerical answer with no dollar sign. You will show your work on the next page.)\n\n6. Assume a firm selling wine faces the following inverse demand curve: P = 30 − 2Q. The total cost function is TC= 10 + 1.5Q2. A local regulation states that wine must be sold for at least \\$20 per bottle. The firm plans to start a wine club and utilize 2-part pricing. Calculate the membership fee the firm will charge in order to maximize profits and comply with the regulation.\n(You already input in answer on the previous page. Show your work here the best you can. There is no need to draw a graph, just give your logic and key equations.)\n\n7. In the previous question the local regulation dictated that wine had to be sold for \\$20 per bottle. Explain how much surplus a typical consumer lost because of the regulation as compared to the situation where price is not regulated.\n\n© BrainMass Inc. brainmass.com March 22, 2019, 3:24 am ad1c9bdddf\nhttps://brainmass.com/economics/principles-of-mathematical-economics/mathematical-economics-price-output-determination-613736\n\n#### Solution Preview\n\nAnswer:\nGiven that,\nDemand function:\nQ=120-2P\nOr,\nP=(120-Q)/2\nCost function:\nC=20+2.5Q^2\nNow,\nRevenue=P*Q\nOr,\nRevenue=(120-Q)/2*Q=60Q-Q^2/2\nTherefore,\nMR=d(60Q-Q^2/2)/dQ=60-Q\nSimilarly,\nMC=dC/dQ=d(20+2.5Q^2 )/dQ\nOr,\nMC=5Q\nFor Profit maximization,\nMR=MC\nOr,\n60-Q=5Q\nOr,\nQ=10\nPutting ...\n\n#### Solution Summary\n\nThis answer helps to determine equilibrium price and output in different market structure.\n\n\\$2.19"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.9091856,"math_prob":0.9234633,"size":3763,"snap":"2019-35-2019-39","text_gpt3_token_len":948,"char_repetition_ratio":0.11066773,"word_repetition_ratio":0.5453149,"special_character_ratio":0.25777304,"punctuation_ratio":0.11153846,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98659855,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-08-21T03:51:13Z\",\"WARC-Record-ID\":\"<urn:uuid:84325af3-eca6-43c0-8e34-ac81ef53cf4e>\",\"Content-Length\":\"97672\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:fb03004c-b999-4fb0-89b9-19de674f5047>\",\"WARC-Concurrent-To\":\"<urn:uuid:cdc4c83d-f66c-4e64-b9a9-179279d9c38a>\",\"WARC-IP-Address\":\"65.39.198.123\",\"WARC-Target-URI\":\"https://brainmass.com/economics/principles-of-mathematical-economics/mathematical-economics-price-output-determination-613736\",\"WARC-Payload-Digest\":\"sha1:WBA6PVKDQNPN4NBZV6Y2EKIRXLJYSPUF\",\"WARC-Block-Digest\":\"sha1:URT5NCKXXEZ32JR3PVHSNDMKEV764H7U\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-35/CC-MAIN-2019-35_segments_1566027315750.62_warc_CC-MAIN-20190821022901-20190821044901-00003.warc.gz\"}"} |
https://thetisproject.org/demos/demo_2d_channel_bnd.py.html | [
"# 2D channel with time-dependent boundary conditions¶\n\nHere we extend the 2D channel example by adding constant and time dependent boundary conditions.\n\nWe begin by defining the domain and solver as before:\n\nfrom thetis import *\n\nlx = 40e3\nly = 2e3\nnx = 25\nny = 2\nmesh2d = RectangleMesh(nx, ny, lx, ly)\n\nP1_2d = FunctionSpace(mesh2d, 'CG', 1)\nbathymetry_2d = Function(P1_2d, name='Bathymetry')\ndepth = 20.0\nbathymetry_2d.assign(depth)\n\n# total duration in seconds\nt_end = 12 * 3600\n# export interval in seconds\nt_export = 300.0\n\nsolver_obj = solver2d.FlowSolver2d(mesh2d, bathymetry_2d)\noptions = solver_obj.options\noptions.simulation_export_time = t_export\noptions.simulation_end_time = t_end\noptions.timestepper_type = 'CrankNicolson'\noptions.timestep = 50.0\n\n\nWe will force the model with a constant volume flux at the right boundary (x=40 km) and impose a tidal volume flux on the left boundary (x=0 km). Note that we have increased t_end and t_export to better illustrate tidal dynamics.\n\nBoundary condtitions are defined for each external boundary using their ID. In this example we are using a RectangleMesh() which assigns IDs 1, 2, 3, and 4 for the four sides of the rectangle:\n\nleft_bnd_id = 1\nright_bnd_id = 2\n\n\nAt each boundary we need to define the external value of the prognostic variables, i.e. in this case the water elevation and velocity. The value should be either a Firedrake Constant or Function (in case the boundary condition is not uniform in space).\n\nWe store the boundary conditions in a dictionary:\n\nswe_bnd = {}\nin_flux = 1e3\nswe_bnd[right_bnd_id] = {'elev': Constant(0.0),\n'flux': Constant(-in_flux)}\n\n\nAbove we set the water elevation to zero and prescribe a constant volume flux. The volume flux is defined as outward normal flux, i.e. a negative value stands for flow into the domain. Alternatively we could also prescribe the normal velocity (with key 'un') or the 2D velocity vector ('uv'). For all supported boundary conditions, see module shallowwater_eq.\n\nIn order to set time-dependent boundary conditions we first define a python function that evaluates the time dependent variable:\n\ndef timedep_flux(simulation_time):\n\"\"\"Time-dependent flux function\"\"\"\ntide_amp = -2e3\ntide_t = 12 * 3600.\nflux = tide_amp*sin(2 * pi * simulation_time / tide_t) + in_flux\nreturn flux\n\n\nWe then create a Constant object with the initial value, and assign it to the left boundary:\n\ntide_flux_const = Constant(timedep_flux(0))\nswe_bnd[left_bnd_id] = {'flux': tide_flux_const}\n\n\nBoundary conditions are now complete, and we assign them to the solver object:\n\nsolver_obj.bnd_functions['shallow_water'] = swe_bnd\n\n\nNote that if boundary conditions are not assigned for some boundaries (the lateral boundaries 3 and 4 in this case), Thetis assumes impermeable land conditions.\n\nThe only missing piece is to add a mechanism that re-evaluates the boundary condition as the simulation progresses. For this purpose we use the optional update_forcings argument of the iterate() method. update_forcings is a python function that updates all time dependent Constants or Functions used to force the model. In this case we only need to update tide_flux_const:\n\ndef update_forcings(t_new):\n\"\"\"Callback function that updates all time dependent forcing fields\"\"\"\ntide_flux_const.assign(timedep_flux(t_new))\n\n\nand finally pass this callback to the time iterator:\n\nsolver_obj.iterate(update_forcings=update_forcings)\n\n\nThis tutorial can be dowloaded as a Python script here."
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https://www.queryhome.com/puzzle/34024/what-the-average-of-all-multiples-of-lying-between-424-and-530 | [
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"# What is the average of all multiples of 12 lying between 424 and 530?\n\n44 views\nWhat is the average of all multiples of 12 lying between 424 and 530?",
null,
"posted Dec 12, 2019\n\nMultiples of 12 between 424 to 530 are 36*12 to 44*12 - total 9 numbers\naverage = 40*12=480",
null,
"answer Dec 12, 2019\n\nSimilar Puzzles\n+1 vote\n\nThe average marks of three batches of 55, 60 and 45 students respectively is 50, 55, 60.\nWhat is the average marks of all the students?"
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https://ai.stackexchange.com/questions/9236/why-do-we-apply-the-mutation-operation-after-generating-the-offspring/9416 | [
"# Why do we apply the mutation operation after generating the offspring?\n\nWhy do we apply the mutation operation after generating the offspring, in genetic algorithms?\n\nThe mutation operation is (usually) needed to introduce new genes not found in the population.\n\nFor example, suppose that you have 4 possible genes $$A$$, $$B$$, $$C$$, and $$D$$, and that your chromosomes have a non-binary encoding. In that case, if no member of your population has the gene $$D$$, then no amount of crossover operations will result in the introduction of that gene.\n\nHowever, if your chromosomes use a binary encoding, then new genes could be introduced as a side effect of crossover operations. But it is always safer to have some kind of mutation to ensure that all genes can be accessed.\n\nSee also the paper Genetic Algorithm for Traveling Salesman Problem with Modified Cycle Crossover Operator, which mentions several non-binary encodings for the TSP.\n\nMutation is used to maintain diversity in the solutions. Crossover alone cannot do this.\n\n• This might be correct, but you should provide more details about why that is the case, because it's not obvious why the cross-over alone doesn't introduce diversity. In fact, it does, but to what degree? The other answer actually provide an example of when the mutation could be useful, but you should also extend this answer to provide more details. Right now, this answer looks like a comment, so it should be converted to a comment.\n– nbro\nJun 15, 2022 at 13:52"
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https://converterin.com/astronomical/kilometer-km-to-light-year-julian-ly.html | [
"# KILOMETER TO LIGHT YEAR [JULIAN] CONVERTER\n\nFROM\nTO\n\nThe result of your conversion between kilometer and light year [Julian] appears here\n\n## KILOMETER TO LIGHT YEAR [JULIAN] (km TO ly) FORMULA\n\nTo convert between Kilometer and Light Year [Julian] you have to do the following:\n\nFirst divide 1000 / 299792458 * 60 * 60 * 24 * 365.25 = 0.\n\nThen multiply the amount of Kilometer you want to convert to Light Year [Julian], use the chart below to guide you.\n\n## KILOMETER TO LIGHT YEAR [JULIAN] (km TO ly) CHART\n\n• 1 kilometer in light year [Julian] = 0. km\n• 10 kilometer in light year [Julian] = 0. km\n• 50 kilometer in light year [Julian] = 0. km\n• 100 kilometer in light year [Julian] = 0. km\n• 250 kilometer in light year [Julian] = 0. km\n• 500 kilometer in light year [Julian] = 0. km\n• 1,000 kilometer in light year [Julian] = 0. km\n• 10,000 kilometer in light year [Julian] = 0. km\n\nSymbol: km\n\nNo description\n\nSymbol: ly\n\nNo description"
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https://nim-lang.org/docs/editdistance.html | [
"# editdistance\n\nDark Mode\nSearch:\nGroup by:\n\nThis module implements an algorithm to compute the edit distance between two Unicode strings.\n\nunicode\n\n# Procs\n\n`proc editDistance(a, b: string): int {...}{.noSideEffect, raises: [], tags: [].}`\n\nReturns the unicode-rune edit distance between a and b.\n\nThis uses the Levenshtein distance algorithm with only a linear memory overhead.\n\nExamples:\n\n```static:\ndoAssert editdistance(\"Kitten\", \"Bitten\") == 1```\nSource Edit\n`proc editDistanceAscii(a, b: string): int {...}{.noSideEffect, raises: [], tags: [].}`\n\nReturns the edit distance between a and b.\n\nThis uses the Levenshtein distance algorithm with only a linear memory overhead.\n\nExamples:\n\n```static:\ndoAssert editDistanceAscii(\"Kitten\", \"Bitten\") == 1```\nSource Edit"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.6889691,"math_prob":0.92649907,"size":690,"snap":"2020-24-2020-29","text_gpt3_token_len":169,"char_repetition_ratio":0.12973762,"word_repetition_ratio":0.54347825,"special_character_ratio":0.24782608,"punctuation_ratio":0.2734375,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95404476,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-05-29T19:51:40Z\",\"WARC-Record-ID\":\"<urn:uuid:a4dc3b95-6b25-4e03-922a-77fc770a4853>\",\"Content-Length\":\"13057\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ea992e18-3189-46bb-9a87-30cf0ea4fc3f>\",\"WARC-Concurrent-To\":\"<urn:uuid:e7960e88-0d82-4ee0-b26c-40bd4e5578dd>\",\"WARC-IP-Address\":\"104.28.19.79\",\"WARC-Target-URI\":\"https://nim-lang.org/docs/editdistance.html\",\"WARC-Payload-Digest\":\"sha1:WABRFWHDTZALALOFL6HSLUBYXXFP427H\",\"WARC-Block-Digest\":\"sha1:SW2LR6FKKGJGOA54XRZAYKIQBW6Y3H3R\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590347406365.40_warc_CC-MAIN-20200529183529-20200529213529-00318.warc.gz\"}"} |
https://number.academy/1003345 | [
"# Number 1003345\n\nNumber 1,003,345 spell 🔊, write in words: one million, three thousand, three hundred and forty-five, approximately 1.0 million. Ordinal number 1003345th is said 🔊 and write: one million, three thousand, three hundred and forty-fifth. The meaning of the number 1003345 in Maths: Is it Prime? Factorization and prime factors tree. The square root and cube root of 1003345. What is 1003345 in computer science, numerology, codes and images, writing and naming in other languages\n\n## What is 1,003,345 in other units\n\nThe decimal (Arabic) number 1003345 converted to a Roman number is (M)MMMCCCXLV. Roman and decimal number conversions.\n\n#### Weight conversion\n\n1003345 kilograms (kg) = 2211974.4 pounds (lbs)\n1003345 pounds (lbs) = 455114.3 kilograms (kg)\n\n#### Length conversion\n\n1003345 kilometers (km) equals to 623450 miles (mi).\n1003345 miles (mi) equals to 1614728 kilometers (km).\n1003345 meters (m) equals to 3291775 feet (ft).\n1003345 feet (ft) equals 305824 meters (m).\n1003345 centimeters (cm) equals to 395017.7 inches (in).\n1003345 inches (in) equals to 2548496.3 centimeters (cm).\n\n#### Temperature conversion\n\n1003345° Fahrenheit (°F) equals to 557396.1° Celsius (°C)\n1003345° Celsius (°C) equals to 1806053° Fahrenheit (°F)\n\n#### Time conversion\n\n(hours, minutes, seconds, days, weeks)\n1003345 seconds equals to 1 week, 4 days, 14 hours, 42 minutes, 25 seconds\n1003345 minutes equals to 2 years, 3 weeks, 3 days, 18 hours, 25 minutes\n\n### Codes and images of the number 1003345\n\nNumber 1003345 morse code: .---- ----- ----- ...-- ...-- ....- .....\nSign language for number 1003345:",
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"Number 1003345 in braille:",
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"QR code Bar code, type 39",
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"",
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"Images of the number Image (1) of the number Image (2) of the number",
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"More images, other sizes, codes and colors ...\n\n## Share in social networks",
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"## Mathematics of no. 1003345\n\n### Multiplications\n\n#### Multiplication table of 1003345\n\n1003345 multiplied by two equals 2006690 (1003345 x 2 = 2006690).\n1003345 multiplied by three equals 3010035 (1003345 x 3 = 3010035).\n1003345 multiplied by four equals 4013380 (1003345 x 4 = 4013380).\n1003345 multiplied by five equals 5016725 (1003345 x 5 = 5016725).\n1003345 multiplied by six equals 6020070 (1003345 x 6 = 6020070).\n1003345 multiplied by seven equals 7023415 (1003345 x 7 = 7023415).\n1003345 multiplied by eight equals 8026760 (1003345 x 8 = 8026760).\n1003345 multiplied by nine equals 9030105 (1003345 x 9 = 9030105).\nshow multiplications by 6, 7, 8, 9 ...\n\n### Fractions: decimal fraction and common fraction\n\n#### Fraction table of 1003345\n\nHalf of 1003345 is 501672,5 (1003345 / 2 = 501672,5 = 501672 1/2).\nOne third of 1003345 is 334448,3333 (1003345 / 3 = 334448,3333 = 334448 1/3).\nOne quarter of 1003345 is 250836,25 (1003345 / 4 = 250836,25 = 250836 1/4).\nOne fifth of 1003345 is 200669 (1003345 / 5 = 200669).\nOne sixth of 1003345 is 167224,1667 (1003345 / 6 = 167224,1667 = 167224 1/6).\nOne seventh of 1003345 is 143335 (1003345 / 7 = 143335).\nOne eighth of 1003345 is 125418,125 (1003345 / 8 = 125418,125 = 125418 1/8).\nOne ninth of 1003345 is 111482,7778 (1003345 / 9 = 111482,7778 = 111482 7/9).\nshow fractions by 6, 7, 8, 9 ...\n\n### Calculator\n\n 1003345\n\n#### Is Prime?\n\nThe number 1003345 is not a prime number. The closest prime numbers are 1003337, 1003349.\n\n#### Factorization and factors (dividers)\n\nThe prime factors of 1003345 are 5 * 7 * 109 * 263\nThe factors of 1003345 are\n1, 5, 7, 35, 109, 263, 545, 763, 1315, 1841, 3815, 9205, 28667, 143335, 200669, 1003345.\nTotal factors 16.\nSum of factors 1393920 (390575).\n\n#### Powers\n\nThe second power of 10033452 is 1.006.701.189.025.\nThe third power of 10033453 is 1.010.068.604.502.288.640.\n\n#### Roots\n\nThe square root √1003345 is 1001,671104.\nThe cube root of 31003345 is 100,111376.\n\n#### Logarithms\n\nThe natural logarithm of No. ln 1003345 = loge 1003345 = 13,81885.\nThe logarithm to base 10 of No. log10 1003345 = 6,00145.\nThe Napierian logarithm of No. log1/e 1003345 = -13,81885.\n\n### Trigonometric functions\n\nThe cosine of 1003345 is -0,405071.\nThe sine of 1003345 is 0,914285.\nThe tangent of 1003345 is -2,257101.\n\n### Properties of the number 1003345\n\nIs a Fibonacci number: No\nIs a Bell number: No\nIs a palindromic number: No\nIs a pentagonal number: No\nIs a perfect number: No\n\n## Number 1003345 in Computer Science\n\nCode typeCode value\n1003345 Number of bytes979.8KB\nUnix timeUnix time 1003345 is equal to Monday Jan. 12, 1970, 2:42:25 p.m. GMT\nIPv4, IPv6Number 1003345 internet address in dotted format v4 0.15.79.81, v6 ::f:4f51\n1003345 Decimal = 11110100111101010001 Binary\n1003345 Decimal = 1212222022221 Ternary\n1003345 Decimal = 3647521 Octal\n1003345 Decimal = F4F51 Hexadecimal (0xf4f51 hex)\n1003345 BASE64MTAwMzM0NQ==\n1003345 SHA18e0b08f4d2f4273777cdee19d58ccdd31078ed85\n1003345 SHA22497a8385458b84dcb1b999e29f400359bf963872d717c6be0c1f05571\n1003345 SHA256c7daa88735b900ab3cb96609bc29ec6c77f8e2bb8ba29aa2b2569e46ed4ea5c4\n1003345 SHA384cd1ea00db9474c367b0f698e41df1240a934b0bbcf798fa0b77da0e40b7f6966b3be445d995f2a4e14b1557832cc4376\nMore SHA codes related to the number 1003345 ...\n\nIf you know something interesting about the 1003345 number that you did not find on this page, do not hesitate to write us here.\n\n## Numerology 1003345\n\n### Character frequency in the number 1003345\n\nCharacter (importance) frequency for numerology.\n Character: Frequency: 1 1 0 2 3 2 4 1 5 1\n\n### Classical numerology\n\nAccording to classical numerology, to know what each number means, you have to reduce it to a single figure, with the number 1003345, the numbers 1+0+0+3+3+4+5 = 1+6 = 7 are added and the meaning of the number 7 is sought.\n\n## № 1,003,345 in other languages\n\nHow to say or write the number one million, three thousand, three hundred and forty-five in Spanish, German, French and other languages. The character used as the thousands separator.\n Spanish: 🔊 (número 1.003.345) un millón tres mil trescientos cuarenta y cinco German: 🔊 (Nummer 1.003.345) eine Million dreitausenddreihundertfünfundvierzig French: 🔊 (nombre 1 003 345) un million trois mille trois cent quarante-cinq Portuguese: 🔊 (número 1 003 345) um milhão e três mil, trezentos e quarenta e cinco Hindi: 🔊 (संख्या 1 003 345) दस लाख, तीन हज़ार, तीन सौ, पैंतालीस Chinese: 🔊 (数 1 003 345) 一百万三千三百四十五 Arabian: 🔊 (عدد 1,003,345) واحد مليون و ثلاثة آلاف و ثلاثمائة و خمسة و أربعون Czech: 🔊 (číslo 1 003 345) milion tři tisíce třista čtyřicet pět Korean: 🔊 (번호 1,003,345) 백만 삼천삼백사십오 Dutch: 🔊 (nummer 1 003 345) een miljoen drieduizenddriehonderdvijfenveertig Japanese: 🔊 (数 1,003,345) 百万三千三百四十五 Indonesian: 🔊 (jumlah 1.003.345) satu juta tiga ribu tiga ratus empat puluh lima Italian: 🔊 (numero 1 003 345) un milione e tremilatrecentoquarantacinque Norwegian: 🔊 (nummer 1 003 345) en million, tre tusen, tre hundre og førti-fem Polish: 🔊 (liczba 1 003 345) milion trzy tysiące trzysta czterdzieści pięć Russian: 🔊 (номер 1 003 345) один миллион три тысячи триста сорок пять Turkish: 🔊 (numara 1,003,345) birmilyonüçbinüçyüzkırkbeş Thai: 🔊 (จำนวน 1 003 345) หนึ่งล้านสามพันสามร้อยสี่สิบห้า Ukrainian: 🔊 (номер 1 003 345) один мільйон три тисячі триста сорок п'ять Vietnamese: 🔊 (con số 1.003.345) một triệu ba nghìn ba trăm bốn mươi lăm Other languages ...\n\n## News to email\n\nI have read the privacy policy\n\n## Comment\n\nIf you know something interesting about the number 1003345 or any other natural number (positive integer), please write to us here or on Facebook.\n\n#### Comment (Maximum 2000 characters) *\n\nThe content of the comments is the opinion of the users and not of number.academy. It is not allowed to pour comments contrary to the laws, insulting, illegal or harmful to third parties. Number.academy reserves the right to remove or not publish any inappropriate comment. It also reserves the right to publish a comment on another topic. Privacy Policy."
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https://www.newsxy.in/what-is-dac.html | [
"",
null,
"# what is dac\n\n### What is a Digital-to-analog converter\n\nA digital to analog (D/A) converter is a device that generates an analog voltage signal in response to its digital representation. Modern electronic devices often utilize signals or processing of signals in a digital format because digital signals or digital signal processing may have numerous advantages over working with or utilizing signals that are in the analog domain. For example, communication devices often receive an analog voice signal from a microphone, and convert this signal to a digital format for processing. Digital to analog converters are an essential interface circuit from the digital domain into the analog domain and, particularly, the analog signal processing domain. Digital to analog converters are widely used in mixed-mode systems requiring monotonicity where the converter acts as an interface between the digital signal processing and analog signal processing components of such systems. Digital to analog converters are also a key to many analog to digital converter techniques. A DAC takes the binary bits of a digital input signal, which originate from a computer or other type of discrete circuitry, and converts the digital input signal into an analog output voltage that can be used to drive analog devices. D/A converters are designed to convert an N-bit digital value into a corresponding analog signal level. The number (N) of bits forming the N-bit digital value may be as low as two, but 6- and 8-bit D/A converters are ubiquitous, and 16-bit D/A converters are not uncommon. A D/A converter for converting discrete digital data into continuous analog signals can be a converter of ladder resistance network type, segment type, integral type, etc. A D/A converter is typically composed of several DAC elements, which receive digital input data and generate element signals according to the digital input data. The element signal can be voltage type or current type. A signal integrator (or a summing node) adds the element signals outputted from the DAC elements and generates an analog output signal. A DAC can be implemented with an array of weighted analog components that are controlled by an incoming digital code. The outputs of the weighted analog components are then summed and filtered to reproduce a continuous-time signal."
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https://345pi.net/lessons/differential/ | [
"# Differential\n\nDifferential Equations\n\nWe know how to find derivatives of functions in the standard form. However not all functions look like that. The hyperbola is one such example of not following this rule. If we wanted to calculate the slope at say this point how would we do that? Well it is possible, but we have to use slightly more sophisticated derivatives. Let’s take a look at a simpler function such as the function $x + y = 1$. Next let’s see how the differentiation of the function of the circle works. Take $x^2 + y^2 = 1$ and then take the derivative. This type of equation is what we call a differential equation. Differential equations are common in calculus where you can get a formula for the slope of an equation, but need to figure out the initial equation itself.\n\nTo do this we must do the process backwards with integration. If we were given the differential equation $\\frac{dy}{dx}=xy$ and asked to find the equation of this graph how would we do it? Then we must remember to add a $+ C$ to one side of the equation. This is because we don’t know exactly where the graph is on the slope field of the equation and different starting points can give vastly different results.\n\n##### Course Vocabulary\n• Differential Equation – an equation involving a derivative\n• Antiderivative of f(x) – The function who’s derivative is equal to f(x)\n• Slope Field – a graph displaying the slope of a function at specific points\n\nWhat is the slope of a parabola?\n\nUsing differential equations what is the slope of a hyperbola centered at the origin, where $a$ and $b$ are $1$. Once you have done this graph the slope field and try to figure out what happens to the hyperbola as your $x$ and $y$ values get very large. Does the hyperbola approach a specific value, what happens if you change the values of $a$ and $b$?\n\nRemember to take the quiz before moving on!\n\nLesson Content"
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https://www.easycalculation.com/square-roots-79.html | [
"# What is Square Root of 79 ?\n\nSeventy nine is the 22nd prime number. It is an emirp, because the reverse of 79 is 97 which is also a prime number. The square root of 79 is equal to 8.88819\n\nSquare Root of 79\n √79 = √(8.888 x 8.888) 8.88819\n\nSeventy nine is the 22nd prime number. It is an emirp, because the reverse of 79 is 97 which is also a prime number. The square root of 79 is equal to 8.88819\n\nThe nearest previous perfect square is 64 and the nearest next perfect square is 81 ."
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http://przyrbwn.icm.edu.pl/APP/ABSTR/121/a121-1a-37.html | [
"Determining the Distribution of Values of Stochastic Impulses Acting on a Discrete System in Relation to Their Intensity M. Jabłońskia and A. Ozgab aFaculty of Mathematics and Computer Science, Jagiellonian University, Gołębia 24, 31-007 Cracow, Poland bAGH University of Science and Technology, Faculty of Mechanical Engineering and Robotics, Department of Mechanics and Vibroacoustics, al. A. Mickiewicza 30, 30-059 Krakow, Poland Full Text PDF In our previous works we introduced and applied a mathematical model that allowed us to calculate the approximate distribution of the values of stochastic impulses ηi forcing vibrations of an oscillator with damping from the trajectory of its movement. The mathematical model describes correctly the functioning of a physical RLC system if the coefficient of damping is large and the intensity λ of impulses is small. It is so because the inflow of energy is small and behaviour of RLC is stable. In this paper we are going to present some experiments which characterize the behaviour of an oscillator RLC in relation to the intensity parameter λ, precisely to λ E(η). The parameter λ is a constant in the exponential distribution of random variables τi, where τi = ti - ti - 1, i = 1, 2, ... are intervals between successive impulses. DOI: 10.12693/APhysPolA.121.A-174PACS numbers: 45.10.-b, 45.30.+s"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8311996,"math_prob":0.8884082,"size":1354,"snap":"2019-26-2019-30","text_gpt3_token_len":323,"char_repetition_ratio":0.08962963,"word_repetition_ratio":0.0,"special_character_ratio":0.22304283,"punctuation_ratio":0.14173229,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98925877,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-07-17T00:28:58Z\",\"WARC-Record-ID\":\"<urn:uuid:c437c2cc-2c7e-4d5a-bcac-829f9fb7f407>\",\"Content-Length\":\"2498\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:1ab2af7e-1f7e-4c8f-8b4f-ba43709a0e56>\",\"WARC-Concurrent-To\":\"<urn:uuid:f2034981-9702-49c4-8244-8bf37a8e6361>\",\"WARC-IP-Address\":\"193.219.28.149\",\"WARC-Target-URI\":\"http://przyrbwn.icm.edu.pl/APP/ABSTR/121/a121-1a-37.html\",\"WARC-Payload-Digest\":\"sha1:3SY5QDG3TZCZK4WGYV2XSDRM4PRTCVYL\",\"WARC-Block-Digest\":\"sha1:5Q4QD3AKZS3L5D5HULLDJIGU2BZVP52U\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-30/CC-MAIN-2019-30_segments_1563195525004.24_warc_CC-MAIN-20190717001433-20190717023433-00431.warc.gz\"}"} |
https://efinancemanagement.com/calculator/cost-of-equity-calculator | [
"data-full-width-responsive=\"true\">\n\n# Cost of Equity (Constant Dividend Growth) Calculator\n\n## Cost of Equity (Constant Dividend Growth)\n\nGordon’s dividend growth model proposes that current market prices are a reflection of the present value of future dividends of a company discounted with an appropriate cost of equity. The model has established a relationship between three variables i.e. Current Market Price, Dividends, and Cost of Equity. Further, there are 3 possible situations for future dividends:\n\n1. Future dividends uncertain or not following any trend\n2. Future dividends having a Constant Growth Rate\n3. Dividends having Phased Growth Situation in future. 5% for 3 Years, then 3% forever.\n\nIn the current post, the calculator will focus 2nd situation i.e. the constant growth rate.\n\n## Formula\n\nThe formula for calculating a cost of equity using the dividend discount model is as follows:\n\nWhere,\n\nKe = D1/P0 + g\n\nKe = Cost of Equity\n\nD1 = Dividend for the Next Year, It can also be represented as ‘D0*(1+g)‘ where D0 is Current Year Dividend.\n\nP0 = present value of a stock.\n\nMost common representation of a dividend discount model is P0 = D1/(Ke-g). This formula is meant for calculating the present value of the stock when the cost of equity is known. The formula mentioned above for calculating the cost of equity (Ke) when the other parameters are known.\n\n## Example\n\nAssume a firm’s share is traded at 300\\$ and the current dividend is \\$8 and a growth rate of 6%. We have the following:\n\nD1 = 8 * (1+6%) = \\$8.48,\n\nP0 = \\$300,\n\ng = 6%\n\nTherefore, Ke = 8.48 / 300 + 6% = 8.83%\n\n## How to Calculate using Calculator?\n\nCost of Equity (Constant Dividend Growth) calculator is easy to calculate the accurate cost of equity. There are 3 basic inputs required for calculating and they are as follows:\n\n1. Current Year Dividend\n2. Constant Growth Rate\n3. Current Market Price\n\n## Interpret Results / Analysis\n\nThe cost of equity calculated using this method has its pros and cons. The calculator calculates the cost of equity with certain assumptions which are not necessarily true all the times. Therefore, this ratio can be used as a reference point. It is advisable to use other tools also along with this.\n\nLast updated on : October 27th, 2018"
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.91854703,"math_prob":0.9946018,"size":2129,"snap":"2019-51-2020-05","text_gpt3_token_len":493,"char_repetition_ratio":0.15435295,"word_repetition_ratio":0.010958904,"special_character_ratio":0.23673086,"punctuation_ratio":0.09774436,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99977714,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-12-13T11:02:43Z\",\"WARC-Record-ID\":\"<urn:uuid:7745953c-afec-4172-8859-a80ce573115f>\",\"Content-Length\":\"132497\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ab6bb91c-179d-473c-9ca6-165e9a11f9ba>\",\"WARC-Concurrent-To\":\"<urn:uuid:bd670700-bafc-4d28-9672-6d7d15f5af67>\",\"WARC-IP-Address\":\"104.27.128.166\",\"WARC-Target-URI\":\"https://efinancemanagement.com/calculator/cost-of-equity-calculator\",\"WARC-Payload-Digest\":\"sha1:U6DK4SYUE754QYZRC7BEN3C4AZZTLCFE\",\"WARC-Block-Digest\":\"sha1:UXMASBTE6TZASIJ4NTTVOEZVPLAHD6SW\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-51/CC-MAIN-2019-51_segments_1575540553486.23_warc_CC-MAIN-20191213094833-20191213122833-00123.warc.gz\"}"} |
https://flypig.co.uk/list?list_id=557&list=blog | [
"# flypig.co.uk\n\n## List items\n\nItems from the current list are shown below.\n\n## Blog\n\n12 Feb 2018 : Countdown #\nI'm not convinced it was good use of my time, but I spent the weekend writing some code to solve the Countdown numbers game. In case you're not familiar with Countdown, here's a clip.\n\nThere are lots of ways to do this, but my solution hinges on being able to enumerate all binary trees with a given number of nodes. Doing this efficiently (both in terms of time and memory) turned out to be tricky, and there's a hinge for this too, based on how the trees are represented. The key is to note that each layer can't have more than n nodes, where n is the number of nodes the tree can have overall.\n\nEach tree is stored as a list, with each item in the list representing the nodes at a given depth in the tree (a layer). Each item is a bit sequence representing which nodes in the layer have children.\n\nThese bit sequences would get long quickly if they represented every possible node in a layer (since there are 2, 4, 8, 16, 32, ... possible nodes at each layer). Instead, the index of the bit represents the index into the actual nodes in the layer, rather than the possible nodes. This greatly limits the length of the bit sequence, because there can no more than n actual nodes in each layer, and there can be no more than n layers in total. The memory requirement is therefore n2.\n\nHere's an example:\n`T = [, [1, 1], [1, 1, 0, 0], [0 ,1, 0, 0]]`\nwhich represents a tree like this:",
null,
"It's really easy to cycle through all of these, because you can just enumerate each layer individually, which involves cyclying through all sequences of binary strings.\n\nIt's not a new problem, but it was a fun exercise to figure out.\n\nThe code is up on GitHub in Python if you want to play around with it yourself."
]
| [
null,
"https://flypig.co.uk/images/blog/tree.png",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.9500511,"math_prob":0.8516437,"size":3245,"snap":"2020-24-2020-29","text_gpt3_token_len":740,"char_repetition_ratio":0.1228016,"word_repetition_ratio":0.85996705,"special_character_ratio":0.23513097,"punctuation_ratio":0.120289855,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9532023,"pos_list":[0,1,2],"im_url_duplicate_count":[null,2,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-06-06T01:17:29Z\",\"WARC-Record-ID\":\"<urn:uuid:9e9b7ccc-bb47-4240-86aa-406e7bff2520>\",\"Content-Length\":\"10675\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:27f6ae73-4d0e-475b-9eee-3f62966a8123>\",\"WARC-Concurrent-To\":\"<urn:uuid:e434e475-4bb1-4989-b768-d1c45d84d659>\",\"WARC-IP-Address\":\"46.32.230.12\",\"WARC-Target-URI\":\"https://flypig.co.uk/list?list_id=557&list=blog\",\"WARC-Payload-Digest\":\"sha1:HKOUAXVDZ5LV5CALKAOKQ3E3BR7BDHBA\",\"WARC-Block-Digest\":\"sha1:WA2K637O7233D7ABZKAPEHXQKURM7SUG\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-24/CC-MAIN-2020-24_segments_1590348509264.96_warc_CC-MAIN-20200606000537-20200606030537-00354.warc.gz\"}"} |
https://answers.everydaycalculation.com/divide-fractions/80-8-divided-by-6-49 | [
"Solutions by everydaycalculation.com\n\n## Divide 80/8 with 6/49\n\n1st number: 10 0/8, 2nd number: 6/49\n\n80/8 ÷ 6/49 is 245/3.\n\n#### Steps for dividing fractions\n\n1. Find the reciprocal of the divisor\nReciprocal of 6/49: 49/6\n2. Now, multiply it with the dividend\nSo, 80/8 ÷ 6/49 = 80/8 × 49/6\n3. = 80 × 49/8 × 6 = 3920/48\n4. After reducing the fraction, the answer is 245/3\n5. In mixed form: 812/3\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":0.7586493,"math_prob":0.9485822,"size":350,"snap":"2019-51-2020-05","text_gpt3_token_len":155,"char_repetition_ratio":0.1618497,"word_repetition_ratio":0.0,"special_character_ratio":0.4857143,"punctuation_ratio":0.09411765,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.95967716,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-01-22T22:45:43Z\",\"WARC-Record-ID\":\"<urn:uuid:d9e45315-ed93-43d3-a12e-fa892025f1af>\",\"Content-Length\":\"7809\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:e188e881-00ea-4660-b84e-253087c55ad1>\",\"WARC-Concurrent-To\":\"<urn:uuid:d6637165-43ba-4cbb-ba9c-9bd8125aea6b>\",\"WARC-IP-Address\":\"96.126.107.130\",\"WARC-Target-URI\":\"https://answers.everydaycalculation.com/divide-fractions/80-8-divided-by-6-49\",\"WARC-Payload-Digest\":\"sha1:ZVPQT3QQNI6TYM565OKG3EQFDZAYEHYX\",\"WARC-Block-Digest\":\"sha1:PZUTYMAJ7MJOE4IFUHATCIXTLQ3V4WNZ\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-05/CC-MAIN-2020-05_segments_1579250607596.34_warc_CC-MAIN-20200122221541-20200123010541-00459.warc.gz\"}"} |
https://godbolt.me/7493a-datasheet-49/ | [
"# 7493A DATASHEET PDF\n\nEach of these monolithic counters contains four master- slave flip-flops and additional gating to provide a divide-by- two counter and a three-stage binary. The datasheet specifies that this counter contains four master-slave flip- flops counter for which the count cycle length is divide-by-eight for the A. DMA datasheet, DMA pdf, DMA data sheet, datasheet, data sheet, pdf, National Semiconductor, 4-Bit Binary Counter.",
null,
"Author: Mazuhn Tudal Country: Panama Language: English (Spanish) Genre: Art Published (Last): 26 January 2014 Pages: 398 PDF File Size: 17.44 Mb ePub File Size: 10.90 Mb ISBN: 329-6-67982-542-9 Downloads: 28415 Price: Free* [*Free Regsitration Required] Uploader: Mezigrel",
null,
"Previous 1 2 A symmetrical divide-by-ten count can be obtained from the ’90A’L9 0or ‘LS90 counters by connecting the Q q output to 749a3 A input and applying the input count to the B input which gives a.\n\nT o use the m axim um count length decade or four-bit binary of these counters, the B input is connected to the output. The input count pulses are applied to CKA input and the outputs are as described in the appropriate function table, A sym metrical divide-by-ten count can be obtained from the ’90A, ‘L90, or ‘LS90 counters by connecting the Qq output to the CKA input and applying the input count to.\n\nLYSEBETH YOGA PDF",
null,
"A symmetrical divide-byten count can be obtained from. No abstract text available Text: The input count pulses are applied to CKA inputcount can be obtained from the ’90A, ‘L90, or ‘LS90 counters by connecting the Qq output to the CKA input datashewt applying the input count to the CKB input which gives a divide-by-ten square waye at output.\n\n### Datasheet PDF – Decade and Binary Counters – TI\n\nS N A. To use their maximum count length decade, divide-by-twelve, or four-bit binary of these counters, the CKB input is connected to the Q a output.",
null,
"The input count pulsessymmetrical divide-byten count can be obtained from the ‘2 9 0 and ‘L S 2 9 0 counters by connecting the Q q. The input count pulsesetrical divide-by-ten count can be obtained from the ’90A or ‘L S 9 0 counters by connecting the Q[ output to the C K A input and applying the input count to the C K B input which gives a divide-byten.\n\nNo file text available.\n\nThe input count pulses are applied to CKA input and the outputs are as 7493 in the appropriate function table. To use their maximum count length decade, divide-by-twelve, or four-bit binary of these counters, the C K B input is connected to the Q a output. The input count pulses are applied to input A and the outputs are as described in the appropriate function table. To use their maximum count length decadecount pulses are applied to input A and the outputs are as described in the appropriate function datashdet.\n\nEL ESNOBISMO LAS GOLONDRINAS PDF\n\n## 74 series digital circuit of 7493A 74L93 4-bit binary counter\n\nThe input count pulses aredivide-by-ten count can datasheeet obtained from the 90Acounters by connecting the QDoutput to the A input and applying the input count to the B input which gives a divide-by-ten square wave at datashete QA. To use th e ir m axim um count lengthdivide-by-ten count can be obtained from the 90A counters by connecting th e Q D output to the A input and applying the input count to the B input w hich gives a divide-by-ten square w ave at output Q A.",
null,
"The input count pulses areoutputs as shown in the Truth Table. To use their maximum count length decade, divide-by-twelve, or four-bit binarythe B input Is connected to the Qa output."
]
| [
null,
"http://www.seekic.com/uploadfile/ic-circuit/201172914014676.gif",
null,
"https://godbolt.me/download_pdf.png",
null,
"http://www.datasheetq.com/contents-image1/TI/74LS90-DI1.gif",
null,
"http://www.seekic.com/uploadfile/ic-circuit/20113311493160.gif",
null,
"https://images.alldatasheet.com/semiconductor/electronic_parts/datasheet/8321/NSC/7493.GIF",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.80537164,"math_prob":0.7561153,"size":3490,"snap":"2021-21-2021-25","text_gpt3_token_len":870,"char_repetition_ratio":0.19707401,"word_repetition_ratio":0.36195287,"special_character_ratio":0.23925501,"punctuation_ratio":0.081779055,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98719007,"pos_list":[0,1,2,3,4,5,6,7,8,9,10],"im_url_duplicate_count":[null,7,null,null,null,8,null,8,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2021-06-16T17:31:56Z\",\"WARC-Record-ID\":\"<urn:uuid:c5f852f2-7c6b-4892-8dc4-a109f222b531>\",\"Content-Length\":\"82061\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:ec41f270-d542-4116-980d-ef5add55a1e4>\",\"WARC-Concurrent-To\":\"<urn:uuid:f668bd15-a10f-4a73-aff4-916fd9a28a47>\",\"WARC-IP-Address\":\"172.67.204.27\",\"WARC-Target-URI\":\"https://godbolt.me/7493a-datasheet-49/\",\"WARC-Payload-Digest\":\"sha1:DFXKUAIJXPX2KWJP5ZO4ATNIKQJROJ4Z\",\"WARC-Block-Digest\":\"sha1:DMQAQCCJWVJCVWUJ7BUCSUBON2AGBCGF\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2021/CC-MAIN-2021-25/CC-MAIN-2021-25_segments_1623487625967.33_warc_CC-MAIN-20210616155529-20210616185529-00453.warc.gz\"}"} |
https://coffeerelax.co/na-atomic-radius/ | [
"### Learning Objectives\n\n• Describe how the atomic changes within a period.\n• Describe how the atomic radius changes within a group.",
null,
"### How can all of these people fit in such a small space?\n\nAtomic radius 1 increases down a Group, from top to bottom, of the Periodic Table. Atomic radius decreases across a Period, from left to right, of the Periodic Table 2. Note trends for ionic radii: ionic radius of a cation is less than atomic radius of the atom. The standard atomic weight is a special value of the relative atomic mass. It is defined as the 'recommended values' of relative atomic masses of sources in the local environment of the Earth's crust and atmosphere as determined by the IUPAC Commission on Atomic Weights and Isotopic Abundances (CIAAW). The Van der Waals radius, r w, of an atom is the radius of an imaginary hard sphere representing the distance of closest approach for another atom. It is named after Johannes Diderik van der Waals, winner of the 1910 Nobel Prize in Physics, as he was the first to recognise that atoms were not simply points and to demonstrate the physical consequences of their size through the Van der Waals.\n\nEvents draw large numbers of people to them. Even an outdoor event can fill up so that there is no room for more people. The crowd capacity depends on the amount of space in the venue, and the amount of space depends on the size of the objects filling it. We can get more people into a given space than we can elephants, because the elephants are larger than people. We can get more squirrels into that same space than we can people for the same reason. Knowing the sizes of objects we are dealing with can be important in deciding how much space is needed.\n\nThe size of atoms is important when trying to explain the behavior of atoms or compounds. One of the ways we can express the size of atoms is with the atomic radius . This data helps us understand why some molecules fit together and why other molecules have parts that get too crowded under certain conditions.\n\nThe standard atomic weight is a special value of the relative atomic mass. It is defined as the 'recommended values' of relative atomic masses of sources in the local environment of the Earth's crust and atmosphere as determined by the IUPAC Commission on Atomic Weights and Isotopic Abundances (CIAAW). Linus Carl Pauling (/ ˈ p ɔː l ɪ ŋ /; February 28, 1901 – August 19, 1994) was an American chemist, biochemist, chemical engineer, peace activist, author, and educator.He published more than 1,200 papers and books, of which about 850 dealt with scientific topics.",
null,
"The size of an atom is defined by the edge of its orbital. However, orbital boundaries are fuzzy and in fact are variable under different conditions. In order to standardize the measurement of atomic radii, the distance between the nuclei of two identical atoms bonded together is measured. The atomic radius is defined as one-half the distance between the nuclei of identical atoms that are bonded together.\n\nFigure 1. The atomic radius (r) of an atom can be defined as one half the distance (d) between two nuclei in a diatomic molecule.\n\nAtomic radii have been measured for elements. The units for atomic radii are picometers, equal to 10−12 meters. As an example, the internuclear distance between the two hydrogen atoms in an H2 molecule is measured to be 74 pm. Therefore, the atomic radius of a hydrogen atom is [latex]frac{74}{2}=37text{ pm}[/latex].",
null,
"Figure 2. Atomic radii of the representative elements measured in picometers.\n\n## Periodic Trend\n\nThe atomic radius of atoms generally decreases from left to right across a period. There are some small exceptions, such as the oxygen radius being slightly greater than the nitrogen radius. Within a period, protons are added to the nucleus as electrons are being added to the same principal energy level. These electrons are gradually pulled closer to the nucleus because of its increased positive charge. Since the force of attraction between nuclei and electrons increases, the size of the atoms decreases. The effect lessens as one moves further to the right in a period because of electron-electron repulsions that would otherwise cause the atom’s size to increase.",
null,
"## Group Trend\n\nThe atomic radius of atoms generally increases from top to bottom within a group. As the atomic number increases down a group, there is again an increase in the positive nuclear charge. However, there is also an increase in the number of occupied principle energy levels. Higher principal energy levels consist of orbitals which are larger in size than the orbitals from lower energy levels. The effect of the greater number of principal energy levels outweighs the increase in nuclear charge and so atomic radius increases down a group.\n\nFigure 3. A graph of atomic radius plotted versus atomic number. Each successive period is shown in a different color. As the atomic number increases within a period, the atomic radius decreases.\n\n### Summary\n\n• Atomic radius is determined as the distance between the nuclei of two identical atoms bonded together.\n• The atomic radius of atoms generally decreases from left to right across a period.\n• The atomic radius of atoms generally increases from top to bottom within a group.\n\n### Practice\n\n1. What influences the atomic size of an atom?\n2. What is a covalent radius?\n3. What is an ionic radius?\n\n### Review",
null,
"2. What are the units for measurement of atomic radius?\n3. How does the atomic radius change across a period?\n4. How does atomic radius change from top to bottom within a group?\n5. Explain why the atomic radius of hydrogen is so much smaller that the atomic radius for potassium.\n\n## Glossary\n\n• atomic radius: The atomic radius is defined as one-half the distance between the nuclei of identical atoms that are bonded together.\nShow References\n\n## References\n\n1. James Cridland. Crowd .\n2. CK-12 Foundation – Christopher Auyeung. . CC-BY-NC-SA 3.0\n3. CK-12 Foundation – Christopher Auyeung. . CC-BY-NC-SA 3.0\n4. CK-12 Foundation – Christopher Auyeung. . CC-BY-NC-SA 3.0\n\nA warning!\n\nIonic radii are difficult to measure with any degree of certainty, and vary according to the environment of the ion. For example, it matters what the co-ordination of the ion is (how many oppositely charged ions are touching it), and what those ions are.\n\nThere are several different measures of ionic radii in use, and these all differ from each other by varying amounts. It means that if you are going to make reliable comparisons using ionic radii, they have to come from the same source.\n\nWhat you have to remember is that there are quite big uncertainties in the use of ionic radii, and that trying to explain things in fine detail is made difficult by those uncertainties. What follows will be adequate for UK A level (and its various equivalents), but detailed explanations are too complicated for this level.\n\nTrends in ionic radius in the Periodic Table\n\nTrends in ionic radius down a group\n\n## Atomic Radius Na To Cl\n\nThis is the easy bit! As you add extra layers of electrons as you go down a group, the ions are bound to get bigger. The two tables below show this effect in Groups 1 and 7."
]
| [
null,
"https://useruploads.socratic.org/PDxdL8CzQAq7cigv9JkB_f07b1af3eb2bc0e5cffb096bdfa3c5dd.jpg",
null,
"https://slideplayer.com/slide/15070753/91/images/4/Atomic+Radius+H+Li+Na+K+Rb.jpg",
null,
"https://i.ytimg.com/vi/4Url0pjbcuU/maxresdefault.jpg",
null,
"https://people.uwplatt.edu/~sundin/114/image/L1425f.gif",
null,
"https://upload.wikimedia.org/wikipedia/commons/thumb/d/d1/Atomic_%26_ionic_radii_de.svg/1200px-Atomic_%26_ionic_radii_de.svg.png",
null
]
| {"ft_lang_label":"__label__en","ft_lang_prob":0.91743153,"math_prob":0.9344266,"size":7245,"snap":"2022-05-2022-21","text_gpt3_token_len":1561,"char_repetition_ratio":0.156332,"word_repetition_ratio":0.16318329,"special_character_ratio":0.20814355,"punctuation_ratio":0.09190372,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9515977,"pos_list":[0,1,2,3,4,5,6,7,8,9,10],"im_url_duplicate_count":[null,1,null,1,null,1,null,1,null,1,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2022-05-20T11:44:55Z\",\"WARC-Record-ID\":\"<urn:uuid:548038e1-afb5-4688-88e1-03612ce30aee>\",\"Content-Length\":\"14850\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:7a66d829-7141-40f0-afd5-9393b9a96c7c>\",\"WARC-Concurrent-To\":\"<urn:uuid:c9109769-98ce-4df8-bc24-19a5055d8cef>\",\"WARC-IP-Address\":\"104.21.82.170\",\"WARC-Target-URI\":\"https://coffeerelax.co/na-atomic-radius/\",\"WARC-Payload-Digest\":\"sha1:O6LRRO4WGDFSA2ZS4CLGSNYM6MKIPGC6\",\"WARC-Block-Digest\":\"sha1:JVGEFZJLLM7QMW3JONQZ6TI46GSSPYUU\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2022/CC-MAIN-2022-21/CC-MAIN-2022-21_segments_1652662531779.10_warc_CC-MAIN-20220520093441-20220520123441-00460.warc.gz\"}"} |
https://trstringer.com/complete-binary-tree/ | [
"Complete Binary Tree\nPost\nCancel\n\n# Complete Binary Tree\n\nA complete binary tree is a really interesting data structure. It is the starting point of a heap sort and in this blog post I want to illustrate what a complete binary tree is and the properties of it that provide its usefulness.\n\nBy definition, a complete binary tree is a data structure where each node has at most two child nodes. Specifically, the tree is designed so that nodes are filled in from top left to bottom right. Put another way, all nodes are as far top and left as they can be. Let’s say you have an array of numbers: [4, 1, 7, 8, 2, 3, 5, 6, 0, 9]. This can be constructed as a complete binary tree by filling all the nodes in from top to bottom, left to right:",
null,
"What makes a complete binary tree important though, and mathematically what properties can we derive from it?\n\nThe level capacity of a complete binary tree can be defined as 2level_index. For example, the root level (level 0) of the binary tree can contain only a single element: 20 = 1. The level with index of 2 can contain 4 elements: 22 = 4. It’s worth noting that the final level of a complete binary tree may not (and usually is not) be completely full. In the above example, the final level (level index 3) has the capacity for 8 nodes (23 = 8), but only contains 3 nodes. This is completely normal. But it is also worth noting that one of the properties of a complete binary tree is that only the last level can be an incomplete level. All preceding levels must be full.\n\nThe child element indexes can be found:\n\n• Left child node index - 2 x parent_index + 1\n• Right child node index - 2 x parent_index + 2\n\nFor instance, to get the child nodes of the node with 8 as its value and 3 as its index, the left child node index would be 2 x 3 + 1, which is index 7 (node value is 6). The right child node index is 2 x 3 + 2, which is index 8 (node value is 0).\n\nThe parent node index can be calculated by floor((index - 1) / 2). Example: to find the parent node of the element with index 5 (value 3), you would calculate that with floor((5 - 1) / 2) = 2. So that node’s parent has an index of 2 (value is 7).\n\nHopefully this blog post introduced you to what a complete binary tree is, how to construct one, and its mathematical properties that make it a viable data structure for many uses!"
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"https://trstringer.com/images/complete-binary-tree3.png",
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https://yahootechpulse.easychair.org/publications/preprint/H5PS | [
"",
null,
"A Closed-Form Solution of Drop Test on an Elastic Bar: Benchmarking Force Response of the Restrained Bar to Impact\n\nEasyChair Preprint no. 5868\n\n12 pagesDate: June 23, 2021\n\nAbstract\n\nThe behaviour of an elastic bar; restrained at one end and subjected to a rigid impactor at the other end is evaluated in this analytical work. In the original work on this problem, duration of impact is only considered up to four-times of the time taken by compressive stress wave to travel from end struck to the bottom support and back. The current work revisits the closed-form solution provided in the literature in terms of the set of first four compressive stresses, then formulates these terms in programming language. The code is then utilised to derive arbitrary number of higher-order stress intervals depending on mass ratio of the system to complete the whole impact process. Compressive stress at the end struck and its corresponding load are then formulated for each stress interval by the current and previous compressive stress formula; a process which provides force history at the end struck for the whole impact duration. Parametric study is then performed on the number of selected input parameters in the stress equations e.g. mass ratio, drop height (or initial velocity), elastic modulus and length of the elastic bar; revealing proportional relations to apparent output variables obtained from force history, namely number of intervals, initial compressive stress, pulse width, peak load and interval frequency. These proportionalities and their corresponding mathematical relations are useful in explaining and correlating respective output variable-parameter relationships obtained via experimental or numerical works. The closed-form solution provided in this work serves as a benchmark to numerical or experimental impact problems assuming homogeneous and isotropic bar behaving linear elastically.\n\nKeyphrases: Elastic bar, Force at end struck, impact, Mathematical relations, Stress intervals"
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"https://yahootechpulse.easychair.org/images/books.png",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.8694591,"math_prob":0.91334355,"size":2067,"snap":"2023-14-2023-23","text_gpt3_token_len":385,"char_repetition_ratio":0.110518664,"word_repetition_ratio":0.0,"special_character_ratio":0.17464925,"punctuation_ratio":0.0862069,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.98444015,"pos_list":[0,1,2],"im_url_duplicate_count":[null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2023-06-03T00:36:12Z\",\"WARC-Record-ID\":\"<urn:uuid:fa4a2b34-a653-4aee-81a7-d6c936eeb979>\",\"Content-Length\":\"6995\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:d15aa0b6-863c-465e-8e14-aa4b36d70992>\",\"WARC-Concurrent-To\":\"<urn:uuid:00d47fc2-258d-45fd-bbe5-a698a06a5e99>\",\"WARC-IP-Address\":\"213.136.76.235\",\"WARC-Target-URI\":\"https://yahootechpulse.easychair.org/publications/preprint/H5PS\",\"WARC-Payload-Digest\":\"sha1:BTRC4WHIVF3J7YXCXODD6K4A74A25VUH\",\"WARC-Block-Digest\":\"sha1:AOMBDVCZG6Q3VEDTAIH7UX22VKBEKVXT\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2023/CC-MAIN-2023-23/CC-MAIN-2023-23_segments_1685224648911.0_warc_CC-MAIN-20230603000901-20230603030901-00606.warc.gz\"}"} |
https://www.physicsforums.com/threads/wish-to-get-singular-points-of-algebraic-functions.552913/ | [
"# Wish to get singular points of algebraic functions\n\nIs there a numeric method to find singular points for managable algebraic functions? I have:\n\n$$w^2+2z^2w+z^4+z^2w^2+zw^3+1/4w^4+z^4w+z^3w^2-1/2 zw^4-1/2 w^5=0$$\n\nand I wish to find the singular points for the function w(z). I can find them for simpler functions like\n$$w^3+2w^2z+z^2=0$$\nIn this case, I differentiate implicitly to get\n$$w'=-\\frac{2(z+w^2)}{w(4z+3w)}$$\nso that the function w(z) is singular when that denominator is zero so I set it to zero and solve for w so w=0 or $w=-4/3 z$\nI can then substitute those values of w into the original equation and find it's zeros (numerically) in terms of z.\n\nI can use this method in Mathematica to compute singular points for even more complicated ones than this simple one, even one of degree four. However, when I get to one like I have above, that's too difficult for Mathematica to handle and it seems it can't even numerically and I just run into CPU-overload after a minute or so.\n\nWould someone know if there is a better method to find these numerically?\n\nThanks,\nJack\n\nLast edited:\n\n## Answers and Replies\n\nHallsofIvy\nScience Advisor\nHomework Helper\nIs there a numeric method to find singular points for managable algebraic functions? I have:\n\n$$w^2+2z^2w+z^4+z^2w^2+zw^3+1/4w^4+z^4w+z^3w^2-1/2 zw^4-1/2 w^5=0$$\n\nand I wish to find the singular points for the function w(z). I can find them for simpler functions like\n$$w^3+2w^2z+z^2=0$$\nIn this case, I differentiate implicitly to get\n$$w'=-\\frac{2(z+w^2)}{w(4z+3w)}$$\nso that the function w(z) is singular when that denominator is zero so I set it to zero and solve for w so w=0 or $w=-4/3 z$\nI can then substitute those values of w into the original equation and find it's zeros (numerically) in terms of z.\n\nI can use this method in Mathematica to compute singular points for even more complicated ones than this simple one, even one of degree four. However, when I get to one like I have above, that's too difficult for Mathematica to handle and it seems it can't even numerically and I just run into CPU-overload after a minute or so.\n\nWould someone know if there is a better method to find these numerically?\n\nThanks,\nJack\nSame idea, really, differentiate both sides of\n$$w^2+2z^2w+z^4+z^2w^2+zw^3+1/4w^4+z^4w+z^3w^2-1/2 zw^4-1/2 w^5=0$$\nto get\n$$2w w'+ 4zw+ 2z^2w'+ 4z^2+ 2zw^2+ 4z^2ww'+ w^3+ 3zw^2w'+ 4z^3w+ z^4w'+ 3z^2w^2+ 2z^3ww'- (1/2)w^4- 2zw^3w'- (5/2)w^4w'= 0$$\n\nCombine all terms involving w' on the left, all others on the right:\n$$(2w+ 2z^2+ 4z^2w+ 4z^2ww'+ 3zw^3w'+ z^4+ 3z^3w+ 2zw^4- (5/2)w^4)w'= -4zw- 4z^2- 2zw^2- w^3- 4z^3w+ 3z^2w^2- (1/2)w^4$$\n\nand solve for w'.\n\nBut when I solve for w'[z] (excuse the mathematica latex):\n\n$$\\left.\\left\\{w'[z]\\to \\frac{-8 z^3-8 z w[z]-8 z^3 w[z]-4 z w[z]^2-6 z^2 w[z]^2-2 w[z]^3+w[z]^4}{4 z^2+2 z^4+4 w[z]+4 z^2 w[z]+4 z^3 w[z]+6 z w[z]^2+2 w[z]^3-4 z w[z]^3-5 w[z]^4}\\right\\}\\right\\}$$\n\nI would then have to set the denonimator to zero and solve for w, which is a quartic, and then substitute that solution into the original equation which would be 9 degrees in w but z is four degrees so I assume that would be 36 solutions. Which would be fine with me if I could get them numerically but Mathematica seems to stall-out with that. Guess I could let it run longer to see if something happens.\n\nI was just wondering if there was any other way to obtain the singular pointis."
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https://ask.sagemath.org/question/9597/solve-contains-wrong-solution/ | [
"# Solve contains wrong solution\n\nHello, I tried to following to find a maxima of a function:\n\nvar('t x');\nf=(e^(x*t))*(x-1)^2;\nmaxima = solve([derivative(f,x)==0, derivative(f,x,2)<0],x)\nshow(maxima);\n\n\nAnd the solution sage spits out are:\n\n[\n[x == 1, -2 > 0],\n[x == (t - 2)/t, -(t - 2)^2 + 2*(t - 2)*t - t^2 + 6 > 0]\n]\n\n\nI understand that sage cannot evaluate the validity of the second solution but the first one surely is no solution at all.\n\nWhy does it give me this solution or am I doing anything wrong?\n\nedit retag close merge delete\n\nI know, that I could only solve for f'(x)==0 and filter for f''(x)<0 but solve shouldn't contain solutions like that, I think.\n\nSort by » oldest newest most voted\n\nThis is a bug (?) in to_poly_solve in Maxima.\n\n(%i1) load(to_poly_solver);\n\nLoading maxima-grobner $Revision: 1.6$ $Date: 2009-06-02 07:49:49$\n(%o1) /Applications/MathApps/Sage-5.4.1-OSX-64bit-10.6.app/Contents/Resources/\\\nsage/local/share/maxima/5.26.0/share/contrib/to_poly_solver.mac\n(%i3) display2d:false;\n\n(%o3) false\n(%i4) to_poly_solve([2*(x-1)*%e^(t*x)+t*(x-1)^2*%e^(t*x)=0,4*t*(x-1)*%e^(t*x)+t^2*(x-1)^2*%e^(t*x)+2*%e^(t*x)>0],[x]);\n\n(%o4) %union([x = 1,2 > 0],[x = (t-2)/t,\nt^2-2*(t-2)*t-4*t+4*(t-2)+(t-2)^2+2 > 0])\n\n\nThe current Maxima has\n\n(%o4) %union([x = 1,2 > 0],[x = (t-2)/t,\nt^2-2*(t-2)*t-4*t+4*(t-2)+(t-2)^2+2 > 0])\n\n\nwhich is basically the same issue. I've reported this upstream here.\n\nmore\n\nI beg to differ :\n\nMaxima 5.28.0 http://maxima.sourceforge.net using Lisp GNU Common Lisp (GCL) GCL 2.6.7 (a.k.a. GCL) Distributed under the GNU Public License. See the file COPYING. Dedicated to the memory of William Schelter. The function bug_report() provides bug reporting information. (%i1) load(to_poly_solve);\n\nLoading maxima-grobner $Revision: 1.6$ $Date: 2009-06-02 07:49:49$\n\n(%o1) /usr/share/maxima/5.28.0/share/to_poly_solve/to_poly_solve.mac\n\n(%i2) display2d:false;\n\n(%o2) false\n\n(%i3) f(x,t):=(%e^(xt))(x-1)^2;\n\n(%o3) f(x,t):=%e^(xt)(x-1)^2\n\n(%i4) map(factor,%solve([factor(diff(f(x,t),x))=0,factor(diff(diff(f(x,t),x),x))<0],x));\n\n(%o4) %union([x = 1,-2 > 0],[x = (t-2)/t,2 > 0])\n\nwhich is correct.\n\nNote that I load()ed to poly solve, not to_poly_solver ; according to a comment in the former source, the latter is obsolete.\n\nHTH,\n\n Emmanuel Charpentier\n\nmore\n\nI would not agree with you that these solutions are 'wrong'. They are just presented in a very user unfriendly way. The 1st one, i.e.:\n\n[x == 1, -2 > 0]\n\n\ndefinitely is a solution - it just specifies a range of measure zero, since\n\nsage: -2>0\nFalse\n\n\nso, it is not 'wrong' as you state - it is just 'totally useless' ;) The other solution is also perfectly ok since\n\nsage: bool(-(t - 2)^2 + 2*(t - 2)*t - t^2 + 6)\nTrue\n\n\nso, the solution you want is\n\nx == (t - 2)/t\n\n\nwhich I think is ok ..... however I would definetely agree with you that\n\nIn:= f[x_, t_] = Exp[x t] (x - 1)^2;\nIn:= Solve[{D[f[x, t], x] == 0 , D[f[x, t], {x, 2}] < 0, {x, t}]\nOut= {{t -> ConditionalExpression[-(2/(-1 + x)), (t | x) \\[Element] Reals]}}\n\n\nfrom a well known competitor is far more user friendly\n\nmore"
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https://www.jiskha.com/questions/359849/need-help-with-2-3-1-record-the-pairs-of-data-for-pressure-atm-and-volume-ml | [
"# Chemistry\n\nNeed help with #2 & # 3\n\n1. Record the pairs of data for pressure (atm) and volume (mL).\n\nPressure(atm) Volume(mL)\n1.000 150 mL\n1.154 130 mL\n1.364 110 mL\n1.667 90 mL\n\n2. Does your experimental data verify Boyle's Law? Explain.\n\n3. What pressure would the gas sample have at a volume of 75 mL? At 300 mL?\n\n1. 👍\n2. 👎\n3. 👁\n1. The gas was propane\n\n1. 👍\n2. 👎\n2. #2. Looks like verification to me.\nPV = k. Multiply P x V and see what you get for the first one, then compare with the other PV = ??\n\n#3. Just use PV = k from the previous data, that same k and 75 mL should give the new pressure.\n\n1. 👍\n2. 👎\n\n## Similar Questions\n\n1. ### chem.\n\nA sample of argon at 300. °C and 50.0 atm pressure is cooled in the same container to a temperature of 0. °C. What is the new pressure? 105 atm 45.5 atm 54.9 atm 23.8 atm 42.7 atm\n\n2. ### Chemistry\n\nA 0.65 mole quantity of O2 occupies 4.0 L at 20.◦C. What is the final pressure exerted by the gas? 1. 0.92 atm 2. 3.9 atm 3. 6.2 atm 4. 1.1 atm 5. 0.27 atm — Initially, I got .27 atm. I got this answer by plugging in the\n\n3. ### Chemistry\n\nSulfur dioxide is used to make sulfuric acid. one method of producing it is by roasting mineral sulfides, for example, FeS2(s) + O2 (g) ---> SO2(g) + Fe2O3(s) (unbalanced). A production error leads to the sulfide being placed in a\n\n4. ### Chemistry\n\nA snorkeler takes a syringe filled with 16 mL of air from the surface, where the pressure is 1.0 ATM, to an unknown depth. The volume of the air in the syringe at this depth is 7.5 mL. What Is the pressure at this depth? If the\n\n1. ### physics\n\nAn unknown liquid fills a square container of sides 10 m. What is the density of a material if the pressure 5 m below the surface is 1.6 atm? Assume g=10 m/s^2 and the pressure at the surface of the liquid is 1 atm. Also assume\n\n2. ### chemistry\n\n1) A gas has a pressure of 3 atm when the temperature is 25C, what is the new pressure when the temperature is raised to 50C? (make sure temp is in K) - round answer to hundredths place 2) Neon at 2 atm and 273K has a volume of\n\n3. ### physical chemistry\n\n2 liters of N2 at 0 degree Celsius and 5 atm pressure are expanded isothermally against a constant pressure of 1 atm until the pressure of the gas is also 1 atm. Assuming the gas to be ideal, what are the values of work,delta E,\n\n4. ### Chem\n\nWould you please tell me if these are right? A sample of helium has a volume of 325 ml and a pressure of 655 mm hg. What will be the pressure if the helium is compressed to 125 ml (t and n are constant) I got 1703 mm of Hg A 75.0\n\n1. ### Chemistry\n\nAt 900.0K, the equilibrium comstant (kp) for the following reaction is 0.345 2SO2 (g) + O2 (g) yields 2SO3 (g) At equilibrium the partial pressure of SO2 is 35.0 atm and that of O2 is 15.9 atm. What is the partial pressure of SO3\n\n2. ### Chemistry 3A\n\na sample of nitrogen gas, N2 occupies 3.0L at a pressure of 3.0 atm. what volume will it occupy when the pressure is changed to 0.50 atm and the temperature remains constant?\n\n3. ### chemistry\n\nThe local weather forecaster reports that the current barometric pressure is 29.5 inches of mercury. What is the current pressure in atmospheres? 9.99 atm 3.93 atm 0.986 atm 883 atm 1.00 atm\n\n4. ### chem\n\nat a depth of 100m underwater the water pressure is equal to 10 atm of pressure. what is the partial pressure of N2 at a pressure of 10 atm?"
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https://ryanwingate.com/assets/5/stroop.html | [
"# Analyzing the Stroop Effect¶\n\nBy: Ryan Wingate\nCompleted: February 20, 2018\n\n## Introduction¶\n\nThe Stroop effect is a psychological phenomenon that impacts the reaction time required for certain cognitive tasks. The most common manifestation of the effect occurs during the performance of a \"Stroop test,\" during which participants are asked to name the font color a list of colors are printed in.\n\nThere are two types of lists the participants read from. \"Congruent\" lists are those where the written color and the font color are the same. \"Incongruent\" lists are those where the written color is different from the font color.\n\nCongruent:\n\nBlue Red Green Red Blue Blue Green\n\nIncongruent:\n\nBlue Red Green Red Blue Blue Green\n\nThe idea is that it takes participants significantly longer to state the color each word is written in for the incongruent list than for the congruent list.\n\n## Identification of Variables¶\n\nIndependent variable: which list is shown to the participant.\n\nDependent variable: the amount of time it takes the participant to name the ink colors for each list.\n\n## Select Statistical Test¶\n\nSince the goal of this anlysis is to infer something about the population from limited samples, the hypothesis will be written in terms of the population mean, $\\mu$.\n\nThe appropriate statistical test to perform is the \"Dependent Samples T Test.\" This test is also known as the \"Paired Samples T Test.\" This is the appropriate test because the data involve two measurements performed on the same person under different conditions, and contains no information about the population.\n\n## Establish Hypotheses¶\n\nSince the goal is to prove the presence of the stroop effect, the appropriate structure for the set of hypotheses is to make the implicit assumption that the stroop effect does not exist.\n\nThat is, the alternative hypothesis is that the mean difference between the time required to read the incongruent and congruent lists is greater than zero. Then, the null hypothesis (initially assumed to be correct) is that the mean difference between the time required to read the incongruent and congruent lists is zero.\n\nRecall that congruent means the ink color is the same as the written color, whereas incongruent means the ink color is different from the written color.\n\nWritten algebraically, the foregoing becomes the following...\n\n$$H_0: \\mu_{diff} = 0$$ $$H_A: \\mu_{diff}> 0$$\n\nwhere, $\\mu_{diff}$ is defined as the average of the pairwise differences, $x_{diff}$:\n\n$$x_{diff} = x_{incongruent}-x_{congruent}$$\n\nThe fact that the samples are dependent is why also why the hypotheses are written in terms of the mean of differences, rather than the difference of means, although those approaches are only subtely different. Rarely would they produce different results.\n\n## Calculate Descriptive Statistics to Build Intuition¶\n\nIn :\nimport pandas as pd\nimport matplotlib.pyplot as plt\nfrom scipy import stats\n%matplotlib inline\n\ndf.shape\n\nOut:\n(24, 2)\n\n24 participants completed the study.\n\nIn :\ndf['difference'] = df['Incongruent'] - df['Congruent']\n\nOut:\nCongruent Incongruent difference\n0 12.079 19.278 7.199\n1 16.791 18.741 1.950\n2 9.564 21.214 11.650\n3 8.630 15.687 7.057\n4 14.669 22.803 8.134\nIn :\ncong_mean = df.Congruent.mean()\ncong_std = df.Congruent.std()\nincong_mean = df.Incongruent.mean()\nincong_std = df.Incongruent.std()\ndiff_mean = df.difference.mean()\ndiff_std = df.difference.std()\ndiff_min = df.difference.min()\n\nprint(' Congruent data - mean : {:.1f}'.format(cong_mean))\nprint(' Congruent data - std dev : {:.1f}'.format(cong_std))\nprint('\\r')\nprint('Incongruent data - mean : {:.1f}'.format(incong_mean))\nprint('Incongruent data - std dev : {:.1f}'.format(incong_std))\nprint('\\r')\nprint(' Difference data - mean : {:.1f}'.format(diff_mean))\nprint(' Difference data - std dev : {:.1f}'.format(diff_std))\nprint('\\r')\nprint(' Difference data - min : {:.1f}'.format(diff_min))\n\n Congruent data - mean : 14.1\nCongruent data - std dev : 3.6\n\nIncongruent data - mean : 22.0\nIncongruent data - std dev : 4.8\n\nDifference data - mean : 8.0\nDifference data - std dev : 4.9\n\nDifference data - min : 1.9\n\n\nThe descriptive statistics above imply that the null will be rejected, for two reasons:\n\n1. A positive mean difference, with magnitude of nearly twice the standard deviation.\n2. There are no negative values in the difference data, as evidenced by the minimum value.\n\n## Visualize the Data¶\n\nIn :\ndef print_hists():\nfig, axs = plt.subplots(1, 3, figsize=(16,4))\nbins = range(0,35,5)\ncolors = ['lightblue', 'pink', 'lightgreen']\nmeans = [cong_mean, incong_mean, diff_mean]\n\naxs.hist(df.Congruent, label='Congruent',\ncolor=colors, bins=bins);\n\naxs.hist(df.Incongruent, label='Incongruent',\ncolor=colors, bins=bins);\n\naxs.hist(df.difference, label='Difference',\ncolor=colors, bins=bins);\n\nfor i, ax in enumerate(axs):\nax.axvline(means[i], color='black');\nax.legend();\n\nfor label in ['top', 'bottom', 'right', 'left']:\nax.spines[label].set_visible(False)\n\nIn :\ndef print_boxplots():\nfig, ax = plt.subplots(1, 1, figsize=(16,6))\ncolors = ['lightblue', 'pink', 'lightgreen']\n\nbp = ax.boxplot([df.Congruent, df.Incongruent, df.difference],\nlabels = ['Congruent', 'Incongruent', 'Difference'],\npatch_artist = True);\n\nfor label in ['top', 'right', 'left']:\nax.spines[label].set_visible(False)\n\nfor i, box in enumerate(bp['boxes']):\nbox.set(color = colors[i], linewidth = 3)\n\nfor i, whisker in enumerate(bp['whiskers']):\nwhisker.set(color = colors[i//2], linewidth = 3)\n\nfor i, cap in enumerate(bp['caps']):\ncap.set(color = colors[i//2], linewidth = 3)\n\nfor i, flier in enumerate(bp['caps']):\nflier.set(color = colors[i//2], linewidth = 3)\n\nIn :\nprint_hists()",
null,
"The three histograms above are plotted on a common x-axis. The values of the incongruent data appear to be generally higher than the congruent data.\n\nIn :\nprint_boxplots()",
null,
"The box plots, above, provide another way to visualize the information in the histograms. Both types of plots appear to provide further indication of the presence of the Stroop effect. The null hypothesis is expected to be rejected based on the distributions of the data shown above.\n\n## Perform the Statistical Test¶\n\nTo perform the statistical test, I calculate the \"p-value,\" which is the strength of evidence in support of the null hypothesis.\n\nAs a standard of comparison for the p-value, I adopt the standard $\\alpha$, or \"Significance Level,\" of 0.05. This is the probability of rejecting the null hypothesis when it is actually true. To arrive at a p value for this set of data, I calculate the t-statistic, which in turn requires the standard error:\n\n$$SE = \\frac{\\sigma}{n^\\frac{1}{2}}$$\n\nwhere $\\sigma$ is the standard deviation of the sample, and $n$ is the number of samples.\n\nThe t-statistic is calculated as:\n\n$$t_{stat} = \\frac{\\mu_{diff}}{SE}$$\n\nwhere $\\mu_{diff}$ is the standard deviation of the differences between the congruent and incongruent test durations for each participant.\n\nFinally, the p-value is calculated using the Cumulative Distribution Function, which requires as inputs the $t_{stat}$ and degrees of freedom. The degrees of freedom are calculated as $n-1$, where $n$, as above, is the number of samples.\n\n$$p_{value} = 1-CDF(t_{stat}, n-1)$$\n\nIn :\ndiff_standard_error = diff_std / (df.shape**0.5)\nt_stat = diff_mean / diff_standard_error\np_value = 1-stats.t.cdf(t_stat, df.shape-1)\n\nprint('Difference standard error = {:.3f}'.format(diff_standard_error))\nprint(' T-stat for test data = {:.2f}'.format(t_stat))\nprint(' P-value for given t-stat = {:.9f}'.format(p_value))\n\nDifference standard error = 0.993\nT-stat for test data = 8.02\nP-value for given t-stat = 0.000000021\n\n\nThe p-value, shown above, is the probability of rejecting the null hypothesis when it is actually true. Another value, called the \"Confidence Level,\" is 1 minus $\\alpha$, expressed as a percentage. For a significance level of 0.05, the confidence level is 95%.\n\nThe T-stat for our test data is 8.02, which, for 23 degrees of freedom, corresponds to a P-value much less than 0.05. Since the P-value is less than the significance level, I reject the null hypothesis. The conclusion is that the alternative hypothesis is true, and that the Stroop effect has had a statistically-significant impact.\n\nHaving taken this particular test myself before, I am not surprised by the results. Even with significant concentration it is difficult to quickly say the ink color a word is written in when that word itself spells out a color."
]
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null,
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https://cmsa.fas.harvard.edu/event/10-12-2021-combinatorics-physics-and-probability-seminar/ | [
"# 10/12/2021 Combinatorics, Physics and Probability Seminar\n\n10/12/2021 9:00 am - 10:00 am\n\nTitle: On counting algebraically defined graphs\n\nAbstract: For many classes of graphs that arise naturally in discrete geometry (for example intersection graphs of segments or disks in the plane), the edges of these graphs can be defined algebraically using the signs of a finite list of fixed polynomials. We investigate the number of n-vertex graphs in such an algebraically defined class of graphs. Warren’s theorem (a variant of a theorem of Milnor and Thom) implies upper bounds for the number of n-vertex graphs in such graph classes, but all the previously known lower bounds were obtained from ad hoc constructions for very specific classes. We prove a general theorem giving a lower bound for this number (under some reasonable assumptions on the fixed list of polynomials), and this lower bound essentially matches the upper bound from Warren’s theorem."
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http://forums.wolfram.com/mathgroup/archive/2009/Aug/msg00010.html | [
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"Assume and \\$Assumptions and Results\n\n• To: mathgroup at smc.vnet.net\n• Subject: [mg102216] Assume and \\$Assumptions and Results\n• From: ivo welch <ivowel at gmail.com>\n• Date: Sat, 1 Aug 2009 04:02:49 -0400 (EDT)\n\n```[Easy Beginner's Query]\n\nDear Experts:\n\nMy goal is to input a set of assumptions for various variables, and then\ndetermine whether an expression of these variables (a long derivative that\nis a few lines) is true or false. That is, I want to input many conditions,\nsuch as \"\\$Assumptions = (x>y) && (y>1)\" and then ask Mathematica whether \"1/(X+Y) >\n1.5\" is true, for example.\n\nAlas, I am a little stuck on home plate:\nSimplify[ x > 1, x>0 ]\ngiven that x is greater than 0, isn't it supposed to be True? Instead Mathematica\nreturns \"x>1\". It also does not help to make the condition \"(x\n<esc>elem<esc> Reals) && (x>0)\" .\n\n(Another brief questions: do \\$Assumptions assignments add or replace\nearlier assumptions?)\n\nHelp appreciated. Am I expecting too much of Mathematica?\n\n/iaw\n\n```\n\n• Prev by Date: Re: Help with concatenating a list with &&\n• Next by Date: Re: Finding the Position of Elements in a List that Contain\n• Previous by thread: Re: Creating a Random Function to Select an Irrational\n• Next by thread: Re: Assume and \\$Assumptions and Results"
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https://slideplayer.com/slide/4213092/ | [
"",
null,
"### Similar presentations\n\n3 You can see from Figure 1 that the sine function y = sin x is not one-to-one (use the Horizontal Line Test). Figure 1\n\n4 Inverse Trigonometric Functions But the function f (x) = sin x, – /2 x /2 is one-to-one (see Figure 2).The inverse function of this restricted sine function f exists and is denoted by sin –1 or arcsin. It is called the inverse sine function or the arcsine function. Figure 2 y = sin x,\n\n5 Inverse Trigonometric Functions Since the definition of an inverse function says that f –1 (x) = y f (y) = x we have Thus, if –1 x 1, sin –1 x is the number between – /2 and /2 whose sine is x.\n\n6 Example 1 Evaluate (a) sin –1 and (b) tan(arcsin ). Solution: (a)We have Because sin( /6) = and /6 lies between – /2 and /2.\n\n7 Example 1 – Solution (b) Let = arcsin, so sin =. Then we can draw a right triangle with angle as in Figure 3 and deduce from the Pythagorean Theorem that the third side has length This enables us to read from the triangle that Figure 3\n\n8 Inverse Trigonometric Functions The cancellation equations for inverse functions become, in this case,\n\n9 Inverse Trigonometric Functions The inverse sine function, sin –1, has domain [–1, 1] and range [– /2, /2], and its graph, shown in Figure 4, is obtained from that of the restricted sine function (Figure 2) by reflection about the line y = x. Figure 4 y = sin –1 x = arcsin x\n\n10 Inverse Trigonometric Functions We know that the sine function f is continuous, so the inverse sine function is also continuous. The sine function is differentiable, so the inverse sine function is also differentiable. Let y = sin –1 x. Then sin y = x and – /2 y /2. Differentiating sin y = x implicitly with respect to x, we obtain and\n\n11 Inverse Trigonometric Functions Now cos y 0 since – /2 y /2, so Therefore\n\n12 Example 2 If f (x) = sin –1 (x 2 – 1), find (a) the domain of f, (b) f (x), and (c) the domain of f. Solution: (a) Since the domain of the inverse sine function is [–1, 1], the domain of f is {x| –1 x 2 – 1 1} = {x | 0 x 2 2}\n\n13 Example 2 – Solution (b) Combining Formula 3 with the Chain Rule, we have (c) The domain of f is {x | –1 < x 2 – 1 < 1} = {x | 0 < x 2 < 2} cont’d\n\n14 Inverse Trigonometric Functions The inverse cosine function is handled similarly. The restricted cosine function f (x) = cos x, 0 x is one-to-one (see Figure 6) and so it has an inverse function denoted by cos –1 or arccos. Figure 6 y = cos x, 0 x π\n\n15 Inverse Trigonometric Functions The cancellation equations are The inverse cosine function, cos –1, has domain [–1, 1] and range [0, ] and is a continuous function whose graph is shown in Figure 7. Figure 7 y = cos –1 x = arccos x\n\n16 Inverse Trigonometric Functions Its derivative is given by The tangent function can be made one-to-one by restricting it to the interval (– /2, /2). Thus the inverse tangent function is defined as the inverse of the function f (x) = tan x, – /2 < x < /2.\n\n17 Inverse Trigonometric Functions It is denoted by tan –1 or arctan. (See Figure 8.) Figure 8 y = tan x, < x <\n\n18 Example 3 Simplify the expression cos(tan –1 x). Solution1: Let y = tan –1 x. Then tan y = x and – /2 < y < /2. We want to find cos y but, since tan y is known, it is easier to find sec y first: sec 2 y = 1 + tan 2 y = 1 + x 2 Thus (since sec y > 0 for – /2 < y < /2)\n\n19 Example 3 – Solution 2 Instead of using trigonometric identities as in Solution 1, it is perhaps easier to use a diagram. If y = tan –1 x, then, tan y = x and we can read from Figure 9 (which illustrates the case y > 0) that cont’d Figure 9\n\n20 Inverse Trigonometric Functions The inverse tangent function, tan –1 x = arctan, has domain and range (– /2, /2). Its graph is shown in Figure 10. Figure 10 y = tan –1 x = arctan x\n\n21 Inverse Trigonometric Functions We know that and and so the lines x = /2 are vertical asymptotes of the graph of tan. Since the graph of tan –1 is obtained by reflecting the graph of the restricted tangent function about the line y = x, it follows that the lines y = /2 and y = – /2 are horizontal asymptotes of the graph of tan –1.\n\n22 Inverse Trigonometric Functions This fact is expressed by the following limits:\n\n23 Example 4 Evaluate arctan Solution: If we let t = 1/(x – 2), we know that t as x 2 +. Therefore, by the first equation in, we have\n\n24 Inverse Trigonometric Functions Because tan is differentiable, tan –1 is also differentiable. To find its derivative, we let y = tan –1 x. Then tan y = x. Differentiating this latter equation implicitly with respect to x, we have and so\n\n25 Inverse Trigonometric Functions The remaining inverse trigonometric functions are not used as frequently and are summarized here.\n\n26 Inverse Trigonometric Functions We collect in Table 11 the differentiation formulas for all of the inverse trigonometric functions.\n\n27 Inverse Trigonometric Functions Each of these formulas can be combined with the Chain Rule. For instance, if u is a differentiable function of x, then and\n\n28 Example 5 Differentiate (a) y = and (b) f (x) = x arctan. Solution: (a) (b)\n\n29 Inverse Trigonometric Functions\n\n30 Example 7 Find Solution: If we write then the integral resembles Equation 12 and the substitution u = 2x is suggested.\n\n31 Example 7 – Solution This gives du = 2dx, so dx = du /2. When x = 0, u = 0; when x =, u =. So cont’d\n\n32 Inverse Trigonometric Functions\n\n33 Example 9 Find Solution: We substitute u = x 2 because then du = 2xdx and we can use Equation 14 with a = 3:"
]
| [
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https://rakshithv.medium.com/einsum-equation-bb5f6292a98c?source=post_internal_links---------2------------------------------- | [
"Einsum equation:\n\nIt’ an elegant way to perform matrix or vector manipulation.\n\nI find it’s extremely useful if I have to perform matrix multiplication of matrices which is of higher dimension, it gives a great flexibility to sum and multiply among certain axis.\n\nEx : if you have to multiply matrix A of shape (1,200,2,32) & matrix B of shape (2,32,32) and results in a matrix C of shape (1,200,32).\n\nThis can be implemented as follows:\n\nnp.einsum(‘abcd,cde->abe’,A,B)\n\nThat’s it !\n\nIt can be implemented similarly in Tensor-flow & PyTorch.\n\nIn “Attention is all you need” paper, they concatenate different heads but in implementation they multiply different heads with weight matrix, I will be discussing few examples from this paper.\n\nSyntax of “einsum” equation:\n\nnp.einsum(‘shape_of_A, shape_of_B -> shape_of_C’,A,B)\n\nLet’s take a simple example:\n\nHere, we are multiplying matrix A of shape (2,3) and matrix of shape (3,5) and results in matrix of shape(2,5).\n\nA.shape = a, A.shape = b,\n\nB.shape = b, B.shape = c\n\nC.shape = a, C.shape = c\n\nIf we want to implement the same using loops:\n\n1. Output indices (indices after ‘->’) ‘ac’ forms the outer loop\n\n2. If an index is in both matrix and not in the output matrix then it will be summed across that index.\n\n‘ab,bc’ -> ‘b’ is in both matrix and not in the output matrix so it will be summed (‘ab,bc->ac’)\n\nNow, few more examples with respect to “Attention is all you need” paper. Let’s say our batch_size is 1, max_words is 200, it’s embedding is 32. Our input will be [1,200,32] and in order to obtain query, key & value, we can multiply with weight matrix let’s say we have 2 heads then[2,32,32] -> Wq . Similarly we will have Wk and Wv.\n\nSo [1,200,32] *[32,2,32] → [1,200,2,32]\n\nAfter performing the attention we have matrix [1,200,2,32]. Now as per as paper, heads are concatenated but it’s actually multiplied as I mentioned earlier.\n\nAs shown earlier this can be written using loops as well\n\na,b& e forms the outer loop and we sum across (c&d) which are common in both and doesn’t appear in the output"
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https://www.tobmac.com/18905.html | [
"# 如何在 Microsoft Excel 中使用 SUMIF",
null,
"## 将 SUMIF 用于单个单元格范围\n\n``=SUMIF(C2:C7,\">25000\")``",
null,
"``=SUMIF(B2:B7,\"<10000\")``",
null,
"``=SUMIF(A2:A7,\"5000\")``",
null,
"## 将 SUMIF 与数字标准一起用于多个范围\n\n``=SUMIF(B2:B7,\"<10000\",C2:C7)``",
null,
"``=SUMIF(C2:C7,\">25000\",B2:B7)``",
null,
"``=SUMIF(C2:C7,\">\"&D2,B2:B7)``",
null,
"## 将 SUMIF 与多个范围的文本条件结合使用\n\n``=SUMIF(A2:B7,\"服装\",C2:C7)``",
null,
"``=SUMIF(B2:B7,\"*ts\",C2:C7)``",
null,
"``=SUMIF(A2:B7,\"\",C2:C7)``",
null,
"Excel 中的 SUMIF 函数允许您采用基本方程并对其进行调整以满足您的需要。当添加数字不像二加二那么简单时,它非常方便。"
]
| [
null,
"https://www.tobmac.com/wp-content/themes/wordpress-theme-puock-2.7.4.2/assets/img/z/load.svg",
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null,
"https://www.tobmac.com/wp-content/themes/wordpress-theme-puock-2.7.4.2/assets/img/z/load.svg",
null,
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null,
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null,
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null
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http://tutorialsocean.com/how-to-calculate-depreciation-in-excel-sln-syd-ddb-functions/ | [
"# How to Calculate Depreciation with Microsoft Excel SLN, SYD, DDB Functions in Easy Way [Full Tutorials]\n\n## Depreciation:\n\nIn this tutorial, we will discuss, How to Calculate Depreciation with Microsoft Excel SLN, SYD, DDB Functions in Excel. Excel Provide five (05) different function to calculate depreciation expense. Let’s start with what is depreciation. How to Calculate Depreciation In Excel SLN SYD DDB Functions\n\nHow to Calculate Depreciation In Excel SLN SYD DDB Functions\n\n## What Is Depreciation?\n\nIn accounting terms, depreciation is defined as the reduction of the recorded cost of a fixed asset in a systematic manner until the value of the asset becomes zero or negligible.\n\nAn example of fixed assets are buildings, furniture, office equipment, machinery etc.. A land is the only exception which cannot be depreciated as the value of land appreciates with time.\n\n## How to Calculate Depreciation In Excel SLN SYD DDB Functions",
null,
"## Microsoft Excel Depreciation Functions.\n\nMicrosoft Excel Provide five (05) different function to calculate depreciation expense as follow:\n\n1. SLN Function Returns the straight-line depreciation of an asset for one period.\n2. SYD Function: Returns the sum-of-years’ digits depreciation of an asset for a specified period.\n3. DB Function: Returns the depreciation of an asset for a specified period using the fixed-declining balance method.\n4. DDB Function: Returns the depreciation of an asset for a specified period using the double-declining balance method or some other method you specify.\n5. VDB Function: Returns the depreciation of an asset for any period you specify, including partial periods, using the double-declining balance method or some other method you specify. VDB stands for variable declining balance.\n\n## SLN Function\n\nReturns the straight-line depreciation of an asset for one period. SLN Function is very simple and easy function, calculate the same every year.\n\n### SLN(cost,salvage,life)\n\nDefine Function Arguments.\n\nCost is the initial cost of the current asset.\n\nSalvage is the value at the end of the depreciation.\n\nLife is the number of periods over which the asset is depreciated.",
null,
"### Example:",
null,
"",
null,
"## SYD Function\n\nReturns the sum-of-years’ digits depreciation of an asset for a specified period.\n\n### SYD(cost,salvage,life,per)\n\nDefine Function Arguments.\n\nCost is the initial cost of the current asset.\n\nSalvage is the value at the end of the depreciation.\n\nLife is the number of periods over which the asset is depreciated.\n\nPer is the period and must use the same units as life.",
null,
"### Example:",
null,
"## DB Function\n\nReturns the depreciation of an asset for a specified period using the fixed-declining balance method.\n\n### DB(cost,salvage,life,period,month)\n\nCost is the initial cost of the asset.\n\nSalvage is the value at the end of the depreciation (sometimes called the salvage value of the asset).\n\nLife is the number of periods over which the asset is being depreciated (sometimes called the useful life of the asset).\n\nPeriod is the period for which you want to calculate the depreciation. Period must use the same units as life.\n\nMonth is the number of months in the first year. If month is omitted, it is assumed to be 12.\n\n### Example:",
null,
""
]
| [
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/Depreciation_car.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/SLN-Formula.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/SLN-Example.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/SLN-Brife.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/SYD-formula.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/Syd-example.png",
null,
"http://tutorialsocean.com/wp-content/uploads/2018/09/DB-Example.png",
null
]
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http://www.infocobuild.com/education/audio-video-courses/mathematics/calculus-i-nyu.html | [
"# InfoCoBuild\n\n## Calculus I\n\nCalculus I (NYU Open Education). Instructor: Professor Matthew Leingang. In this course, we will study the foundations of calculus, the study of functions and their rates of change. We want you to learn how to model situations in order to solve problems. If you have already taken calculus before, we want you to gain an even deeper understanding of this fascinating subject.\n\nThe derivative measures the instantaneous rate of change of a function. The definite integral measures the total accumulation of a function over an interval. These two ideas form the basis for nearly all mathematical formulas in science. The rules by which we can compute the derivative (respectively, the integral) of any function are called a calculus. The Fundamental Theorem of Calculus links the two processes of differentiation and integration in a beautiful way.\n\n Functions and their Representations\n\n Lecture 01 - Functions and their Representations Lecture 02 - A Catalogue of Essential Functions Lecture 03 - Limit Lecture 04 - Calculating Limits Lecture 05 - Continuity Lecture 06 - Limits Involving Infinity Lecture 07 - The Derivative Lecture 08 - Basic Differentiation Rules Lecture 09 - The Product, Quotient, and Chain Rules Lecture 10 - Implicit Differentiation Lecture 11 - Linear Approximations and Differentials Lecture 12 - Exponential Functions Lecture 13 - Derivatives of Logarithmic and Exponential Functions Lecture 14 - Exponential Growth and Decay Lecture 15 - Inverse Trigonometric Functions Lecture 16 - Indeterminate Forms and L'Hospital's Rule Lecture 17 - Maximum and Minimum Values Lecture 18 - The Mean Value Theorem Lecture 19 - Derivatives and the Shapes of Curves Lecture 20 - Curve Sketching Lecture 21 - Optimization Lecture 22 - Antiderivatives Lecture 23 - Areas and Distances, the Definite Integral Lecture 24 - Evaluating Definite Integrals Lecture 25 - The Fundamental Theorem of Calculus Lecture 26 - Integration by Substitution"
]
| [
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https://amulettejewelry.com/all-physics-formulas-pdf/ | [
"# All Physics Formulas Pdf\n\n## all physics formulas pdf",
null,
"You might care about employees like engineers, engineers, software engineers, etc. Scientists have arranged all the elements that are currently known in tables as periodic tables, and at different events, you can determine the value of studying graphs. Science is an extraordinary thing. As soon as you start thinking about it, then you are aware of your studies. As for home improvement, mathematics can also help owners to answer other questions as well.\nThis is a mathematical expression that can also be written as words. Many students find physics difficult because of various theories and mathematical problems. Prime numbers are very special not only in mathematics but also in special properties. Not difficult to use and has many features.\n\nThe more successful you get the easier it is to get more success and the harder it is for others to find access to success. Although there are many advantages of collaborative team work, it is not without problems. More than a proportional increase in management input may need to be expanded as soon as the organization becomes very large. The rate of change in the position of an object in a specific direction to time is known as velocity. The proportion of primary CT transformation was found.I plan your essay in the first five minutes is the secret of success. The question is how you approach the subject. Each problem will help you in each phase so you can understand how to get a solution. The problem is, in the financial world, it doesn’t sound like it seems, or a little ‘a little’. TOO can be synthetic and concise which can be misinterpreted or removed from the context.\n\nA very difficult problem may require a lot of knowledge or may be related to knowledge, but what makes it difficult must be the reason needed to find a problem where you can make an answer.\nChanges in leadership can bring a lot of anxiety into the team. You change the way you see things, you change things. Comparable to changes in leadership, changes in organizational structure can be a direct or indirect effect on the team.In essence, this is a matter of trying to clarify the complexity of the universe, predicting what will happen based on simple ideas. These are questions that can be integrated into the application. Some simple math skills will let you learn more. Again, training is important.\n\n## all physics formulas pdf",
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"By : www.pinterest.com\n\n## Physics Equation List (Formulas) & Solution Tips (PDF & Form)",
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"By : latestcontents.com\n\n## all physics formulas pdf",
null,
"By : www.nnci.net\n\n## PHYS 2206: physics formula sheet & constants (great overview",
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"By : www.pinterest.com\n\n## all physics formulas pdf",
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"By : www.slideshare.net\n\nElectromagnetism refers to the forces created by the electrons that are observed in certain varieties of matter across the universe. Physics involves many calculations and problem solving. This is one of the most important topics of Class 9. As you begin to explore physics, basic principles such as the use of substantial numbers and going beyond the fundamentals of the metric system will be important Physical formulas Physics is concerned with articulating things instead to memorize them.\n\nOur list should simply highlight the most useful key equations for the new MCAT. The physical form will also assist students during the review period prior to their examination. However, keep in mind that you won’t have the physical spreadsheet under your eyes during the exam, so you won’t want it to become a huge storage test.\nMost of the time, you have not been able to solve problems simply because you have forgotten the necessary formula. After all, the ideal of physics is the fact that it can be used to deal with the difficulties of the real world. Physics questions test your skills and your knowledge of physics based on three elements. To solve these types of problems, it is necessary to understand the formula of physics and its concepts. So you can easily find the best you need to solve your problems. If you want to solve a complex problem in your math topic or simply want to calculate your percentage in the final exams, you just have to use a formula to make sure you have an appropriate answer. The situation in the jar is far from ideal, so the estimates will be quite approximate.\n\nLooking at the Nautilus shapeddiagram, you can observe the organic symmetry in practice. Try to remember that the equations are approximate or take into account the air resistance. If you don’t recognize, check your schedule. These equations are called kinematic equations. Having the most used equations and physics formulas makes them possible. The formulas are approximate because they assume that there is no air resistance.\nDown the street, you can compare spreadsheets to see exactly which parts have changed. Page 1 sheet of formula geometrygeorgia The pdf file contains information on the geometrygeorgia formula sheet. It can be found in different versions. Georgia Geometry Formula Sheet The georgia geometry formula sheet is available in different versions.\n\nAmong the variables in the calculation must be incorrect. The value of the test record is considered the valid reference. Increasing the amount of gas molecules is not the only way to improve pressure.\nA tire pressure gauge is used to measure the most pressure created in the can once the ethanol is turned on. All you would like to do is follow the following simple steps. Another way to increase the pressure in a fixed volume container is to increase the temperature. It is therefore possible to estimate the temperature. Furthermore, a number of water which constitutes a reaction product will be liquid. Electricity, of course, is created through the manipulation of electromagnetic forces. The energy an object has because of its movement is called KE."
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https://www.onlinecalculatorsfree.com/convert/binary-to-octal.html | [
"# Binary to Octal converter",
null,
"Convert binary numbers to octal effortlessly with our user-friendly online tool. Whether you have a binary string or a series of binary digits, our converter can accurately convert it into octal format. Simply input the binary number and let our converter do the rest. It supports both unsigned and signed binary numbers, providing flexibility for various applications.\n\n2\n8\n10\n\nRelated\n\n## what is Binary to Octal converter\n\nA Binary to Octal converter is a tool that allows you to convert binary numbers (base-2) into octal numbers (base-8). The binary system uses only two digits, 0 and 1, while the octal system uses eight digits, 0 to 7.\n\nHere's how a Binary to Octal converter typically works:\n\n1. Input the binary number you want to convert.\n2. Group the binary digits into sets of three, starting from the rightmost digit. If the number of digits is not a multiple of three, pad the left side with zeros to complete the groupings.\n3. Replace each group of three binary digits with their corresponding octal digit.\n• 000 = 0\n• 001 = 1\n• 010 = 2\n• 011 = 3\n• 100 = 4\n• 101 = 5\n• 110 = 6\n• 111 = 7\n4. Concatenate the octal digits obtained in step 3 to form the final octal representation.\n\nFor example:\n\n• Converting the binary number 101010 to octal would be calculated as: 10 101 0 -> 2 5 0 -> 250.\n\nBinary to Octal converters are useful in computer programming and digital systems analysis, especially when dealing with bit manipulation or storage optimization. They can be found as online tools, calculator applications, or programming language functions for easy conversion between binary and octal representations.\n\n## How to convert binary to octal\n\nConvert every 3 binary digits (start from bit 0) to 1 octal digit, with this table:\n\nBinary Octal\n000 0\n001 1\n010 2\n011 3\n100 4\n101 5\n110 6\n111 7\n\n### Example\n\nConvert binary 11011002 to octal:\n\nConvert every 3 binary bits (from bit0) to octal digit:\n\n11011002 = 1 101 100 = 1 5 4 = 1548"
]
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"https://www.onlinecalculatorsfree.com/calculator/images/full_in.png",
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https://www.broadheath.coventry.sch.uk/11-05-20-4b-maths-home-learning/ | [
"# 11.05.20 – 4B Maths home learning\n\nMorning 4 Blue, this week we are moving on to learning about money. Now money and decimals are very closely linked so you will need to use your knowledge from the last few weeks and apply it to this weeks learning.\n\nBRONZE: How many ways can you make the following amounts of money?\n\n1. 55p\n2. 37p\n3. 108p\n4. 502p\n5. 99p\n6. 88p\n\nSILVER: Answer the following questions. 7a and 7b, 8a and 8b.\n\nGOLD:\n\nGreater Depth\n\n## 46 thoughts on “11.05.20 – 4B Maths home learning”\n\n1. Yalda N.\n\nBronze\n55\n50+5= 55,\n20+20+10+5, 2+2+1+2+2+1+20+20+5= 55, Are some ways to make 55.\n\n37\n20+10+2+2+1+1+1=37.\n10+10+5+5++5+1+1+1=37.\nAre some ways to make 37\n\n£1.08\n£1+8= £1.08\n£1+2+2+2+2= £1.08\nAre some ways to make £1.08\n\n£5.02\n£5+2=£5.02\n£2+£2+£1+1+1=£5.02\nAre some ways to make £5.02\n\n99\n50+20+20+5+2+2=99\n5+5+5+5+20+50+1+1+1+1+1+1+1+1+1=99\nAre some ways to make 99\n\n88\n50+20+10+5+2+1=88\n5+5+20+20+10+20+2+2+2+2=88\nAre some ways to make 88\n\n55p. 50p + 5p\n37p. 10p +5p+ 20+ 2p\n108p 1pound + 5p + 3p\n502p 1pound+2pound+ 2pound +2p\n99p. 50p+20p+20p+5p+2p+2p\n88p. 20p x4 +5p +2p+1p\n1. £1.85p\n2. £1.72p\n3. £1.61P\n4. £1.80P\n\n3. Merab R.\n\nBronze\n1)55p. 50+5=55p. 30+25=55. 20+20+10+5=55\n37p. 30+7=37p 20+17=37p. 37+0=37p\n108p. 100+8=108. 107+1=108. 99+9=108\n502p. 500+2=502. 501+1=502. 499+3=502\n99p. 90+9=99. 89+10=99. 87+12=99\n88p. 80+8=88. 72+16=88. 79+9=88\n\nSilver\n7a)\nA)£1.85p\nB)£1.72p\n\n7b)\nA)£1.61p\nB)£1.80p\n\n8a)£2.30p\n8b)£1.40p\n\nGold\n4a)No one can get it because they do not have the total of £3.75.Laura has £3.65 and Liam has £2.75p which means they don’t have the total amount they need to get the football.\n\n6a)The combination Awais can make to get £2.20p is:\n£2+5p+5p+10p\n\nGreater depth\nShe can make a total which ends in 2-sometimes\nShe can make an odd amount-sometimes\nShe can make an amount greater tan £6.00-sometimes\nShe can make a total which is a multiple of 5p-always.\n\n4. Harris B.\n\nBronze\n55p=50p+5p\n55p=10p+10p+10p+10p+10p+5p\n37p=10p+10p+10p+5p+2p\n37p=20p+10p+5p+1p+1p\n108p=50p+50p+5p+3p\n108p=£1+8p\n502p=£2+2£+1£+2p\n99p=50p+20p+20p+5p+2p+2p+1p\n88p=50p+20p+10p+2p+2p+2p+2p\nsilver\n7.a.£1+50p+20p+10p+5p=£1+80p+5p=£1+85p=100p+85p=185p\n=1.85£\nB=1£+50p+20p+2p=£1+70p+2p=£1+72p=172p=1.72£\n7.b.\nA=£1+50p+10p+1p=£1+61p=161p=1.61£\nB=1£+50p+10p+20p=1£+80p=180p=1.80£\n8.a.1£+50p+20px4=1£+50p+80p=1£+130p=230p=2.30£\n\n• Miss Roberts\n\nWell done Harris. Remember the pound sign goes before the numbers, for example; £1.40\n\n5. Eesa F.\n\n55p- 50p+5p+55p 40p+10+5p=55p 20p+20p+10p+5p=55p\n37p- 10+10+10+2p+2p+2p+1p=37P 20p+10p+5p+2p=37p\n£1.08p- 50p+50p+ 2p+2p+2p+2p=£1.08p 20p+20p+10p+50p+2p+2p+2p+2p = £1.08p\n£5.02p- £2 + £2 + £1 + 2p = £5.02p\n£1 + £1 + £1 + £1 + £1 + 1p + 1p = £5.02p\n99p- 50p + 20p +10p + 10p + 5p + 2p + 2p = 99p\n20p + 20p + 20p + 20p + 10p + 2p + 2p+ 2p+ 2p+1p=99p\n88p 20p + 20p + 20p + 20p + 2p + 2p + 2p +2p =88p\n50p + 20p + 10p + 5p + 2p + 1p = 88p\n\n6. Kia J.\n\n55p. 50p + 5p\n37p. 10p +5p+ 20+ 2p\n108p 1pound + 5p + 3p\n502p 1pound+2pound+ 2pound +2p\n99p. 50p+20p+20p+5p+2p+2p\n88p. 20p x4 +5p +2p+1p\n\n1. £1.85p\n2. £1.72p\n3. £1.61P\n4. £1.80P\n\n• Miss Roberts\n\nWell done Kia\n\n7. Aleena M.\n\nBRONZE\n55p-50 p+5p\n37p-30p+7p\n108p-100p+8p\n502p-500p+2p\n99p-90+9p\n88p-80p+8p\n\nSILVER\n7a- jar 1 £1.85\nJar 2 £1.72\n7b- jar 1 £1.61\nJar 2 £1.80\n8a. £2.30\n8b. £1.40\n\nGOLD\nLiam can afford the football because £1+£1+50p+50p+50p+20p+5p=£3.75.\n\n• Mr Carter\n\nFor bronze you needed to make the amounts out of UK coins.\n\n8. Asilah K.\n\nBronze\n55p\n10 + 10 + 10 + 10 +10 + 5 = 55p\n37 + 29 = 55p\n55 + 0 = 55\n37\n20 + 10 + 7 = 37\n10+ 10+ 10+ 7=37\n30+ 7 = 37\n108\n£1 + 8 = 108\n98 + 10 = 108\n50 + 50 + 8 = 108\n\n30 + 7 = 37\n\n5+5+5+5+5+5+7=37\n108\n£1 + 8 = 108\n98 + 10 = 108\n\n• Mr Carter\n\nGood try, but remember this is all about money and you can only use the coins we have in real life.\n\n9. Esra S.\n\n55p=\n25+30=55p\n10+10+10+10+10+5=55p\n37p=\n20+10+5+2=37p\n10+20+2+2+1+2=37p\n108p=\n100+5+2+1=108p\n50+50+5+1+2=108p\n502p=\n500+2=502p\n200+200+50+50+2=502p\n99p=\n50+20+20+5+2+2=99p\n£1-1=99p\n\n• Mr Carter\n\nA good start Esra, but still lots to do. You should be completing all challenges in this blog please.\n\n10. Rida W.\n\nSilver:\n7a) A £1 + 50p + 20p + 10p + 5p = £1.85\nB £1 + 50p + 20p + 2p = £1.72\n\n7b) A £1 + 50p + 10p + 1p = £1.61\nB £1 + 50p + 20p + 10p = £1.80\n\n8a. £1 + 50p + 20p + 20p + 20p + 20p = £2.30\n8b. 50p + 20p + 20p + 20p + 10p + 10p + 10p = £1.40\n\n• Mr Carter\n\nGood understanding Rida, but you also need to give each total in pence too. For example, £1.85=185p\n\n11. Musab H.\n\nsilver\n£1.85\n£1.72\n£1.61\n£1.80\n\nGold\nLiam can afford it because he has enough money and laura cant\n\n• Mr Carter\n\nWell done for getting on the blog, but you are not doing all of each challenge. For this challenge you also need to give each total in pence too. For example, £1.85=185p\n\nBronze\n5p+50p=55p\n10p+5p+20p+20p=55p\n20p+20p+10p+5=55p\n\n2p+10p+10p+10p+5p=37p\n20p+10p+5p+2p=37p\n10p+10p+10p+5p+2p=37p\n\n£1+2+2+2+2=108\n£1+5+2+1=108\n£1+1+2+5=108\n\n£5+2=502\n£5+1+1=502\n£4+50+50+2=502\n\n50+20+20+5+2+2=99\n20+50+20+5+2+1+1=99\n50+10+10+2+1+2+2+2\n\n20+20+20+20+5+2+1=88\n50+20+10+5+2+1=88\n10+10+10+50+2+1+5=88\n______________________________________________\nSilver\n7a 1.85\n1.72\n7b 1.61\n1.80\n8a 2.30\n8b 1.40\n\nGold:\n4a Liam =2.75 X\nLuara = 3.45\nNone of them can afford because their money is lower than 3.75 X\n\n6a £1+£1+10p+10p = £2.20\n\nGD- I tried on Greater depth\n1-Sometimes X\n2-Sometimes\n3-Always X\n4- always\n\n• Mr Carter\n\nWell done Rayyan, you Bronze answers have used the coins. Not everyone has done this but there are some misconceptions here. Firstly, you have not included the unit of measure for a few.\nWith your Silver challenges, what is the unit of measure? 185p = 1.85 what?\nAlso, your calculating for Liam’s coins is not quite right, please think again.\n\n13. Raihaan N.\n\nBronze\n55p =50p+5p=27p+28p=13p+42p\n37p =20p+17=35p+2p=21p+16p\n108p =58p+50p=100p+8p\n502p =250p+252p=372+130p\n99p =98p+1p=90p+8p\n88p =76p+12p=80p+8p\nSilver\n7.A a) There is 195p in the jar.1.95\nb)There is 182p in the jar.1.82\n7.B a) There is 161p in the jar.1.61\nb) There is 180p in the jar.1.80\n8.A. There is £2.30\n8.B. There is £1.40\nGold\nLiam can buy a football because he has £2+£1.50+20p+5p=£3.75 Liam has 3.75 so he can buy a football that costs that exact amount.But Laura has £3+40p+25p=3.65 Laura has 3.65 meaning she has 10p less then Liam meaning she can’t buy a football.\nAwais could have a 20p a £1 and 2 50p coins.He could also have a 2 £1 and 2 10p coins.\n\n• Mr Carter\n\nYou have a few misconceptions here Raihaan. Next time, please make sure you read all the teaching slides, because they would have explained and made it clear how you needed to answer.\nFor example, where you have said, “13p+42p”, there is no 13p coin or 42p coin. Remember this is all about money and you can only use the coins we have in real life.\n\nAlso, when you have converted 185p into decimals, you have put 1.85. What is the unit of measure?\n\n14. Rasan M.\n\nBronze:\n1. 55p\n5×11=55p\n50p+5p=55p\n30p+25p=55p\n35p+20p=55p\n2. 37p\n20p+17p=37p\n27p+10p=37p\n67p+30p=37p\n69p+32p=37p\n3. 108p\n50p+58p=108p\n38p+70p=108p\n78p+30p=108p\n60p+48p=108p\n4. 502p\n302p+200p=502p\n152p+350p=502p\n400p+102=502p\n132p+370p=502p\n5. 99p\n90p+9p=99p\n49p+50p=99p\n37p+62p=99p\n6. 88p\n80p+8p=88p\n40p+48p=88p\n58p+40p=88p\n38p+50p=88p\nSilver:\n7a. A:185p–0.185p\nB:182p–0.182p\n7b. A:161p–0.161p\nB:180p–0.180p\n\n• Mr Carter\n\nYou have a few misconceptions here Rasan. Next time, please make sure you read all the teaching slides, because they would have explained and made it clear how you needed to answer.\nFor example, where you have said, “30p+25p=55p”, there is no 30p coin or 25p coin. Remember this is all about money and you can only use the coins we have in real life.\nYou have also said, “185p–0.185p” when showing the decimal. To show the decimal, you would need to convert the pence into pounds. e.g. 185p = £1.85. Please can you have a go at correcting your mistakes.\n\n• Rasan M.\n\n1)55p\n20p+10p+20p+5p=55p\n20p+10p+5p+20p=55p\n2) 37p\n20p+10p+5p+2p=37p\n10p+10p+10p+5p+2p=37p\n3)£1.08\n50p+50p+5p+1p+1p+1p=£1.08\n20p+20p+20p+20p+20p+5p+1p+1p+1p=£1.08\n4) £5.02\n50p+50p+50p+50p+50p+50p+50p+50p+50p+50p+2p=£5.02\n5) 99p\n50p+20p+20p+5p+2p+2p=99p\n6)88p\n20p+20p+20p+20p+5p+1p+1p+1p=88p\nSilver:\n7a) A)185p=£1.85\nB)182p=£1.82\n7b) A)161p=£1.61\nB)180p=£1.80\n\n15. Sheima B.\n\nBRONZE: How many ways can you make the following amounts of money?\n\n55p 50+5 49+6 48+7 47+8 46+9 45+10\n37p 30+7 29+8 28+9 27+10 26+11 25+12\n108p 100+8 99+9 98+10 97+11 96+12 95+13\n502p 498+4 500+2 499+3 497+5 496+6\n99p 90+9 89+10 88+11 87+12 86+13\n88p 80+8 79+9 78+10 77+11 76+12\nsilver\n7a. 1 pound 85p 1 pound 72p\n7b. 1 pound 65p 1 pound 80p\n8a. you have £2.30\n8b. you have £1.40\n\n• Miss Roberts\n\nShemia you are more than capable of gold. Please try and push yourself\n\n16. Ellie T.\n\n55p\nSliver 1 pound 88p\n1 pound 72p\n1 pound 61 p\n1 pound 80 p\n\n• Mr Carter\n\nWell done Ellie.\nWith your silver answers, you needed to give them in pence and decimal form… e.g. 188p and £1.88. See if you can add these for the other 3.\n\n17. Shabaz A.\n\nBronze\n1. 50p+5p=55p 50+1+1+1+1+1=55 50+2+2+1 50+2+1+1+1=55 are some ways\n2. 20+10+5+2=37 10+10+10+2+2+1+2=37 are some ways\n3. £1+5p+2p+1p=108p is a way\n4. £5+2p=502p £5+1p+1p=502p are ways\n5. 50p+50p-1p=99p is a way\n6. 50p+20p+10p+5p+2p+1p=88\nSilver\n7a. A. There is £1.85 B. There is £1.71\n7b. A. There is £1.71 B. There is £1.80.\n8a. You have £2.30\n8b. You have £1.40\nGold\nLiam could afford the football because 2 pounds, three fifty pence, twenty pence and a five pence coin which makes £3.75 and Laura made £3.65 which was just ten less than Liam.\n\n• Miss Roberts\n\nHave a look at answer 7ab. And 7ba again. It’s important to always check your answers Shabaz.\n\n• Shabaz A.\n\n7a. £1.85\n7b. £1.72\n\n• Shabaz A.\n\n7ba. £1.61\n\n• Miss Roberts\n\n18. Siddra K.\n\nBronze\n55p.1 p+1p+1p+1p+1p+50p=55p\n37p. 1p + 20p +16p =37p\n108p.50p + 50p + 4p + 4p =108p\n502p.250p + 250p + 2p = 502p\n99p. 81p + 18p = 99p\n88p.70p + 18p = 88p\n\n• Mr Carter\n\nSome good answers Siddra but you were asked to show the amount in lots of different ways. Please make sure you complete challenge how they are requested.\n\nBronze\n35+20=55\n50+5=55\n45+10=55\n55+0=55\n40+15=55\n30+7=37\n20+17=37\n25+12=37\n35+2=37\n10+27=37\n£1+8=108\n90+18=108\n70+38=108\n80+28=108\n95+13=108\n90+9=99\n80+19=99\n85+14=99\n70+29=99\n95+4=99\n80+8=88\n85+3=88\n60+28=88\n70+18=88\n75+13=88\nSilver\nA. There is £1.85\nB. There is £1.72\nA. There is £1.61\nB. There is £1.80\n\n• Miss Roberts\n\nCan you finish all the questions in silver and gold Danyaal. You are capable of much much more!\n\nGold\nLiam can afford a football and Laura can’t and Liam has £3.75. But Laura has £3.65 so she is 10p short.\nThe coins Awais could have are two 1 pound coins and 2 ten coins. Then it will equal £2.20 in 4 coins.\n\n20. Yalda N.\n\nBronze\n1+54+55. 5+50=55. 40+15=55. 20+35=55. Are some ways to make 55.\n30+7=37. 20+17=37.15+22=37.10+25=37. Are some ways to make 37.\n£1+8p=108. £1+2+2+2+2=108. £1+3+3+2=108.Are some ways to make\n108.\n£5+2=502. £5+1+1=502. £1+£1+£3+2=502. Are some ways.\n90+9=99. 50+49=99. 88+11=99. Are some ways.\n80+8=88. 40+48=88. 10+40+38=88. Are some ways.\n\n• Mr Carter\n\nYou have very few correct answers here Yalda because you haven’t used coin values. For example, where you have said, “40+15=55”, there is no 40p coin or 15p coin. Remember this is all about money and you can only use the coins we have in real life.\n\nAlso, please ensure you include your unit of measure (p or £) in each calculation.\ne.g. 50p + 1p +2p +2p = 55p\n\n21. 1. 10+10+10+10+10+5= 55p\n10+10+10+10+10+2+2+1=55p\n50 + 5 =55p\n20 + 20 + 10 + 5 = 55p\n2. 10 + 10 + 10 + 5 + 2 = 37p\n20 + 10 + 2 + 2 + 2 + 1 = 37p\n20 + 5 + 5 + 5 + 1 + 1 = 37p\n3. 50 + 50 + 5 + 2 + 1 = £1.08p\n20 + 20 + 50 + 10 + 2 + 2 + 2 + 2 = £1.08 p\n4. £2 + £2 + £1 + 2p = £5.02p\n£1 + £1 + £1 + £1 + £1 + 1p + 1p = £5.02p\n5. 50 + 20 +10 + 10 + 5 + 2 + 2 = 99p\n20 + 20 + 20 + 20 + 10 + 2 + 2+ 2+ 2+1=99p\n6.20 + 20 + 20 + 20 + 2 + 2 + 2 +2 =88p\n50 + 20 + 10 + 5 + 2 + 1 = 88p\n\nSilver\n7a. £1.85 7b. £1.72\n8a. £1.61 8b. £1.80\n\nGold\nLiam has £3.75 because £1 + £1 + 50p + 50p + 50p + 20p + 5p = £3.75\nLaura has £3.65 because £1 + £1 +£1 + 20p + 20p + 5p + 5p + 5p + 5p + 5p = £3.65. So Liam has enough money to buy the football.\n\nAwais has these coins ; £1 + £1 + 10p + 10p = £2.20\n\n• Miss Roberts\n\nWell done Noah, remember to answer all of the task. As you’ve missed some questions from silver.\n\n22. Timothy C.\n\nBronze\n1.50p+5p=55p 50+1+1+1+1+1=55 50+2+2+1 50+2+1+1+1=55 are some ways\n2.20+10+5+2=37 10+10+10+2+2+1+2=37 are some ways\n3.£1+5p+2p+1p=108p is a way\n4.£5+2p=502p £5+1p+1p=502p are ways\n5.50p+50p-1p=99p is a way\n6.\n\n• Timothy C.\n\n6.50p+20p+10p+5p+2p+1p=88\nSilver\n7a. A. There is £1.85 B. There is £1.71\n7b. A. There is £1.71 B. There is £1.80.\n8a. You have £2.30\n8b. You have £1.40\nGold\nLaura could’ve of afford the football if she had a 50p instead of two 20p\n\n• Mr Carter\n\nTimothy, please complete all gold challenges as these are the ones that will stretch you."
]
| [
null
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https://oxyplot.userecho.com/communities/1/topics/64-polar-plot-point-interpolation?lang=de | [
"",
null,
"+1\nWird überprüft\n\n# Polar plot point interpolation\n\nbsguedes vor 5 Jahren aktualisiert vor 5 Jahren\nHi,\n\nI'm trying to translate a XY chart into a polar plot. I have a collection of points in a given time that are represented on the XY chart (chart 1) with time on the X axis and the angle (in function of time) on the Y axis.\n\nWhen I try to plot the equivalent polar chart, I expect to have the time on the radius and the angle on the angle axis. However, Oxyplot connects the points using a direct line between each two subsequent points, like the attachment image I've uploaded (on the 'wrong' label, chart 4).\n\nI would expect that this interpolation would create an arc between each pair of points (char 3): this way, we don't go 'back in time' (you can notice this behaviour on the orange section of one of those lines that I marked on the attachment image... the interpolation that oxyplot does implies that on a XY chart we would have something like the chart number 3... notice that we go backwards in that interpolation too).\n\nIs there a way to consider this kind of interpolation on the polar chart (chart number 2)?",
null,
"Forgot the attachment: http://i.imgur.com/qdDZ9Jx.png",
null,
"Wird überprüft\nHave you tried setting the \"Smooth\" property on the LineSeries to true?",
null,
"Hi objo, thanks for the answer!\n\nUnfortunately it does not return the expected chart. If I set Smooth to true, I have this:\n\nhttp://i.imgur.com/UjQenrZ.png\n\nAs you can see, I still have the \"series going backwards\" problem.",
null,
"thanks for testing! Yes, smooth is interpolating the final transformed points and will not help here. In this case I think we need to interpolate before applying the polar axes transforms. I think there should be a similar problem for logarithmic axes. It could be handled by the LineSeries, but I think the problem is to find how many interpolated points are required... I think a workaround is to interpolate yourself before adding the points to the LineSeries. Add a ScatterSeries with the original points for the markers.",
null,
"There is something interesting going on when I set Smooth to true. Even though the series is not respecting the time constraint, the tracker is not following the series! It is following the exactly path that I wanted in the first place.\n\nhttp://i.imgur.com/PmbOkMs.png\n\nIt may be difficult to view this as a static image, but when I advance the tracker I never go backwards, like I was trying to do (this will only happen with smooth = true). So this interpolation is being done already some place, it is just not plotted as a series."
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https://www.howtogeek.com/howto/28961/calculate-simple-math-quickly-in-onenote/ | [
"Did you know that you can solve a wide range of math problems in OneNote? Whether you’re taking notes in class and working homework in OneNote or simply need to solve some quick math, here’s how you can use OneNote to help you out.\n\nOneNote is a great tool for taking notes, keeping outlines, and more. It makes it easy to keep your info organized and connected, and lets you include a wide range of data in your notes.",
null,
"One slightly hidden OneNote feature is its ability to solve math problems. Simply enter a simple equation with an equals sign, press Enter or the spacebar on your keyboard, and OneNote will automatically calculate the result.",
null,
"OneNote can calculate SIN, COS, logarithms, radians, and more. Here’s a longer equation we solved directly in OneNote; just write out your equation as you’d enter it in a scientific or graphing calculator, and it’ll calculate the results just like you’d expect.",
null,
"You can solve factorials in seconds, or find the remainder with the mod function.",
null,
"OneNote also works with the Greek letters used in mathematics, such as π and φ. To add these to problems, click the Symbol button in the Insert tab, and select the symbol you need.",
null,
"Here we solved a problem with π:",
null,
"Here’s a list of all the mathematics operators and functions you can use in OneNote, courtesy of the OneNote Blog:\n\nSupported operators:\n\n Arithmetic operator Meaning Example + (plus sign) Addition 3+3 – (minus sign) Subtraction, Negation 3–1, –1 * (asterisk) Multiplication 3*3 X or x Multiplication 3×3 / (forward slash) Division 3/3 % (percent sign) Percent 20% ^ (caret) Exponentiation 3^2 ! (exclamation) Factorial computation 5!\n\nMath and Trigonometry functions:\n\n Function Description Syntax ABS Returns the absolute value of a number ABS(number) ACOS Returns the arccosine of a number ACOS(number) ASIN Returns the arcsine of a number ASIN(number) ATAN Returns the arctangent of a number ATAN (number) COS Returns the cosine of a number COS(number) DEG Converts an angle (in radians) to degrees DEG(angle) LN Returns the natural logarithm of a number LN(number) LOG Returns the natural logarithm of a number LOG(number) LOG2 Returns the base-2 logarithm of a number LOG2(number) LOG10 Returns the base-10 logarithm of a number LOG10(number) MOD Returns remainder of a division operation (number)MOD(number) PI Returns the value of π as a onstant PI PHI Returns the value of φ (the golden ratio) PHI PMT Calculates a loan payment based on a constant interest rate, a constant number of payments, and the present value of the total amount PMT(rate;nper;pv) RAD Converts an angle (in degrees) to radians RAD(angle) SIN Returns the sine of the given angle SIN(angle) SQRT Returns a positive square root SQRT(number) TAN Returns the tangent of a number TAN(number)\n\n## More OneNote Goodness\n\nIf you need to solve more advanced math problems in OneNote, check out our article on How to Solve and Graph Equations in OneNote with the Mathematics Addin. This lets you create 2D and 3D graphs, as well as solve, integrate, or differentiate a wide range of equations.",
null,
"OneNote is one of the best apps for students, and is tremendously versatile. If you’re just getting started with OneNote and want to learn more, check out our Beginners Guide to OneNote. Also, be sure to check out our list of Great Back to School Apps and Resources including student discounts for Office 2010 and more.\n\nHere’s some more great ways you can put OneNote to use:\n\nMatthew Guay\nMatthew Guay is a veteran app reviewer and technology tip writer. His work has appeared on Zapier's blog, AppStorm, Envato Tuts+, and his own blog, Techinch."
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https://stacks.math.columbia.edu/tag/09E4 | [
"Definition 15.108.1. We say that $A \\to B$ or $A \\subset B$ is an extension of discrete valuation rings if $A$ and $B$ are discrete valuation rings and $A \\to B$ is injective and local. In particular, if $\\pi _ A$ and $\\pi _ B$ are uniformizers of $A$ and $B$, then $\\pi _ A = u \\pi _ B^ e$ for some $e \\geq 1$ and unit $u$ of $B$. The integer $e$ does not depend on the choice of the uniformizers as it is also the unique integer $\\geq 1$ such that\n\n$\\mathfrak m_ A B = \\mathfrak m_ B^ e$\n\nThe integer $e$ is called the ramification index of $B$ over $A$. We say that $B$ is weakly unramified over $A$ if $e = 1$. If the extension of residue fields $\\kappa _ A = A/\\mathfrak m_ A \\subset \\kappa _ B = B/\\mathfrak m_ B$ is finite, then we set $f = [\\kappa _ B : \\kappa _ A]$ and we call it the residual degree or residue degree of the extension $A \\subset B$.\n\n## Post a comment\n\nYour email address will not be published. Required fields are marked.\n\nIn your comment you can use Markdown and LaTeX style mathematics (enclose it like $\\pi$). A preview option is available if you wish to see how it works out (just click on the eye in the toolbar).\n\nUnfortunately JavaScript is disabled in your browser, so the comment preview function will not work.\n\nAll contributions are licensed under the GNU Free Documentation License.\n\nIn order to prevent bots from posting comments, we would like you to prove that you are human. You can do this by filling in the name of the current tag in the following input field. As a reminder, this is tag 09E4. Beware of the difference between the letter 'O' and the digit '0'."
]
| [
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http://pys60.garage.maemo.org/doc/lib/profile-instant.html | [
"# 25.2 Instant User's Manual\n\nThis section is provided for users that ``don't want to read the manual.'' It provides a very brief overview, and allows a user to rapidly perform profiling on an existing application.\n\nTo profile an application with a main entry point of foo(), you would add the following to your module:\n\n```import cProfile\ncProfile.run('foo()')\n```\n\n(Use profile instead of cProfile if the latter is not available on your system.)\n\nThe above action would cause foo() to be run, and a series of informative lines (the profile) to be printed. The above approach is most useful when working with the interpreter. If you would like to save the results of a profile into a file for later examination, you can supply a file name as the second argument to the run() function:\n\n```import cProfile\ncProfile.run('foo()', 'fooprof')\n```\n\nThe file cProfile.py can also be invoked as a script to profile another script. For example:\n\n```python -m cProfile myscript.py\n```\n\ncProfile.py accepts two optional arguments on the command line:\n\n```cProfile.py [-o output_file] [-s sort_order]\n```\n\n-s only applies to standard output (-o is not supplied). Look in the Stats documentation for valid sort values.\n\nWhen you wish to review the profile, you should use the methods in the pstats module. Typically you would load the statistics data as follows:\n\n```import pstats\np = pstats.Stats('fooprof')\n```\n\nThe class Stats (the above code just created an instance of this class) has a variety of methods for manipulating and printing the data that was just read into `p`. When you ran cProfile.run() above, what was printed was the result of three method calls:\n\n```p.strip_dirs().sort_stats(-1).print_stats()\n```\n\nThe first method removed the extraneous path from all the module names. The second method sorted all the entries according to the standard module/line/name string that is printed. The third method printed out all the statistics. You might try the following sort calls:\n\n```p.sort_stats('name')\np.print_stats()\n```\n\nThe first call will actually sort the list by function name, and the second call will print out the statistics. The following are some interesting calls to experiment with:\n\n```p.sort_stats('cumulative').print_stats(10)\n```\n\nThis sorts the profile by cumulative time in a function, and then only prints the ten most significant lines. If you want to understand what algorithms are taking time, the above line is what you would use.\n\nIf you were looking to see what functions were looping a lot, and taking a lot of time, you would do:\n\n```p.sort_stats('time').print_stats(10)\n```\n\nto sort according to time spent within each function, and then print the statistics for the top ten functions.\n\nYou might also try:\n\n```p.sort_stats('file').print_stats('__init__')\n```\n\nThis will sort all the statistics by file name, and then print out statistics for only the class init methods (since they are spelled with `__init__` in them). As one final example, you could try:\n\n```p.sort_stats('time', 'cum').print_stats(.5, 'init')\n```\n\nThis line sorts statistics with a primary key of time, and a secondary key of cumulative time, and then prints out some of the statistics. To be specific, the list is first culled down to 50% (re: \".5\") of its original size, then only lines containing `init` are maintained, and that sub-sub-list is printed.\n\nIf you wondered what functions called the above functions, you could now (`p` is still sorted according to the last criteria) do:\n\n```p.print_callers(.5, 'init')\n```\n\nand you would get a list of callers for each of the listed functions.\n\nIf you want more functionality, you're going to have to read the manual, or guess what the following functions do:\n\n```p.print_callees()"
]
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https://www.colorhexa.com/04e4c0 | [
"# #04e4c0 Color Information\n\nIn a RGB color space, hex #04e4c0 is composed of 1.6% red, 89.4% green and 75.3% blue. Whereas in a CMYK color space, it is composed of 98.2% cyan, 0% magenta, 15.8% yellow and 10.6% black. It has a hue angle of 170.4 degrees, a saturation of 96.6% and a lightness of 45.5%. #04e4c0 color hex could be obtained by blending #08ffff with #00c981. Closest websafe color is: #00cccc.\n\n• R 2\n• G 89\n• B 75\nRGB color chart\n• C 98\n• M 0\n• Y 16\n• K 11\nCMYK color chart\n\n#04e4c0 color description : Vivid cyan.\n\n# #04e4c0 Color Conversion\n\nThe hexadecimal color #04e4c0 has RGB values of R:4, G:228, B:192 and CMYK values of C:0.98, M:0, Y:0.16, K:0.11. Its decimal value is 320704.\n\nHex triplet RGB Decimal 04e4c0 `#04e4c0` 4, 228, 192 `rgb(4,228,192)` 1.6, 89.4, 75.3 `rgb(1.6%,89.4%,75.3%)` 98, 0, 16, 11 170.4°, 96.6, 45.5 `hsl(170.4,96.6%,45.5%)` 170.4°, 98.2, 89.4 00cccc `#00cccc`\nCIE-LAB 81.464, -54.023, 4.668 37.304, 59.314, 59.349 0.239, 0.38, 59.314 81.464, 54.224, 175.061 81.464, -66.517, 15.608 77.016, -48.317, 8.222 00000100, 11100100, 11000000\n\n# Color Schemes with #04e4c0\n\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #e40428\n``#e40428` `rgb(228,4,40)``\nComplementary Color\n• #04e450\n``#04e450` `rgb(4,228,80)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #0498e4\n``#0498e4` `rgb(4,152,228)``\nAnalogous Color\n• #e45004\n``#e45004` `rgb(228,80,4)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #e40498\n``#e40498` `rgb(228,4,152)``\nSplit Complementary Color\n• #e4c004\n``#e4c004` `rgb(228,192,4)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #c004e4\n``#c004e4` `rgb(192,4,228)``\n• #28e404\n``#28e404` `rgb(40,228,4)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #c004e4\n``#c004e4` `rgb(192,4,228)``\n• #e40428\n``#e40428` `rgb(228,4,40)``\n• #039981\n``#039981` `rgb(3,153,129)``\n• #03b296\n``#03b296` `rgb(3,178,150)``\n• #04cbab\n``#04cbab` `rgb(4,203,171)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #07fbd3\n``#07fbd3` `rgb(7,251,211)``\n• #20fbd8\n``#20fbd8` `rgb(32,251,216)``\n• #39fcdc\n``#39fcdc` `rgb(57,252,220)``\nMonochromatic Color\n\n# Alternatives to #04e4c0\n\nBelow, you can see some colors close to #04e4c0. Having a set of related colors can be useful if you need an inspirational alternative to your original color choice.\n\n• #04e488\n``#04e488` `rgb(4,228,136)``\n• #04e49b\n``#04e49b` `rgb(4,228,155)``\n``#04e4ad` `rgb(4,228,173)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #04e4d3\n``#04e4d3` `rgb(4,228,211)``\n• #04e3e4\n``#04e3e4` `rgb(4,227,228)``\n• #04d0e4\n``#04d0e4` `rgb(4,208,228)``\nSimilar Colors\n\n# #04e4c0 Preview\n\nText with hexadecimal color #04e4c0\n\nThis text has a font color of #04e4c0.\n\n``<span style=\"color:#04e4c0;\">Text here</span>``\n#04e4c0 background color\n\nThis paragraph has a background color of #04e4c0.\n\n``<p style=\"background-color:#04e4c0;\">Content here</p>``\n#04e4c0 border color\n\nThis element has a border color of #04e4c0.\n\n``<div style=\"border:1px solid #04e4c0;\">Content here</div>``\nCSS codes\n``.text {color:#04e4c0;}``\n``.background {background-color:#04e4c0;}``\n``.border {border:1px solid #04e4c0;}``\n\n# Shades and Tints of #04e4c0\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, #00100d is the darkest color, while #fcfffe is the lightest one.\n\n• #00100d\n``#00100d` `rgb(0,16,13)``\n• #01231e\n``#01231e` `rgb(1,35,30)``\n• #01372e\n``#01372e` `rgb(1,55,46)``\n• #014a3e\n``#014a3e` `rgb(1,74,62)``\n• #025d4e\n``#025d4e` `rgb(2,93,78)``\n• #02705f\n``#02705f` `rgb(2,112,95)``\n• #02846f\n``#02846f` `rgb(2,132,111)``\n• #03977f\n``#03977f` `rgb(3,151,127)``\n• #03aa8f\n``#03aa8f` `rgb(3,170,143)``\n• #03bda0\n``#03bda0` `rgb(3,189,160)``\n• #04d1b0\n``#04d1b0` `rgb(4,209,176)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\n• #04f7d0\n``#04f7d0` `rgb(4,247,208)``\n• #14fbd6\n``#14fbd6` `rgb(20,251,214)``\n• #28fbd9\n``#28fbd9` `rgb(40,251,217)``\n• #3bfcdd\n``#3bfcdd` `rgb(59,252,221)``\n• #4efce0\n``#4efce0` `rgb(78,252,224)``\n• #61fce3\n``#61fce3` `rgb(97,252,227)``\n• #75fde7\n``#75fde7` `rgb(117,253,231)``\n• #88fdea\n``#88fdea` `rgb(136,253,234)``\n• #9bfdee\n``#9bfdee` `rgb(155,253,238)``\n• #affef1\n``#affef1` `rgb(175,254,241)``\n• #c2fef4\n``#c2fef4` `rgb(194,254,244)``\n• #d5fef8\n``#d5fef8` `rgb(213,254,248)``\n• #e8fffb\n``#e8fffb` `rgb(232,255,251)``\n• #fcfffe\n``#fcfffe` `rgb(252,255,254)``\nTint Color Variation\n\n# Tones of #04e4c0\n\nA tone is produced by adding gray to any pure hue. In this case, #6f7977 is the less saturated color, while #04e4c0 is the most saturated one.\n\n• #6f7977\n``#6f7977` `rgb(111,121,119)``\n• #66827d\n``#66827d` `rgb(102,130,125)``\n• #5d8b83\n``#5d8b83` `rgb(93,139,131)``\n• #54948a\n``#54948a` `rgb(84,148,138)``\n• #4b9d90\n``#4b9d90` `rgb(75,157,144)``\n• #42a696\n``#42a696` `rgb(66,166,150)``\n• #3aae9c\n``#3aae9c` `rgb(58,174,156)``\n• #31b7a2\n``#31b7a2` `rgb(49,183,162)``\n• #28c0a8\n``#28c0a8` `rgb(40,192,168)``\n• #1fc9ae\n``#1fc9ae` `rgb(31,201,174)``\n• #16d2b4\n``#16d2b4` `rgb(22,210,180)``\n• #0ddbba\n``#0ddbba` `rgb(13,219,186)``\n• #04e4c0\n``#04e4c0` `rgb(4,228,192)``\nTone Color Variation\n\n# Color Blindness Simulator\n\nBelow, you can see how #04e4c0 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"
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https://reference.wolfram.com/language/ref/CoxModel.html | [
"# CoxModel\n\nCoxModel[]\n\nrepresents the symbolic proportional hazards model obtained from CoxModelFit.\n\n# Details and Options",
null,
"• Properties of a Cox model are obtained from CoxModel[][\"property\"].\n• CoxModel[][{prop1,prop2,}] gives several properties.\n• CoxModel[][x0][t] gives the value of the best-fit function at a particular point t for covariate levels x0.\n• Normal gives the expression for the baseline survival function in a CoxModel.\n• CoxModel[][prop,ann] gives the annotation ann associated with the property prop.\n• Possible properties available for a given type of fitted model are listed on the pages for functions such as CoxModelFit that generate the model.\n\n# Examples\n\nopen all close all\n\n## Basic Examples(1)\n\nCreate a CoxModel from some right-censored data:\n\n In:=",
null,
"In:=",
null,
"Out=",
null,
"Extract a property from the model:\n\n In:=",
null,
"Out=",
null,
"Evaluate the baseline survival function at 3:\n\n In:=",
null,
"Out=",
null,
"Use normal to obtain the baseline survival function:\n\n In:=",
null,
"Out=",
null,
"Obtain a list of available properties:\n\n In:=",
null,
"Out=",
null,
"## Scope(5)\n\nIntroduced in 2012\n(9.0)"
]
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/details_1.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/I_2.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/I_4.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/O_2.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/I_8.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/O_3.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/I_10.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/O_4.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/I_12.png",
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"https://reference.wolfram.com/language/ref/Files/CoxModel.en/O_5.png",
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https://richashworth.com/blog/functional-patterns-in-scala-monads/ | [
"",
null,
"Dec 30, 2017 5 min read\n\n# Functional Design Patterns in Scala: 3. Monads",
null,
"Learning (and subsequently trying to explain) monads has become something of a rite of passage in functional programming. Burrito analogies aside, the most helpful description I have come across is given by Noel Welsh and Dave Gurnell in Scala with Cats:\n\n“A monad is a mechanism for sequencing computations.”\n\nMonads provide a pattern for abstracting over the effects of these computations, allowing them to be composed into larger programs. In this post, we will discuss three uses of this pattern: the Writer, Reader, and State monads.\n\nThis pattern provides a means to return a log along with the result of a computation. This is especially useful in multithreaded contexts to avoid the log messages of concurrent computations becoming interleaved. An implementation of the Writer monad is provided in `cats.data.Writer`, which we can use as follows:\n\n``````import cats.data.Writer\nimport cats.instances.vector._\n\nval x = Writer(Vector(\"some intermediary computation\"), 3)\nval y = Writer(Vector(\"another intermediary computation\"), 4)\n\nval z = for {\na <- x\nb <- y\n} yield a + b\n\n// WriterT(Vector(some intermediary computation, another intermediary computation),7)\n``````\n\nWe can access the result and the log separately:\n\n``````println(z.value)\n// 7\n\nprintln(z.written)\n// Vector(some intermediary computation, another intermediary computation)\n``````\n\nA computation wrapped in a `Writer` monad can be executed with the `run` method:\n\n``````val (log, result) = z.run\n``````\n\nThe `cats.syntax.writer` package provides additional syntax for working with Writers, with the `pure` and `tell` methods:\n\n``````import cats.syntax.applicative._\nimport cats.syntax.writer._\n\ntype Logged[A] = Writer[Vector[String], A]\nval writer1 = for {\na <- 10.pure[Logged] // no log\n_ <- Vector(\"a\", \"b\", \"c\").tell // no value, but log still gets appended\nb <- 32.writer(Vector(\"x\", \"y\", \"z\")) // log and value\n} yield a + b // map transforms the result\n\nprintln(writer1)\n// WriterT((Vector(a, b, c, x, y, z),42))\n``````\n\nThe Reader monad provides a functional mechanism for implementing dependency injection. It is particularly useful for passing in a known set of parameters into a program composed of pure functions. Another advantage of using Readers is that each step of a program can be easily tested in isolation.\n\nSuppose we have some configuration, whose structure is given by the following case class:\n\n``````case class Config(name: String, age: Int)\n``````\n\nWe can then say that programs that depend on this configuration are effectively a function from `Config` to some type `A`. We can wrap these functions in the `Reader` monad, so that they can be composed in the usual way using `map` and `flatMap`. In our example, two such ‘programs’ allow us to read a name given in the config object, and perform validation on the configured age:\n\n``````import cats.data.Reader\n\n``````\n\nBecause these programs are both expressed using the Reader monad, we can use them as the building blocks of larger programs (which are themselves Readers). We do this in the below example to construct a greeting from the given config:\n\n``````import cats.syntax.applicative._ // allows us to use `pure`\n\ndef greeting: ConfigReader[String] = for {\ng <- greet(\"Hi\")\na <- validAge\n} yield s\"\\$g; you are \\$p.\"\n``````\n\nThe program can finally be run by supplying a concrete `Config` instance to the `Reader`‘s `run` method.\n\n``````val myCfg = Config(\"Holmes\", -37)\n\nprintln(greeting.run(myCfg))\n// Hi, Mr Holmes; you are an adult.\n``````\n\nPrograms that carry state along with a computation can be expressed in terms of the State monad. For some state `S` and result type `A`, the type `State[S, A]` represents a function that takes an initial state and returns a result together with some new state. In the example below, we will show how a sequence of arithmetic operations can be chained together, passing the result as the state between each step:\n\n``````import cats.data.State\n\ndef addOne = State[Int, String] { state =>\nval a = state + 1\n(a, s\"Result of addOne is \\$a\")\n}\n\ndef double = State[Int, String] { state =>\nval a = state * 2\n(a, s\"Result of double is \\$a\")\n}\n\ndef modTen = State[Int, String] { state =>\nval a = state % 10\n(a, s\"Result of modTen is \\$a\")\n}\n``````\n\nBecause each of these individual steps is wrapped in a monad, we can chain them together using a for-comprehension:\n\n``````def genNumber = for {\na <- addOne // threads the new state to the next computation\nb <- double // threads the new state to the next computation\nc <- modTen\n} yield c\n``````\n\nThe resulting program can then be executed using the `run` method, passing in an initial state:\n\n``````val (state, result) = genNumber.run(3).value\n\nprintln(state)\nprintln(result)\n``````\n\nWe can use the `runA` and `runS` methods to return only the result or state respectively:\n\n``````val resultOnly = genNumber.runA(3)\nval stateOnly = genNumber.runS(3)\n``````\n\n### Summary\n\nWe have seen from the examples in this post that the general concept of a Monad allows us to build different types of sequential programs. The implementations of `flatMap` and `pure` encapsulated in the implementations of Writer, Reader and State handle the mechanics of this composition, allowing us to focus on the business logic within each step of the program. In this sense, we can see Monads as an extremely general pattern for building the more specialised tools that we have examined here."
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https://socratic.org/questions/533eb40a02bf34111b5d6576 | [
"# Question #d6576\n\nNov 21, 2014\n\nKinetic Energy is the energy of motion. An object in motion has a Kinetic Energy which can be calculated from its mass and velocity.\n\n$K E = \\frac{1}{2} m {v}^{2}$\n\nThis can also be thought of as the amount of work that was done on the object to get it up to the velocity $v$. Alternatively, it is the amount of work that will be required to slow the object down from velocity $v$ to rest.\n\nA 1000 kg car traveling down the road at 20 $\\frac{m}{s}$ as a Kinetic Energy\n$K E = \\frac{1}{2} \\cdot 1000 \\cdot {20}^{2} \\frac{k g {m}^{2}}{s} ^ 2 = 200 , 000 J$\n\nTo bring the car to a stop one needs either a large force for a short period of time (hitting a brick wall) or a small force for a longer period of time (imagine sliding on an icy road). The ideal stoping force and distance are somewhere in between, of course. But the amount of Kinetic Energy which must be converted into another form is the same."
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https://electronics.stackexchange.com/questions/501797/4-20-ma-output-from-arduino-for-vfd | [
"# 4-20 mA output from Arduino for VFD\n\nI'm a beginner with electronics, so everything has to be explained in simple terms to me.\n\nI have an Arduino with a program which provides a value via the Analog output, so that is anything from 0-5 V.\n\nOn the other side, I have a VFD with an IO card which allows it to connect to a 4-20 mA current loop, to vary the speed of the motor accordingly.\n\nHow do I convert from, let's say, 0-5 V output (PWM) from Arduino, to the 4-20 mA in a somewhat cheap and safe way (I don't want to destroy the VFD [and possibly the Arduino])?\n\nCurrently, I am using the circuit below:\n\nThe problem is that the simulation on \"Multisim\" is giving accurate results. However practically, the circuit did not give the accurate results.\n\nFor example:\n\n• When V = 5 V output (from Arduino analog), I = 20 mA (V=IR) --> which is correct\n• But, when V = 3.3 V output (from Arduino analog), I = 16 mA (V=IR)--> which is incorrect, as it should be 13 mA\n\nWill this circuit work practically\n\n• If V = 3.3 volts then Iout should be 14.56 mA. I don't know how you got 13 mA. OK you assumed that 1 volts = 4 mA rather than 0 volts is 4 mA. You need to decide this. – Andy aka May 25 at 11:29\n• How it is 14.56mA? Plz Explain – usman shah May 25 at 12:26\n• 0 volts maps to 4 mA and 5 volts maps to 20 mA plus a straight-line graph. – Andy aka May 25 at 12:29\n• Oh! I got it.Thanks – usman shah May 25 at 12:34\n• FOR 1-5V to 0-20mA: I am very confused! When I use 3.3V ouput from Arduino Nano Power Pin--> Iout=13mA (which is ok). But,When I use 3.3V ouput from Arduino Nano Analog pin(PWM)--> Iout=16mA (I can't understand this value). At 2.5V output from Arduino Nano Analog Pin--> Iout=13.7mA. Is seems their is a problem using Analog pins of arduino nano.?? – usman shah May 25 at 13:19"
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https://mailund.dk/posts/c-generators/ | [
"Mailund on the Internet\n\nOn Writing, Science, Programming and more\n\nGenerators in C\n\nNow that I am almost done with The Joys of Hashing, I am looking at the material I made last year for our Genome-scale Algorithms class. I implemented a toy read mapper as an example for the final project. I wrote several different approaches to mapping, from generating all strings at a certain edit distance to a read and doing exact matching to branch-and-bound using BWT.\n\nIn the implementation, there were a few design decisions there that I was never quite happy with. I didn’t have time to fix them, though. We will teach the next class in the spring, and now I have a few weeks to improve the code.\n\nOne thing I particularly disliked with the implementation was the control-flow—several places I need to iterate through reads or matches or such. So, I have functions for that. To combine these iterations with my program, I used callbacks.\n\nThis approach is not a bad idea in some languages. If you have closures, it is a natural approach—you call an iteration algorithm with a closure that does what it does in the scope where you use the iterator.\n\nUnfortunately, I used C, and there are no closures there. That makes it very hard to follow what the program does. So, instead, I wanted something similar to Python’s generators. There, you can write a function that iterates over a sequence of objects and returns control-flow to the caller for each of them, and when called again, continues with the iteration.\n\nYou cannot do this directly in C, but you can wrap the iteration state in a `struct` and use that. It is not unlike how `FILE` pointers are used to work with streams.\n\nI rewrote a couple of functions today to experiment with it.\n\nA simple example is iterating through reads in a FASTQ file. In my implementation from last year, I defined a callback that is called with each read and a function that iterates through a FASTQ file. The interface looks like this:\n\n``````typedef void (*fastq_read_callback_func)(\nconst char *quality,\nvoid * callback_data\n);\n\nvoid scan_fastq(\nFILE *file,\ncallback,\nvoid * callback_data\n);``````\n\nI implemented the function like this:\n\n``````void scan_fastq(\nFILE *file,\nvoid * callback_data\n) {\nchar buffer[MAX_LINE_SIZE];\n\nwhile (fgets(buffer, MAX_LINE_SIZE, file) != 0) {\nchar *name = strtok(buffer+1, \"\\n\");\nfgets(buffer, MAX_LINE_SIZE, file);\nchar *seq = strtok(buffer, \"\\n\");\nfgets(buffer, MAX_LINE_SIZE, file);\nfgets(buffer, MAX_LINE_SIZE, file);\nchar *qual = strtok(buffer, \"\\n\");\n\ncallback(name, seq, qual, callback_data);\n\nfree(name);\nfree(seq);\nfree(qual);\n}\n}``````\n\nTo get a generator instead, I need to wrap the iteration state, and I need a structure to return reads.\n\n``````struct fastq_iter {\nFILE *file;\nchar *buffer;\n};\nstruct fastq_record {\nconst char *name;\nconst char *sequence;\nconst char *quality;\n};``````\n\nI could make the second struct an opaque structure by putting it in the .c file and work with pointers to it in the interface, but so far I have put it in the header so I can allocate iterators on the stack. I expose the structure, but you are not supposed to mess with it—if you do, you will get punished if I change it. So, I might change that design.\n\nAs it stands right now, I have a function that initialises the iterator and one that frees resources from it. They both take the iterator as a parameter.\n\n``````void fastq_init_iter(\nstruct fastq_iter *iter,\nFILE *file\n);\nvoid fastq_dealloc_iter(\nstruct fastq_iter *iter\n);``````\n\nI put the file-stream in the iterator and allocate a buffer for it. Since the file object can be any stream, I do not want to allocate it for the iterator, so I do not touch it when I free iterator resources either. But, of courses, I do need to free the buffer.\n\n``````void fastq_init_iter(\nstruct fastq_iter *iter,\nFILE *file\n) {\niter->file = file;\niter->buffer = malloc(MAX_LINE_SIZE);\n}\n\nvoid fastq_dealloc_iter(\nstruct fastq_iter *iter\n) {\nfree(iter->buffer);\n}``````\n\nTo iterate over reads, I use this function:\n\n``````bool fastq_next_record(\nstruct fastq_iter *iter,\nstruct fastq_record *record\n) {\nFILE *file = iter->file;\nchar *buffer = iter->buffer;\nif (fgets(buffer, MAX_LINE_SIZE, file)) {\nrecord->name = string_copy(strtok(buffer+1, \"\\n\"));\nfgets(buffer, MAX_LINE_SIZE, file);\nrecord->sequence = string_copy(strtok(buffer, \"\\n\"));\nfgets(buffer, MAX_LINE_SIZE, file);\nfgets(buffer, MAX_LINE_SIZE, file);\nrecord->quality = string_copy(strtok(buffer, \"\\n\"));\nreturn true;\n}\nreturn false;\n}``````\n\nIt does the same as the callback function but it uses the iterator for all the state, and it returns `true` when it generates an object—and puts it in the `record` structure. When there are no more objects, it returns `false`.\n\nA simple program that iterates through a file of reads and prints them out again—a specialised `cat` if you will, can look like this:\n\n``````#include <stdlib.h>\n#include <stdio.h>\n#include <fastq.h>\n\nint main(int argc, char *argv[])\n{\nif (argc != 2) {\nprintf(\"needs one argument\\n\");\nreturn EXIT_FAILURE;\n}\n\nFILE *input = fopen(argv, \"r\");\nstruct fastq_iter iter;\nstruct fastq_record record;\nfastq_init_iter(&iter, input);\nwhile (fastq_next_record(&iter, &record)) {\nprintf(\"@%s\\n\", record.name);\nprintf(\"%s\\n\", record.sequence);\nprintf(\"+\\n\");\nprintf(\"%s\\n\", record.quality);\n}\nfastq_dealloc_iter(&iter);\nfclose(input);\n\nreturn EXIT_SUCCESS;\n}``````\n\nExact pattern matching\n\nAnother example of iteration is pattern matching, i.e. finding all occurrences of one string, `pattern`, in another, `text`. I have implemented different algorithms for this. Below I have listed a naive algorithm—one that tries to match the pattern at each index in the text—and the Knuth-Morris-Pratt algorithm. The callback versions have the same interface.\n\n``````typedef void (*match_callback_func)(\nsize_t index,\nvoid * data\n);\n\nvoid naive_exact_match(\nconst char *text, size_t n,\nconst char *pattern, size_t m,\nmatch_callback_func callback,\nvoid *callback_data\n);\nvoid knuth_morris_pratt(\nconst char *text, size_t n,\nconst char *pattern, size_t m,\nmatch_callback_func callback,\nvoid *callback_data\n);``````\n\nThe state in the iterations differs, though. The naive algorithm only needs to know the index in the text we have reached to match a pattern:\n\n``````void naive_exact_match(\nconst char *text, size_t n,\nconst char *pattern, size_t m,\nmatch_callback_func callback,\nvoid *callback_data\n) {\nif (m > n) {\n// This is necessary because n and m are unsigned so the\n// \"j < n - m + 1\" loop test can suffer from an overflow.\nreturn;\n}\n\nfor (size_t j = 0; j <= n - m; j++) {\nsize_t i = 0;\nwhile (i < m && text[j+i] == pattern[i]) {\ni++;\n}\nif (i == m) {\ncallback(j, callback_data);\n}\n}\n}``````\n\nThe KMP algorithm also needs a border array.\n\n``````void knuth_morris_pratt(\nconst char *text, size_t n,\nconst char *pattern, size_t m,\nmatch_callback_func callback,\nvoid *callback_data\n) {\nif (m > n) {\n// This is necessary because n and m are unsigned so the\n// \"j < n - m + 1\" loop test can suffer from an overflow.\nreturn;\n}\n\n// preprocessing\nsize_t prefixtab[m];\nprefixtab = 0;\nfor (size_t i = 1; i < m; ++i) {\nsize_t k = prefixtab[i-1];\nwhile (k > 0 && pattern[i] != pattern[k])\nk = prefixtab[k-1];\nprefixtab[i] = (pattern[i] == pattern[k]) ? k + 1 : 0;\n}\n\n// matching\nsize_t j = 0, q = 0;\nsize_t max_match_len = n - m + 1; // same as for the naive algorithm\n// here we compensate for j pointing q into match\nwhile (j < max_match_len + q) {\nwhile (q < m && text[j] == pattern[q]) {\nq++; j++;\n}\nif (q == m) {\ncallback(j - m, callback_data);\n}\nif (q == 0) {\nj++;\n} else {\nq = prefixtab[q-1];\n}\n}\n}``````\n\nThe generator functions need a structure for returning each match. I could use an integer here, but for consistency, I have used a struct.\n\n``````struct match {\nsize_t pos;\n};``````\n\nThe interface to the two algorithms is the same but since I need more state in the KMP algorithm, the iterator structures differ, so I cannot use the same functions. So, I have these functions for the naive algorithm:\n\n``````struct match_naive_iter {\nconst char *text; size_t n;\nconst char *pattern; size_t m;\nsize_t current_index;\n};\nvoid match_init_naive_iter(\nstruct match_naive_iter *iter,\nconst char *text, size_t n,\nconst char *pattern, size_t m\n);\nbool next_naive_match(\nstruct match_naive_iter *iter,\nstruct match *match\n);\nvoid match_dealloc_naive_iter(\nstruct match_naive_iter *iter\n);``````\n\nAnd I have these functions for KMP.\n\n``````struct match_kmp_iter {\nconst char *text; size_t n;\nconst char *pattern; size_t m;\nsize_t *prefixtab;\nsize_t max_match_len;\nsize_t j, q;\n};\nvoid match_init_kmp_iter(\nstruct match_kmp_iter *iter,\nconst char *text, size_t n,\nconst char *pattern, size_t m\n);\nbool next_kmp_match(\nstruct match_kmp_iter *iter,\nstruct match *match\n);\nvoid match_dealloc_kmp_iter(\nstruct match_kmp_iter *iter\n);``````\n\nI do the sanity test in the iterator initialisation instead of the generators:\n\n``````void match_init_naive_iter(\nstruct match_naive_iter *iter,\nconst char *text, size_t n,\nconst char *pattern, size_t m\n) {\n// This is necessary because n and m are unsigned so the\n// \"j < n - m + 1\" loop test can suffer from an overflow.\nassert(m <= n);\n\niter->text = text; iter->n = n;\niter->pattern = pattern; iter->m = m;\niter->current_index = 0;\n}\n\nvoid match_init_kmp_iter(\nstruct match_kmp_iter *iter,\nconst char *text, size_t n,\nconst char *pattern, size_t m\n) {\n// This is necessary because n and m are unsigned so the\n// \"j < n - m + 1\" loop test can suffer from an overflow.\nassert(m <= n);\n\niter->text = text; iter->n = n;\niter->pattern = pattern; iter->m = m;\niter->j = 0; iter->q = 0;\niter->max_match_len = n - m + 1;\n\niter->prefixtab = malloc(m);\niter->prefixtab = 0;\nfor (size_t i = 1; i < m; ++i) {\nsize_t k = iter->prefixtab[i-1];\nwhile (k > 0 && pattern[i] != pattern[k])\nk = iter->prefixtab[k-1];\niter->prefixtab[i] = (pattern[i] == pattern[k]) ? k + 1 : 0;\n}\n}``````\n\nIn the KMP iterator initialisation, I build the border array as well.\n\nThe function for freeing resources for the naive algorithm does do anything, but I have it for consistency (and in case I need to free something at a later time).\n\n``````void match_dealloc_naive_iter(\nstruct match_naive_iter *iter\n) {\n// nothing to do here...\n}``````\n\nFor the KMP deallocator, I need to free the border array.\n\n``````void match_dealloc_kmp_iter(\nstruct match_kmp_iter *iter\n) {\nfree(iter->prefixtab);\n}``````\n\nWith the iterator states, the generators look precisely like the callback versions.\n\n``````bool next_naive_match(\nstruct match_naive_iter *iter,\nstruct match *match\n) {\nsize_t n = iter->n, m = iter->m;\nconst char *text = iter->text;\nconst char *pattern = iter->pattern;\n\nfor (size_t j = iter->current_index; j <= n - m; j++) {\nsize_t i = 0;\nwhile (i < m && text[j+i] == pattern[i]) {\ni++;\n}\nif (i == m) {\n//callback(j, callback_data);\niter->current_index = j + 1;\nmatch->pos = j;\nreturn true;\n}\n}\n\nreturn false;\n}\n\nbool next_kmp_match(\nstruct match_kmp_iter *iter,\nstruct match *match\n) {\n// aliases to make the code easier to read... but\n// remember to update the actual integers before\n// yielding to the caller...\nsize_t j = iter->j;\nsize_t q = iter->q;\nsize_t m = iter->m;\nsize_t max_match_index = iter->max_match_len;\nconst char *text = iter->text;\nconst char *pattern = iter->pattern;\n\n// here we compensate for j pointing q into match\nwhile (j < max_match_index + q) {\nwhile (q < m && text[j] == pattern[q]) {\nq++; j++;\n}\nif (q == m) {\n// yield\nif (q == 0) j++;\nelse q = iter->prefixtab[q-1];\niter->j = j; iter->q = q;\nmatch->pos = j - m;\nreturn true;\n}\nif (q == 0) {\nj++;\n} else {\nq = iter->prefixtab[q-1];\n}\n}\nreturn false;\n}``````\n\nHandling recursion\n\nTo do approximate matching, I wrote a function that generates all strings at a maximum distance from a pattern. I know that this is a very inefficient approach to approximative matching, but I used it for pedagogical reasons.\n\n``````typedef void (*edits_callback_func)(\nconst char *string,\nconst char *cigar,\nvoid * data\n);\n\nvoid generate_all_neighbours(\nconst char *pattern,\nconst char *alphabet,\nint max_edit_distance,\nedits_callback_func callback,\nvoid *callback_data\n);``````\n\nA natural way to implement the function is using recursion, and I already added a bit of state for that. I do not update most of it, however. I use it mainly to store pointers to buffers I use to generate patterns and CIGAR-strings for the edits. I modify the buffers in the recursion, and the structure keeps the beginning of the buffers so I can use them when reporting a string.\n\nThe code listing below is a bit long, but it is simple enough. I try all edits in the recursion and report a string whenever I reach the base cases of the recursion.\n\n``````struct recursive_constant_data {\nconst char *buffer_front;\nconst char *cigar_front;\nconst char *alphabet;\nchar *simplify_cigar_buffer;\n};\nvoid generate_all_neighbours(\nconst char *pattern,\nconst char *alphabet,\nint max_edit_distance,\nedits_callback_func callback,\nvoid *callback_data\n) {\nsize_t n = strlen(pattern) + max_edit_distance + 1;\nchar buffer[n];\nchar cigar[n], cigar_buffer[n];\nstruct recursive_constant_data data = {\nbuffer, cigar, alphabet, cigar_buffer\n};\nrecursive_generator(\npattern,\nbuffer,\ncigar,\nmax_edit_distance,\n&data,\ncallback,\ncallback_data\n);\n}\n\nstatic void recursive_generator(\nconst char *pattern, char *buffer, char *cigar,\nint max_edit_distance,\nstruct recursive_constant_data *data,\nedits_callback_func callback,\nvoid *callback_data\n) {\nif (*pattern == '\\0') {\n// no more pattern to match ... terminate the buffer and call back\n*buffer = '\\0';\n*cigar = '\\0';\nsimplify_cigar(data->cigar_front, data->simplify_cigar_buffer);\ncallback(data->buffer_front, data->simplify_cigar_buffer, callback_data);\n\n} else if (max_edit_distance == 0) {\n// we can't edit any more, so just move pattern to buffer and call back\nsize_t rest = strlen(pattern);\nfor (size_t i = 0; i < rest; ++i) {\nbuffer[i] = pattern[i];\ncigar[i] = 'M';\n}\nbuffer[rest] = cigar[rest] = '\\0';\nsimplify_cigar(data->cigar_front, data->simplify_cigar_buffer);\ncallback(data->buffer_front, data->simplify_cigar_buffer, callback_data);\n\n} else {\n// --- time to recurse --------------------------------------\n// deletion\n*cigar = 'I';\nrecursive_generator(pattern + 1, buffer, cigar + 1,\nmax_edit_distance - 1, data,\ncallback, callback_data);\n// insertion\nfor (const char *a = data->alphabet; *a; a++) {\n*buffer = *a;\n*cigar = 'D';\nrecursive_generator(pattern, buffer + 1, cigar + 1,\nmax_edit_distance - 1, data,\ncallback, callback_data);\n}\n// match / substitution\nfor (const char *a = data->alphabet; *a; a++) {\nif (*a == *pattern) {\n*buffer = *a;\n*cigar = 'M';\nrecursive_generator(pattern + 1, buffer + 1, cigar + 1,\nmax_edit_distance, data,\ncallback, callback_data);\n} else {\n*buffer = *a;\n*cigar = 'M';\nrecursive_generator(pattern + 1, buffer + 1, cigar + 1,\nmax_edit_distance - 1, data,\ncallback, callback_data);\n}\n}\n}\n}``````\n\nIn the recursion, what I do is this: I create a pattern for all the edits, and then I construct a string that contains all the edits operations. For example, two deletions and two matches will give me the edit string `DDMM`. Yes, it looks strange that two insertions are recorded at two deletions, but this is because the operations are relative to the `text` string and not the `pattern`, so insertions and deletions are switched.\n\nWhat the `simplify_cigar` function does is translating the string with the individual edit operations into a CIGAR string. Maybe the name isn’t that well chosen, but that is what I called it. A better name could be `edits_to_cigar` or something like that. Anyway, in a CIGAR string, two deletions and two matches are recorded as `2D2M`. The function does that translation.\n\n``````void simplify_cigar(const char *cigar, char *buffer)\n{\nwhile (*cigar) {\nconst char *next = scan(cigar);\nbuffer = buffer + sprintf(buffer, \"%lu%c\", next - cigar, *cigar);\ncigar = next;\n}\n*buffer = '\\0';\n}``````\n\nTo handle recursion in an iterator, I need an explicit stack. I use a stack frame structure for this.\n\n``````struct edit_iter_frame;\nstruct edit_iter {\nconst char *pattern;\nconst char *alphabet;\n\nchar *buffer;\nchar *cigar;\nchar *simplify_cigar_buffer;\n\nstruct edit_iter_frame *frames;\n};\nstruct edit_pattern {\nconst char *pattern;\nconst char *cigar;\n};\n\nvoid edit_init_iter(\nstruct edit_iter *iter,\nconst char *pattern,\nconst char *alphabet,\nint max_edit_distance\n);\nbool edit_next_pattern(\nstruct edit_iter *iter,\nstruct edit_pattern *result\n);\nvoid edit_dealloc_iter(\nstruct edit_iter *iter\n);``````\n\nWhere it gets a little complicated is that I need several recursions when in the edit cases. If I had persistent frame data—that is, if I never modified data that would give me side effects—I could push frames to the stack. Unfortunately, that is not the case here. I modify the buffers in the recursions, so the frames I push onto the stack are modified between the push and the pop.\n\nBecause of this, I need to modify the buffers just before I recurse; I cannot push a frame to the stack and handle the frames one a time.\n\nI am not sure this is the most elegant way to handle it, but what I did was this: I split the recursions into two steps. The first generates the recursive calls, and the second modifies the buffers and push a frame to the stack for running the first step recursively.\n\nI defined opcodes for the different operations and structures for storing the state of the operations like this:\n\n``````enum edit_op {\nEXECUTE,\nDELETION,\nINSERTION,\nMATCH\n};\nstruct deletion_info {\n// No extra info\n};\nstruct insertion_info {\nchar a;\n};\nstruct match_info {\nchar a;\n};``````\n\nThe `EXECUTE` operation pushes the different edits to the stack; the other operations modify the state and push the `EXECUTE` operation for the recursions onto the stack.\n\nThe stack frames contain the opcodes, the data associated with them, and the program state I need for each frame:\n\n``````struct edit_iter_frame {\nenum edit_op op;\nunion {\nstruct deletion_info d;\nstruct insertion_info i;\nstruct match_info m;\n} op_data;\n\nconst char *pattern_front;\nchar *buffer_front;\nchar *cigar_front;\nint max_dist;\nstruct edit_iter_frame *next;\n};``````\n\nI wrote a function for pushing stack frames. It doesn’t set the entire state for the frames—I would need separate functions for each operation if I want to add the operation data with the frame. Instead, I will update the frame after I have pushed it. Maybe not that pretty, but that is where I am right now.\n\n``````static struct edit_iter_frame *\npush_edit_iter_frame(\nenum edit_op op,\nconst char *pattern_front,\nchar *buffer_front,\nchar *cigar_front,\nint max_dist,\nstruct edit_iter_frame *next\n) {\nstruct edit_iter_frame *frame =\nmalloc(sizeof(struct edit_iter_frame));\nframe->op = op;\nframe->pattern_front = pattern_front;\nframe->buffer_front = buffer_front;\nframe->cigar_front = cigar_front,\nframe->max_dist = max_dist;\nframe->next = next;\nreturn frame;\n}``````\n\nWhen I initialise the iterator, I push an `EXECUTE` frame to the stack. It will push the first operation-recursions onto the stack when I start the generator.\n\n``````void edit_init_iter(\nstruct edit_iter *iter,\nconst char *pattern,\nconst char *alphabet,\nint max_edit_distance\n) {\nsize_t n = strlen(pattern) + max_edit_distance + 1;\n\niter->pattern = pattern;\niter->alphabet = alphabet;\n\niter->buffer = malloc(n); iter->buffer[n - 1] = '\\0';\niter->cigar = malloc(n); iter->cigar[n - 1] = '\\0';\niter->simplify_cigar_buffer = malloc(n);\n\niter->frames = push_edit_iter_frame(\nEXECUTE,\niter->pattern,\niter->buffer,\niter->cigar,\nmax_edit_distance,\n0\n);\n}``````\n\nWhen I deallocate an iterator, I free the buffers.\n\n``````void edit_dealloc_iter(struct edit_iter *iter)\n{\nfree(iter->buffer);\nfree(iter->cigar);\nfree(iter->simplify_cigar_buffer);\n}``````\n\nNow, for the generator, I report that I am finished when there are no more stack frames. Otherwise, I check if I have reached a base case in the recursion and if so, I report a string. Otherwise, I figure out which operation I need to do in a `switch`. An `EXECUTE` operation means that I need to push the different recursion frames to the stack. The other operations mean I need to update the buffers and then push an `EXECUTE` operation to execute the operation.\n\n``````bool edit_next_pattern(\nstruct edit_iter *iter,\nstruct edit_pattern *result\n) {\nassert(iter);\nassert(result);\n\nif (iter->frames == 0) return false;\n\n// pop top frame\nstruct edit_iter_frame *frame = iter->frames;\niter->frames = frame->next;\n\nconst char *pattern = frame->pattern_front;\nchar *buffer = frame->buffer_front;\nchar *cigar = frame->cigar_front;\n\nif (*pattern == '\\0') {\n// no more pattern to match ... terminate the buffer and call back\n*buffer = '\\0';\n*cigar = '\\0';\nsimplify_cigar(iter->cigar, iter->simplify_cigar_buffer);\nresult->pattern = iter->buffer;\nresult->cigar = iter->simplify_cigar_buffer;\nfree(frame);\nreturn true;\n\n} else if (frame->max_dist == 0) {\n// we can't edit any more, so just move pattern to buffer and call back\nsize_t rest = strlen(pattern);\nfor (size_t i = 0; i < rest; ++i) {\nbuffer[i] = pattern[i];\ncigar[i] = 'M';\n}\nbuffer[rest] = cigar[rest] = '\\0';\nsimplify_cigar(iter->cigar, iter->simplify_cigar_buffer);\nresult->pattern = iter->buffer;\nresult->cigar = iter->simplify_cigar_buffer;\nfree(frame);\nreturn true;\n}\n\nswitch (frame->op) {\ncase EXECUTE:\nfor (const char *a = iter->alphabet; *a; a++) {\niter->frames = push_edit_iter_frame(\nINSERTION,\nframe->pattern_front,\nframe->buffer_front,\nframe->cigar_front,\nframe->max_dist,\niter->frames\n);\niter->frames->op_data.i.a = *a;\niter->frames = push_edit_iter_frame(\nMATCH,\nframe->pattern_front,\nframe->buffer_front,\nframe->cigar_front,\nframe->max_dist,\niter->frames\n);\niter->frames->op_data.m.a = *a;\n}\niter->frames = push_edit_iter_frame(\nDELETION,\nframe->pattern_front,\nframe->buffer_front,\nframe->cigar_front,\nframe->max_dist,\niter->frames\n);\nbreak;\n\ncase DELETION:\n*cigar = 'I';\niter->frames = push_edit_iter_frame(\nEXECUTE,\nframe->pattern_front + 1,\nframe->buffer_front,\nframe->cigar_front + 1,\nframe->max_dist - 1,\niter->frames\n);\nbreak;\n\ncase INSERTION:\n*buffer = frame->op_data.i.a;\n*cigar = 'D';\niter->frames = push_edit_iter_frame(\nEXECUTE,\nframe->pattern_front,\nframe->buffer_front + 1,\nframe->cigar_front + 1,\nframe->max_dist - 1,\niter->frames\n);\n\nbreak;\ncase MATCH:\nif (frame->op_data.m.a == *pattern) {\n*buffer = frame->op_data.m.a;\n*cigar = 'M';\niter->frames = push_edit_iter_frame(\nEXECUTE,\nframe->pattern_front + 1,\nframe->buffer_front + 1,\nframe->cigar_front + 1,\nframe->max_dist,\niter->frames\n);\n} else {\n*buffer = frame->op_data.m.a;\n*cigar = 'M';\niter->frames = push_edit_iter_frame(\nEXECUTE,\nframe->pattern_front + 1,\nframe->buffer_front + 1,\nframe->cigar_front + 1,\nframe->max_dist - 1,\niter->frames\n);\n}\nbreak;\n\ndefault:\nassert(false);\n}\n\nfree(frame);\nreturn edit_next_pattern(iter, result);\n}``````\n\nI have a lot more callback functions to update, but this is how I have gotten this far. What do you think? Do you have suggestions for smarter ways to do this? How do you implement generators in C? I would love to hear from you if you have ideas or experience with this.\n\nIf you liked what you read, and want more like it, consider supporting me at Patreon."
]
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.70550346,"math_prob":0.8763986,"size":22822,"snap":"2019-26-2019-30","text_gpt3_token_len":5921,"char_repetition_ratio":0.17473048,"word_repetition_ratio":0.24100113,"special_character_ratio":0.28174567,"punctuation_ratio":0.17763317,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9643625,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2019-06-17T17:04:39Z\",\"WARC-Record-ID\":\"<urn:uuid:09afc3c6-d23d-4f53-849a-4afebf9da43d>\",\"Content-Length\":\"85389\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:477c392c-9efa-4341-bd27-b8b9b76541dd>\",\"WARC-Concurrent-To\":\"<urn:uuid:b45f4ab8-5ec4-4b0b-9599-92967a1adafd>\",\"WARC-IP-Address\":\"212.242.91.159\",\"WARC-Target-URI\":\"https://mailund.dk/posts/c-generators/\",\"WARC-Payload-Digest\":\"sha1:JMUR3URJGI2SSDKSK3RVVDCTZKRW44DC\",\"WARC-Block-Digest\":\"sha1:PR6UDBKCIQ7VBSTVZ4W4NBYQYSF7Q2SB\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2019/CC-MAIN-2019-26/CC-MAIN-2019-26_segments_1560627998513.14_warc_CC-MAIN-20190617163111-20190617185111-00315.warc.gz\"}"} |
https://edurev.in/question/3264759/If-P-and-Q-be-two-sets-such-that-P-%e2%88%aa-Q-P--then-P-%e2%88%a9-Q-will-beCorrect-answer-is--Q---Can-you-explain-t | [
"If P and Q be two sets such that P ∪ Q = P, ...\n\n### Related Test",
null,
"If P and Q be two sets such that P ∪ Q = P, then P ∩ Q will be:",
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"Kunaal Satija",
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"Intersection\nLet A and B be two sets. The intersection of A and B is the set of all those elements which are present in both sets A and B.\nThe intersection of A and B is denoted by A ∩ B\ni.e., A ∩ B = {x : x ∈ A and x ∈ B}\nThe Venn diagram for intersection is as shown below:",
null,
"Union:\nLet A and B be two sets. The union of A and B is the set of all those elements which belong to either A or B or both A and B.\nThe union of A and B is denoted by A ∪ B.\ni.e., A ∪ B = {x : x ∈ A or x ∈ B}\nThe Venn diagram for the union of any two sets is shown below:",
null,
"A ∪ B = A + B - A ∩ B\nAs we know,\nP ∪ Q = P + Q - P ∩ Q\nPutting the values given in the question,\nP = P + Q - P ∩ Q\nP ∩ Q = Q\nHence, the correct answer is Q.",
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"View courses related to this question Explore CAT courses\n Explore CAT coursesView courses related to this question",
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"1 Crore+ students have signed up on EduRev. Have you?\n\n• ### Directions [Set of 5 questions]: Read the following passage carefully and a... more",
null,
"(Scan QR code)"
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"https://edurev.gumlet.io/cdn_assets/v253/assets/img/stats/test_icon.svg",
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"https://edurev.gumlet.io/cdn_assets/v253/assets/img/vfd_ans_1.webp",
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"https://edurev.gumlet.io/ApplicationImages/Temp/921b4be7-682f-4592-8d26-682cdfb6f82f_lg.png",
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"https://edurev.gumlet.io/ApplicationImages/Temp/cf83b913-d860-4f9b-a95e-c88308a36b5c_lg.png",
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"https://edurev.gumlet.io/cdn_assets/v253/assets/img/explore.svg",
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"https://edurev.gumlet.io/cdn_assets/v253/assets/img/arrow_next_grey.svg",
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https://simplyans.com/mathematics/find-the-values-of-x-and-y-that-mak-14042703 | [
"",
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", 03.12.2019 05:46 allisonlillian\n\n# Find the values of x and y that make these triangles congruent by the hl theorem.",
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"",
null,
"",
null,
"",
null,
"### Another question on Mathematics",
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"Mathematics, 03.02.2019 00:37\nEstimate the area under the curve f(x) = 16 - x^2 from x = 0 to x = 3 by using three inscribed (under the curve) rectangles. answer to the nearest integer.",
null,
"Mathematics, 02.02.2019 22:57\nMe! i will mark you brainliest if you are right and show your i don't get polynomials and all the other stuff. multiply and simplify.2x(^2)y(^3)z(^2) · 4xy(^4)x(^2)show your",
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"Mathematics, 02.02.2019 22:30\nThe expression 1.01*1.005(^t) gives the amount of money, in thousands of dollars, in carter's savings account (t) years after he opens it. what does 1.01 represent in this expression?",
null,
"Mathematics, 01.02.2019 18:53\nMe answer this question: -2/3p + 1/5 - 1 + 5/6p i think the simplified expression is 1/6p - 4/5 correct me if i'm wrong, and explain it! if i have it right, just tell me. you so\nFind the values of x and y that make these triangles congruent by the hl theorem.\n\n...\nQuestions",
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.71584797,"math_prob":0.9671196,"size":1412,"snap":"2020-34-2020-40","text_gpt3_token_len":527,"char_repetition_ratio":0.23011364,"word_repetition_ratio":0.12037037,"special_character_ratio":0.42351276,"punctuation_ratio":0.24933687,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.9955059,"pos_list":[0,1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58],"im_url_duplicate_count":[null,null,null,1,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null,null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-09-19T18:44:37Z\",\"WARC-Record-ID\":\"<urn:uuid:8a296703-c386-4133-a075-2667c725d897>\",\"Content-Length\":\"129049\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:62e30d4f-e6b2-4750-96e9-76a7ce743982>\",\"WARC-Concurrent-To\":\"<urn:uuid:2b149103-bb3e-450a-927c-3e6916c3ce7b>\",\"WARC-IP-Address\":\"64.74.160.240\",\"WARC-Target-URI\":\"https://simplyans.com/mathematics/find-the-values-of-x-and-y-that-mak-14042703\",\"WARC-Payload-Digest\":\"sha1:G7TLKQOIGNIF6VLM7CQE4ZN3BSUKGMYO\",\"WARC-Block-Digest\":\"sha1:KEU7Y74IHK2E2JNJUJCS5ONWTSQIBIZT\",\"WARC-Identified-Payload-Type\":\"text/html\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-40/CC-MAIN-2020-40_segments_1600400192783.34_warc_CC-MAIN-20200919173334-20200919203334-00310.warc.gz\"}"} |
https://discuss.codechef.com/t/help-me-in-solving-flow016-problem/108637 | [
"# Help me in solving FLOW016 problem\n\n### My code\n\n``````#include <stdio.h>\n\nint main(void) {\nint t;\nscanf(\"%d\",&t);\nwhile(t--)\n{\nint a,b;\nscanf(\"%d %d\",&a,&b);\nint gcd,lcm;\nfor(int i=1; i<=(a<b?a:b);i++)\n{\nif(((a%i)==0) && ((b%i)==0))\ngcd=i;\n}\nlcm=(long int)(a*b)/gcd;\nprintf(\"%d %li\\n\",gcd,lcm);\n}\nreturn 0;\n}\n\n``````\n\nProblem Link: FLOW016 Problem - CodeChef\n\nWhat’s wrong in this code?\n\n@sagunsingh\nuse long long int in all but this is also not correct since it will give tle\nso to remove tle u have to find gcd in log(n) time complexity which can be done by using euclidean algorithm\n\nokay, understood\n\nhowever, instead of tle, it is showing that the answer is wrong\n\n@sagunsingh\nhere is the code for reference\ninclude <stdio.h>\nlong long int Gcd(long long int a,long long int b)\n{\n// Everything divides 0\nif (a == 0)\nreturn b;\nif (b == 0)\nreturn a;\n\n``````// Base case\nif (a == b)\nreturn a;\n\n// a is greater\nif (a > b)\nreturn Gcd(a - b, b);\nreturn Gcd(a, b - a);\n``````\n\n}\nint main(void) {\nint t;\nscanf(“%d”,&t);\nwhile(t–)\n{\nlong long int a,b;\nscanf(“%lli %lli”,&a,&b);\nlong long int gcd,lcm;\ngcd=Gcd(a,b);\nlcm=(a*b)/gcd;\nprintf(“%lli %lli\\n”,gcd,lcm);\n}\nreturn 0;\n}\n\n1 Like"
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https://nursingskool.com/determine-the-number-of-moles-for-the-water-of-crystallization-in-copper-sulphate/ | [
"# Determine the Number of Moles for the Water of Crystallization in Copper Sulphate\n\nChange in Potential Energy Worksheet\n1. A 7. 3 kg gallon paint can is lifted 1. 78 meters vertically to a shelf. What is the change in potential energy of the paint can?\n2. A roller coaster car of mass 465 kg rolls up a hill with a vertical height of 75 m from the ground. What is the change in potential energy relative to the ground?\n\n3. If the car in problem #2 starts at rest from the height of 75 m, what will its speed be when it is 5 meters from the ground? What is the change in potential energy relative to the ground? What is the change in kinetic energy relative to the ground?\n4. The same roller coaster car in problem #2 rolls down a vertical height of 40 m from the ground. What is the change in potential energy relative to the ground?\n5. A 783 kg elevator rises straight up 164 meters. What is the change in the potential energy of the elevator relative to the ground?\n6. A car coasts 62. 2 meters along a hill that makes a 28. 3° angle with the ground. If the car’s mass is 1234 kg, then what is the change in potential energy?\n7.\n\nDon't use plagiarized sources. Get Your Custom Essay on\nDetermine the Number of Moles for the Water of Crystallization in Copper Sulphate\nJust from \\$13/Page\n\na) How fast is the bicyclist traveling when she jumps off the ramp 4 m high?\nb) What is the maximum vertical height the bicyclist will reach?\n\n8. What is the highest height Tarzan can travel to given the information above?\n9. What is the jet’s new velocity if it coasts to its new, lower, altitude?\n10. An 80 kg trucker loads a crate as shown below. He pushes the 40 kg box such that his arms are parallel to the ground. He pushes with a 100 N force. How much work is done by the trucker on the box?\n11. A 2800 kg car exerts a constant force of 20,000 N while traveling across 50 m. The car starts from rest.\n\n(a) How much work is done by the car?\n(b) How much power is exerted by the car, in watts?\n\n12. A car 2400 kg is traveling down the road at 26. 1 m/s. If the car accelerates up to 35 m/s over a distance of 200 m then\n\n(a) How much work is done by the car?\n(b) How much power is exerted by the car, in watts?\n\n13. What is the work done over the first 12 meters? What is the power if it is done in 1 minute?\n14. What is the work done over the first 24 meters? What is the power if it is done in 1 hour?\n15. What is the work done over the first 32 meters? What is the power if it is done in 30 minutes?\n16. What is the work done over the first 52 meters? What is the power if it is done in 1200 s?\n17. How much work is done between 32 and 52 meters? What was the change in power if it was\n\nCalculator\n\nTotal price:\\$26\nOur features\n\n## Need a better grade? We've got you covered.\n\nSTAY HOME, SAVE LIVES Order your paper today and save 15% with the discount code SKOOL"
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https://numberworld.info/11904 | [
"# Number 11904\n\n### Properties of number 11904\n\nCross Sum:\nFactorization:\n2 * 2 * 2 * 2 * 2 * 2 * 2 * 3 * 31\nDivisors:\n1, 2, 3, 4, 6, 8, 12, 16, 24, 31, 32, 48, 62, 64, 93, 96, 124, 128, 186, 192, 248, 372, 384, 496, 744, 992, 1488, 1984, 2976, 3968, 5952, 11904\nCount of divisors:\nSum of divisors:\nPrime number?\nNo\nFibonacci number?\nNo\nBell Number?\nNo\nCatalan Number?\nNo\nBase 2 (Binary):\nBase 3 (Ternary):\nBase 4 (Quaternary):\nBase 5 (Quintal):\nBase 8 (Octal):\nBase 32:\nbk0\nsin(11904)\n-0.48418857515349\ncos(11904)\n-0.87496366992626\ntan(11904)\n0.5533813480442\nln(11904)\n9.3846297570729\nlg(11904)\n4.0756929182018\nsqrt(11904)\n109.10545357589\nSquare(11904)\n\n### Number Look Up\n\nLook Up\n\n11904 which is pronounced (eleven thousand nine hundred four) is a very amazing number. The cross sum of 11904 is 15. If you factorisate 11904 you will get these result 2 * 2 * 2 * 2 * 2 * 2 * 2 * 3 * 31. The figure 11904 has 32 divisors ( 1, 2, 3, 4, 6, 8, 12, 16, 24, 31, 32, 48, 62, 64, 93, 96, 124, 128, 186, 192, 248, 372, 384, 496, 744, 992, 1488, 1984, 2976, 3968, 5952, 11904 ) whith a sum of 32640. 11904 is not a prime number. The number 11904 is not a fibonacci number. 11904 is not a Bell Number. The number 11904 is not a Catalan Number. The convertion of 11904 to base 2 (Binary) is 10111010000000. The convertion of 11904 to base 3 (Ternary) is 121022220. The convertion of 11904 to base 4 (Quaternary) is 2322000. The convertion of 11904 to base 5 (Quintal) is 340104. The convertion of 11904 to base 8 (Octal) is 27200. The convertion of 11904 to base 16 (Hexadecimal) is 2e80. The convertion of 11904 to base 32 is bk0. The sine of the number 11904 is -0.48418857515349. The cosine of the figure 11904 is -0.87496366992626. The tangent of the number 11904 is 0.5533813480442. The root of 11904 is 109.10545357589.\nIf you square 11904 you will get the following result 141705216. The natural logarithm of 11904 is 9.3846297570729 and the decimal logarithm is 4.0756929182018. that 11904 is unique number!"
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| {"ft_lang_label":"__label__en","ft_lang_prob":0.7403697,"math_prob":0.9786969,"size":2039,"snap":"2020-34-2020-40","text_gpt3_token_len":756,"char_repetition_ratio":0.17641278,"word_repetition_ratio":0.23255815,"special_character_ratio":0.51005393,"punctuation_ratio":0.1923077,"nsfw_num_words":0,"has_unicode_error":false,"math_prob_llama3":0.99323744,"pos_list":[0],"im_url_duplicate_count":[null],"WARC_HEADER":"{\"WARC-Type\":\"response\",\"WARC-Date\":\"2020-08-11T03:46:18Z\",\"WARC-Record-ID\":\"<urn:uuid:51fbd693-042b-4b6c-8458-290006b3a2f9>\",\"Content-Length\":\"14704\",\"Content-Type\":\"application/http; msgtype=response\",\"WARC-Warcinfo-ID\":\"<urn:uuid:6b399690-66b1-4548-9769-2c419d89bc12>\",\"WARC-Concurrent-To\":\"<urn:uuid:134f42c8-3902-40f1-b0c5-2624cb671a43>\",\"WARC-IP-Address\":\"176.9.140.13\",\"WARC-Target-URI\":\"https://numberworld.info/11904\",\"WARC-Payload-Digest\":\"sha1:OXSAYSPRXHAQQNMU6MIS2VY3KXNBFY3X\",\"WARC-Block-Digest\":\"sha1:U2CHTSVRDQ2OUWGAWB3ZXCTXX6NUAV6A\",\"WARC-Identified-Payload-Type\":\"application/xhtml+xml\",\"warc_filename\":\"/cc_download/warc_2020/CC-MAIN-2020-34/CC-MAIN-2020-34_segments_1596439738727.76_warc_CC-MAIN-20200811025355-20200811055355-00377.warc.gz\"}"} |
https://www.physics.brocku.ca/PPLATO/h-flap/math3_2.html | [
"# 1 Opening items\n\n## 1.1 Module introduction\n\nThe symbol i is defined to have the property that i × i = −1. Expressions involving i, such as 3 + 2i, are known as complex numbers, and they are used extensively to simplify the mathematical treatment of many branches of physics, such as oscillations, waves, a.c. circuits, optics and quantum theory. This module is concerned with the representation of complex numbers in terms of polar coordinates, together with the related exponential representation. Both representations are particularly useful when considering the multiplication and division of complex numbers, and are widely used in physics.\n\nIn Subsection 2.1 we review the Cartesian representation of complex numbers and show how any complex number can be represented as a point on an Argand diagram (the complex plane). We also show how complex numbers can be interpreted as an ordered pair of real numbers. Points in a plane are often specified in terms of their Cartesian coordinates, x and y, but they can equally well be defined in terms of polar coordinates r and θ. It will transpire that, while addition and subtraction of complex numbers is easy for complex numbers in Cartesian form, multiplication and division are usually simplest when the numbers are expressed in terms of polar coordinates. Subsection 2.2 and the subsequent two subsections are concerned with the polar representation of complex numbers, that is, complex numbers in the form r(cosθ + isinθ). Subsection 2.5 introduces the exponential representation, re. Section 3 is devoted to developing the arithmetic of complex numbers and the final subsection gives some applications of the polar and exponential representations which are particularly relevant to physics.\n\nStudy comment Having read the introduction you may feel that you are already familiar with the material covered by this module and that you do not need to study it. If so, try the following Fast track questions. If not, proceed directly to Ready to study? in Subsection 1.3.\n\n## 1.2 Fast track questions\n\nStudy comment Can you answer the following Fast track questions? If you answer the questions successfully you need only glance through the module before looking at the Subsection 4.1Module summary and the Subsection 4.2Achievements. If you are sure that you can meet each of these achievements, try the Subsection 4.3Exit test. If you have difficulty with only one or two of the questions you should follow the guidance given in the answers and read the relevant parts of the module. However, if you have difficulty with more than two of the Exit questions you are strongly advised to study the whole module.\n\nQuestion F1\n\nThe complex number z is defined by z = 1 + i. Find the following in their simplest representations: z, |z|, arg(z), z* and z−1.\n\nWe can write z as\n\n$z = 1 + i = \\sqrt{2\\os}\\left(\\dfrac{1}{\\sqrt{2\\os}}+i\\dfrac{1}{\\sqrt{2\\os}}\\right)$\n\nBut we also know that\n\n$\\cos(\\pi/4) = \\dfrac{1}{\\sqrt{2\\os}}$ and $\\sin(\\pi/4) = \\dfrac{1}{\\sqrt{2\\os}}$\n\nand therefore\n\nz = 2[cos(π/4) + isin(π/4)]\n\nwhich is the polar representation of z.\n\nThe modulus of z is given by |z| = $\\sqrt{2\\os}$. The argument of z is given by arg(z) = π/4. (The argument is undefined up to an additive term of 2πn, where n is any integer.)\n\nThe complex conjugate of z is given by\n\n$z\\cc = \\sqrt{2\\os}[\\cos(\\pi/4) - i\\sin(\\pi/4)]$\n\nThe reciprocal of z is given by\n\n$z^{-1}= \\dfrac{1}{\\sqrt{2\\os}}[\\cos(\\pi/4) - i\\sin(\\pi/4)]$\n\nbecause $z^{-1} = \\dfrac{z\\cc}{\\lvert\\,z\\,\\rvert^2}$\n\nQuestion F2\n\nThe complex numbers z and w are defined by z = 3e/10 and w = 4e/5. Find the simplest exponential representations of zw and z/w.\n\nzw = 3e/10 × 4e/5 = 3 × 4ei(π/10 + π/5) = 12e3/10\n\n$\\dfrac{z}{w} = \\dfrac{3{\\rm e}^{i\\pi/10}}{4{\\rm e}^{i\\pi/5}} = \\dfrac{3}{4}{\\rm e}^{i(\\pi/10-\\pi/5)} = \\dfrac{3}{4}{\\rm e}^{-i\\pi/10}$\n\nQuestion F3\n\nSuppose that a complex quantity, z, is known to satisfy\n\nz = 2 + i + e\n\nwhere θ can take any real value. Sketch a curve on an Argand diagram giving the position of all possible points representing z.",
null,
"All complex numbers which satisfy z = eiθ lie on a circle of radius 1, centre the origin, on an Argand diagram. The additional terms, 2 + i, have the effect of moving the centre to the point representing 2 + i, so the curve on which z = 2 + i + eiθ must lie is shown in Figure 13.\n\nStudy comment Having seen the Fast track questions you may feel that it would be wiser to follow the normal route through the module and to proceed directly to the following Ready to study? Subsection. Alternatively, you may still be sufficiently comfortable with the material covered by the module to proceed directly to the Section 4Closing items.\n\nStudy comment To begin the study of this module you need to be familiar with the following topics: the arithmetic of complex numbers in the form, z = x + iy, where i2 = −1. You should know how to add, subtract and multiply such numbers, be able to reduce the quotient of two complex numbers to rationalizing_a_complex_quotientrational form, to find the modulus_of_a_complex_numbermodulus, complex conjugate, real part and imaginary part of a complex number, and you should know how to plot a complex number on an Argand diagram.\n\nYou should be familiar with the addition of two–dimensional vectors by means of a diagram and by adding their components_of_a_vectorcomponents. You should also be familiar with Pythagoras’s theorem, the definition of sine, cosine and tangent, the measurement of angles in terms of radians and the following trigonometric identities\n\nsin(α + β) = cosαsinβ + sinαcosβ(1)\n\ncos(α + β) = cosαcosβ − sinαsinβ(2)\n\nYou should also know that (n factorial) n! = n(n − 1) ... 3, 2, 1, and 0! = 1. We will need to refer to the following power series for ex, sinx and cosx:\n\n$\\displaystyle {\\rm e}^x = \\sum_{n=0}^{\\infty} \\dfrac{x^n}{n!} = 1 + \\dfrac{x}{1!} + \\dfrac{x^2}{2!} + \\dfrac{x^3}{3!} + \\dots$(3)\n\n$\\displaystyle \\sin x = \\sum_{n=0}^{\\infty} \\dfrac{(-1)^n x^{2n+1}}{(2n+1)!} = x - \\dfrac{x^3}{3!} + \\dfrac{x^5}{5!} - \\dfrac{x^7}{7!} + \\dots$(4)\n\n$\\displaystyle \\cos x = \\sum_{n=0}^{\\infty} \\dfrac{(-1)^n x^{2n}}{(2n)!} = 1 - \\dfrac{x^2}{2!} + \\dfrac{x^4}{4!} - \\dfrac{x^6}{6!} + \\dots$(5)\n\nYou will need to be familiar with the following properties of power_mathematicalpowers (i.e. indices)\n\nuaub = u(a + b), (uv)a = uava, (ua)b = uab(6)\n\nalso to know that the nth root of u can be written as u1/n and to be able to use inverse trigonometric functions to solve an equation such as sinθ = 0.5 for θ (and to use the graph of sinθ, or otherwise, to find all the solutions). If you are unfamiliar with any of these topics you can review them by referring to the Glossary, which will indicate where in FLAP they are developed. The following questions will help you to establish whether you need to review some of the above topics before embarking on this module.\n\nThroughout this module $\\sqrt{x\\os}$ means the positive square root, so that $\\sqrt{4\\os} = 2$.\n\nQuestion R1\n\nRationalize the expression $z = \\dfrac{3 + 2i}{1+2i}$ (i.e. express z in the form x + iy, finding the values of the real numbers x and y). What are the real and imaginary parts of z? Also find the complex conjugate and the modulus of z.\n\nTo rationalize the expression we multiply the denominator and the numerator by the complex conjugate of the denominator\n\n$z = \\dfrac{3 + 2i}{1 + 2i} = \\dfrac{3 + 2i}{1 + 2i} \\times \\dfrac{1 - 2i}{1 - 2i}$\n\n$\\phantom{z }= \\dfrac{(3\\times 1 + 2\\times 2)+i\\,(-2\\times 3 + 2\\times 1)}{1^2+2^2} = \\dfrac{7-4i}{5}$\n\nThe real part of z (often written as Re(z)) is 7/5 and the imaginary part of z (often written as Im(z)) is −4/5. Notice that Im(z) is not equal to −4i/5.\n\nThe complex conjugate of z = x + iy (sometimes written as $\\bar{z}$ but as z* in FLAP) is equal to xiy and so in this case we have\n\n$z\\cc = x - iy = \\dfrac{7+4i}{5}$\n\nThe modulus of z = x + iy (usually written as |z|) is defined by |z| = $\\sqrt{x^2+y^2}$ and therefore we have\n\n$\\lvert\\,z\\,\\rvert = \\sqrt{x^2+y^2} = \\dfrac{\\sqrt{7^2+4^2}}{5} = \\dfrac{\\sqrt{65\\os}}{5} = \\sqrt{13/5\\os} \\approx 1.612$\n\nNote that the modulus of a complex number cannot be negative, i.e. |z| ≥ 0.\n\nConsult the relevant terms in the Glossary for further information.\n\nQuestion R2\n\nDraw and label the points representing the complex numbers −2 + i, −2 − i and −3i on an Argand diagram.",
null,
"The points representing the complex numbers −2 + i, −2 − i and −3i are shown on the Argand diagram in Figure 14.\n\nConsult Argand diagram in the Glossary for further information.",
null,
"Figure 1 See Question R3.\n\nQuestion R3 i\n\nThe equilateral triangle shown in Figure 1 has a perpendicular drawn from one vertex to the opposite side. Use the triangle in Figure 1 to find the values of cos(π/3), sin(π/3), tan(π/3), cos(π/6), sin(π/6) and tan(π/6).\n\nBy Pythagoras’s theorem the length of the perpendicular in Figure 1 is $\\sqrt{2^2-1^2} = \\sqrt{3\\os}$, so we have\n\ncos(π/3) = 1/2, sin(π/3) = $\\sqrt{3\\os}$/2, tan(π/3) = $\\sqrt{3\\os}/1 = \\sqrt{3\\os}$\n\ncos(π/6) = $\\sqrt{3\\os}$/2, sin(π/6) = 1/2, tan(π/6) = 1/$\\sqrt{3\\os}$\n\nConsult Pythagoras’s theorem and trigonometric functions in the Glossary for further information.",
null,
"Figure 2 See Question R4.\n\nQuestion R4 i\n\nUse the right–angled triangle with two sides equal, shown in Figure 2 to find the values of cos(π/4), sin(π/4) and tan(π/4).\n\nBy Pythagoras’s theorem the length of the hypotenuse in Figure 2 is $\\sqrt{1^2+1^2} = \\sqrt{2\\os}$ so we have\n\ncos(π/4) = 1/$\\sqrt{2\\os}$, sin(π/4) = 1/$\\sqrt{2\\os}$, tan(π/4) = 1/1 = 1\n\nConsult inverse trigonometric functions in the Glossary for further information.\n\nQuestion R5\n\nTwo two–dimensional vectors, u and v, are specified in component form as (2, 3) and (1, −4), respectively. Find u + v by (a) drawing a suitable diagram and (b) adding the components directly.",
null,
"(a) The two vectors are shown in Figure 15 and their sum is represented by the third side of the triangle.\n\n(b) The sum of the vectors can also be obtained by adding their components,\n\n(2, 3) + (1, −4) = (2 + 1, 3 −4) = (3, −1)\n\nConsult vector addition in the Glossary for further information.\n\nQuestion R6\n\nSolve the equation tanθ = 1.",
null,
"From Answer R4 we know that θ = π/4 is one solution of the equation tanθ = 1.\n\nHowever, from the graph of y = tanθ (see Figure 16) it is easy to see that π/4 ± is also a solution for any integer n.\n\nConsult inverse trigonometric functions in the Glossary for further information.\n\nQuestion R7\n\nExpress $\\left.\\sqrt{{\\rm e}^{3x}}\\middle /{\\rm e}^x\\right.$ in the form ekx (for some value of k) and hence write down the first three terms of its power series expansion.\n\n$\\left.\\sqrt{{\\rm e}^{3x}}\\middle /{\\rm e}^x\\right. = {\\rm e}^{3x/2} \\times {\\rm e}^{-x} = {\\rm e}^{x/2} = 1 + x/2 + x^2/8 + \\dots$\n\nwhere the power series has been obtained by substituting y = x/2 into the general power series\n\n${\\rm e}^y = 1 + y + \\dfrac{y^2}{2!} + \\dfrac{y^3}{3!} + \\dots$\n\nConsult power series in the Glossary for further information.\n\n# 2 Representing complex numbers\n\n## 2.1 Complex numbers and Cartesian coordinates\n\nA complex number, z, can be written as z = x + iy where x and y are real numbers and i2 = −1. Some examples of complex numbers are 2 + 3i, 7i and 2.4. i\n\nSuch numbers satisfy straightforward rules for addition and subtraction, which essentially mean that the real and imaginary parts are treated separately, so that, for example,\n\n(3 + 4i) + (2 − i) − (−2 − 3i) = (3 + 2 + 2) + (4ii + 3i) = 7 + 6i",
null,
"Figure 3 An Argand diagram showing the point corresponding to a complex number, z = a + ib.",
null,
"Figure 4 An Argand diagram showing the addition of 3 + 2i and 1 + 3i.\n\nMultiplication is quite simple provided that we remember to replace every occurrence of i × i by −1, although a mathematician would probably prefer a formal statement that the product of two complex numbers (a + ib) and (x + iy) is given by\n\n(a + ib)(x + iy) = (axby) + i(ay + bx)(7)\n\nFor a long time the meaning of the symbol i gave many famous mathematicians cause for concern. However, in 1833 Sir William Rowan Hamilton (1805–1865) realized that the i and + sign in z = x + iy are both unnecessary sources of confusion. The role of the i is really to keep the x and y separate, while the + sign is there to tell us that x and y are part of a single entity; it does not mean addition in the sense that we might, for example, add 2 apples to 3 apples to get 5 apples. In fact, the x and y in z = x + iy are very much like the (ordered) pairs of numbers used as Cartesian coordinates. Hamilton’s ideas are closely linked to the those of Robert Argand (1768–1822) and Karl Friedrich Gauss (1777–1855) who both suggested representing a complex number by a point in a plane. As an example, the complex number a + ib is shown on an (x, y) coordinate system in Figure 3; notice that it is conventional that the number multiplying the i corresponds to the y–value. A figure in which the real and imaginary parts of complex numbers are used as Cartesian coordinates is known as an Argand diagram or the complex plane. An expression such as a + ib, where a and b are real numbers, is said to be the cartesian_form_of_a_complex_numberCartesian form (or cartesian_representation_of_a_complex_numberCartesian representation) of a complex number.\n\nIn some mathematics textbooks the authors avoid the problem of the meaning of the symbol i entirely – by not mentioning it – and they introduce the complex numbers as a set of ordered pairs of real numbers (x, y) with certain operations defined on them. Such a treatment has the advantage that complex numbers can immediately be seen to have much in common with vectors. The addition of two complex numbers is then defined by\n\n(x, y) + (a, b) = (x + a, y + b)(8)\n\nwhich is just the same as the rule that defines the addition of two vectors. An example is shown in Figure 4 where the addition of z = 3 + 2i and w = 1 + 3i is performed graphically on an Argand diagram or, equivalently\n\nz + w = (3, 2) + (1, 3) = (4, 5)\n\nQuestion T1\n\nIf z = 4 + 8i and w = 15 − 12i, use an Argand diagram to find the sum, z + w. Check your answer by means of vector addition using the (x, y) notation.",
null,
"The points representing w and z are plotted on the Argand diagram in Figure 17. Lines drawn from the origin to these points can be considered as vectors which define the sides of a parallelogram and the sum of these vectors is a diagonal of this parallelogram. From the diagram we find that z + w is 19 − 4i. This can be checked numerically\n\n(4, 8) + (15, −12) = (19, −4)\n\nAlthough complex numbers behave like vectors as far as addition is concerned, when it comes to multiplication and division the two topics diverge. In terms of ordered pairs of real numbers, multiplication of complex numbers can be defined by i\n\n(a, b) × (x, y) = [(axby), (ay + bx)](9)\n\nAlthough one can introduce complex numbers by this route, which is entirely independent of the symbol i, it must be admitted that Equation 9 looks as though it came out of thin air. In practice i is a very useful notational convenience which makes Equation 9 look much more natural. The i notation is used throughout science and engineering, and even by the purest of pure mathematicians. It is a practice which we follow in FLAP.\n\n## 2.2 Polar coordinates\n\nWe have seen how it is straightforward to interpret complex addition as vector addition on an Argand diagram. In order to investigate the effect of complex multiplication, try the following question.\n\nQuestion T2\n\n(a) Plot the numbers, 1, 2i, −3 −i and 2 − i on an Argand diagram.\n\n(b) Multiply each of the numbers in part (a) by 2 and plot the resulting points on the same diagram. Suggest a geometric interpretation of multiplication by 2 and check your conjecture by finding the effect of multiplying −1 − i by 2.\n\n(c) Repeat parts (a) and (b), but multiply by i instead of 2.\n\n(d) Repeat parts (a) and (b), but multiply by 2i.",
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"",
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"",
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"",
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"(a) The points are plotted on the Argand diagram in Figure 18.\n\n(b) Multiplying each number by 2 gives us\n\n1 × 2 = 2,\n\n2i × 2 = 4i\n\n(−3 −i) × 2 = −6 − 2i,\n\n(2 − i) × 2 = 4 − 2i\n\nThese results are plotted in Figure 19.\n\nYou can see that all points move along a line through the origin to a position twice as far from the origin.\n\nIf we multiply −1 −1i by 2 we find\n\n(−1 −1i) × 2 = −2 − 2i\n\nThis point is plotted in Figure 20 and confirms this conclusion.\n\n(c) Multiplying each number by i we find:\n\n1 × i = i,\n\n2i × i = −2,\n\n(−3 − i) × i = 1 − 3i,\n\n(2 − i) × i = 1 + 2i\n\nLooking at Figure 21 we see that multiplication by i produces a rotation of (π/2) rad in an anticlockwise direction about the origin. This observation is consistent with\n\n(−1 − i) × i = 1− i\n\nwhich is also shown on Figure 21.\n\n(d) Multiplying each number by 2i we obtain:\n\n1 × 2i = 2i,\n\n2i × 2i = −4,\n\n(−3 − i) × 2i = 2 − 6i,\n\n(2 − i) × 2i = 2 + 4i\n\nLooking at Figure 22 we see that multiplication by 2i produces a rotation of (π/2) rad in an anticlockwise direction about the origin. There is also an increase by a factor of 2 in the distance of the points from the origin.\n\nThis observation is consistent with\n\n(−1 − i) × 2i = 2 − 2i\n\nwhich is also shown on Figure 22.",
null,
"Figure 5 Polar coordinates, r, θ.\n\nThe solution to this problem suggests that the geometric interpretation of complex multiplication may involve both a rotation and a change in the distance from the origin, but this is not easy to see if we write complex numbers in the Cartesian form x + iy.\n\nHowever, the geometric properties of complex multiplication are quite evident when the complex numbers are expressed in terms of polar coordinates. Figure 5 shows a point specified by means of polar coordinates; we can see that the ‘distance’ of the point from the origin is called r and θ is the angle between the line from the point to the origin and the x–axis. Notice that r is (by definition) non–negative and that θ is conventionally measured anticlockwise. i\n\nStandard results from trigonometry enable us to express the Cartesian coordinates (x and y) in terms of polar coordinates (r and θ )\n\nx = rcosθ(10)\n\ny = rsinθ(11)\n\nThis means that we can write a complex number, z = x + iy, in the form\n\nz = r(cosθ + isinθ)(12)\n\nwhich is known as the polar_form_of_a_complex_numberpolar form (or polar_representation_of_a_complex_numberpolar representation) of the complex number, z. Examples of complex numbers in polar form are:\n\n2[cos(π/4) + isin(π/4)]\n\n3.5[cos(π/16) + isin(π/16)]\n\nand0.025[cos(1.05) + isin(1.05)]\n\nTo convert a complex number from polar to Cartesian form we can again use Equations 10 and 11.\n\nFor example, z = 3[cos(π/4) + isin(π/4)] has r = 3 and θ = π/4. If we substitute these values into Equations 10 and 11, we find\n\nx = rcosθ = 3cos(π/4) = $\\dfrac{3}{\\sqrt{2\\os}}$ and y = rsinθ = 3sin(π/4) = $\\dfrac{3}{\\sqrt{2\\os}}$\n\ni.e.$z = \\dfrac{3}{\\sqrt{2\\os}} + \\dfrac{3}{\\sqrt{2\\os}}\\,i = \\dfrac{3}{\\sqrt{2\\os}}(1+i)$",
null,
"Figure 6 The complex number, $z = 1 + \\sqrt{3\\os}\\,i$, in terms of polar coordinates.\n\nIt is also straightforward to convert from Cartesian to polar form since the length, r, is given by i\n\n$r = \\sqrt{x^2+y^2}$(13)\n\nand the angle, θ, is such that\n\n$\\cos\\theta = \\dfrac{x}{\\sqrt{x^2+y^2}}$(14)\n\n$\\cos\\theta = \\dfrac{y}{\\sqrt{x^2+y^2}}$(15)\n\nFor example, the complex number, $z = 1 + \\sqrt{3\\os}\\,i$ which has x = 1 and $y = \\sqrt{3\\os}$, can be represented in terms of polar coordinates by\n\n$r = \\sqrt{x^2+y^2} = \\sqrt{1+3\\os} = 2$\n\nand since sin(θ) = $\\dfrac{3}{\\sqrt{2\\os}}$ and cos(θ) = 1/2 we have θ = (π/3) rad. The position of the number $1 + \\sqrt{3\\os}\\,i$ on an Argand diagram is shown in terms of polar coordinates in Figure 6.\n\n✦ The polar coordinates of three points A, B and C are, respectively,\n\nr = 2 θ = (π/4) rad\n\nr = 3 θ = (−π/3) rad\n\nr = 4 θ = (5π/6) rad\n\nExpress the points in Cartesian coordinates.\n\n✧ We can use Equations 10 and 11\n\nx = rcosθ(Eqn 10)\n\ny = rsinθ(Eqn 11)\n\nto convert from polar coordinates to Cartesian coordinates\n\nFor A we have\n\n$x = r\\cos\\theta = 2\\cos(\\pi/4) = 2\\times 1/\\sqrt{2\\os} = \\sqrt{2\\os}$\n\nand$x = r\\sin\\theta = 2\\sin(\\pi/4) = 2\\times 1/\\sqrt{2\\os} = \\sqrt{2\\os}$\n\nFor B\n\n$x = r\\cos\\theta = 3\\cos(\\pi/3) = 3\\times 1/2 = 3/2$\n\nand$x = r\\sin\\theta = -3\\sin(\\pi/3) = -3\\times \\sqrt{3\\os}/2 = -3\\sqrt{3\\os}/2$\n\nFor C\n\n$x = r\\cos\\theta = 4\\cos(5\\pi/6) = -4\\cos(\\pi/6) = -4\\times \\sqrt{3\\os}/2 = -2\\sqrt{3\\os}$\n\nand$x = r\\sin\\theta = 4\\sin(5\\pi/6) = 4\\sin(\\pi/6) = 4\\times 1/2 = 2$\n\nOne big advantage of the polar representation is that the multiplication of complex numbers is easy when they are expressed in this form. To see this, consider two complex numbers, z = x + iy and w = a + ib for which\n\nx = rcosθ and y = rsinθ\n\na = ρcosϕ and b = ρsinϕ\n\nRecalling two results from trigonometry:\n\nsin(α + β) = cosαsinβ + sinαcosβ(Eqn 1) i\n\ncos(α + β) = cosαcosβ − sinαsinβ(Eqn 2)\n\nwe see that the real part of the product zw (see Equation 7) is given by\n\nRe(zw) = axby = ρcosϕ × rcosθρsinϕ × rsinθ\nRe(zw) = ρr(cosθcosϕ − sinθsinϕ)\nRe(zw) = ρrcos(θ + ϕ)\n\nand the imaginary part is given by\n\nIm(zw) = ay + bx = ρcosϕ × rsinθ + ρsinϕ × rcosθ\nIm(zw) = ρr(cosϕsinθ + sinϕcosθ)\nIm(zw) = ρrsin(θ + ϕ)\n\nWe can summarize these two results by the following rule for multiplying complex numbers in polar form:\n\nr(cosθ + isinθ) × ρ(cosϕ + isinϕ) = ρr[cos(θ + ϕ) + isin(θ + ϕ)](16)\n\nSo, multiplying a complex number, w say, by a complex number with a polar representation r(cosθ + isinθ), produces a new complex number which corresponds to the line from the origin to the point representing w being first scaled by a factor r, then the resulting line being rotated anticlockwise about the origin through an angle θ.",
null,
"Figure 9 Complex multiplication causing a rotation and a change in distance from the origin.",
null,
"Figure 8 Complex multiplication causing a rotation.",
null,
"Figure 7 Complex multiplication resulting in a change in distance from the origin.\n\nAs an illustration we will start with the complex number w = 2[cos(π/4) + isin(π/4)] and first multiply it by 2 in Figure 7, then by [cos(π/8) + isin(π/8)] in Figure 8, and finally by 2[cos(π/8) + isin(π/8)] in Figure 9.\n\nNotice that in Figure 9 the line from the origin to the original point is rotated through an angle of (π/8) and the distance from the origin is doubled.\n\n## 2.3 The modulus of a complex number\n\nGiven a complex number, z = x + iy, the modulus_of_a_complex_numbermodulus of z is defined by\n\n$\\lvert\\,z\\,\\rvert = \\sqrt{x^2+y^2}$(17)\n\nIn polar coordinates, where x = rcosθ and y = rsinθ, we have\n\nx2 + y2 = r2cos2θ + r2sin2θ = r2 (because cos2θ + sin2θ = 1)\n\nSo in polar coordinates, the modulus of a complex number is simply the distance from the origin of a point on an Argand diagram. This distance is clearly a non–negative real number.",
null,
"Figure 10 See Question T3.\n\nQuestion T3\n\n(a) Figures 10a and 10b show two complex numbers z1 and z2, respectively. Write z1 and z2 in the x + iy form.\n\n(b) Figures 10c and 10d show two complex numbers z3 and z4, respectively. Calculate the modulus of the complex numbers z3z4.\n\n(a) z1 = 3[cos(7π/6) + isin(7π/6)] = $3\\left(-\\dfrac{\\sqrt{3\\os}}{2}-\\dfrac{i}{2}\\right) = -\\dfrac{3}{2}\\left(\\sqrt{3\\os} + i\\right)$\n\nz2 = 2[cos(−π/3) + isin(−π/3)] = $2\\left(\\dfrac{1}{2}-\\dfrac{i\\sqrt{3\\os}}{2}\\right) = 1 - i\\sqrt{3\\os}$\n\n(b) |z3z4| = 2 × 3.6056 = 7.2112\n\n(by putting ρ = 2 and r = 3.6056 into Equation 16),\n\nr(cosθ + isinθ) × ρ(cosϕ + isinϕ) = ρr[cos(θ + ϕ) + isin(θ + ϕ)](Eqn 16)\n\n## 2.4 The argument of a complex number",
null,
"Figure 6 The complex number,",
null,
"Figure 5 Polar coordinates, r, θ.\n\nIf a complex number is written in polar form as z = r(cosθ + isinθ), then θ is known as the argument of z and is denoted by argument_of_a_complex numberarg(z). For example, if z = 4[cos(π/15) + isin(π/15)] then arg(z) is (π/15) rad which can be interpreted geometrically as follows. Consider a typical point representing a complex number, z, on an Argand diagram such as in Figure 5. Then the angle θ made by the line joining the point to the origin with the positive real axis is the argument. Notice that by convention the angle is measured anticlockwise (so that a negative angle would be measured in a clockwise direction). If z = 1 + $\\sqrt{3\\os}$i then arg(z) is (π/3) rad, as shown in Figure 6.\n\nThere is a slight complication in the definition of the argument since a point, z, on an Argand diagram does not correspond to a single value of arg(z) because we can always add any integer multiple of 2π to the value of θ; in other words, if we rotate the point about the origin through any number of complete turns we always get back to the same point (see Figure 11). i",
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"Figure 11 The non–uniqueness of arg(z) (shown here as θ).\n\nHowever, if we impose the condition that −π < θπ i then θ is uniquely determined, and with this condition θ is known as the principal value of the argument of z. Notice that whereas the lower limit is greater than −π, the upper limit is less than or equal to π. i\n\nIf we have a complex number, z = x + iy, where x and y are not both zero, then the argument, θ, is given by the solution to the following pair of equations\n\n$\\cos\\theta = \\dfrac{x}{\\sqrt{x^2+y^2}}$(18)\n\n$\\sin\\theta = \\dfrac{y}{\\sqrt{x^2+y^2}}$(19)\n\nFrom Equations 18 and 19 we obtain\n\ntanθ = y/x(20)\n\nand while it is possible to use Equation 20 to find the angle θ, this must be done with some care as the following example shows. (Alternatively we can use the Equations 18 and 19, see Solution B to Example 1).\n\n### Example 1\n\nFind the principal value of the argument of the complex number z = −1 + i.\n\n#### Solution A",
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"Figure 12 The complex number, z = −1 + i, plotted on an Argand diagram.\n\nIn this case x = −1 and y = 1, and from Equation 20 we have tanθ = −1. In order to find θ your first thought might be to set your calculator to radian mode and to evaluate arctan(−1), which will give you the approximate value −0.785 398 rad for θ.\n\nHowever, this is not a value of the argument, and certainly not the principal value, as you can easily see if you plot the point −1 + i on an Argand diagram, see Figure 12. The correct answer is approximately 2.356 194 rad (or more precisely (3π/4) rad).\n\nThe essential point to realize here is that Equation 20 does not determine the angle θ uniquely because there are generally two angles in the range −π < θπ that correspond to a given value of the tangent, and these angles differ by π radians. The difficulty is quite easy to resolve if we always draw a diagram (such as Figure 12) when calculating a value for arg(z). In this case we would obtain the value −00.785 398 rad from the calculator as before, then we see from the diagram that we must add π radians to obtain the principal value\n\narg(z) ≈ −0.785 0398 + 3.141 1593 = 2.356 0194 rad\n\nFor this particular value of z you may be able to avoid the use of the calculator if you can see that arg(z) = (3π/4) rad directly from the figure.\n\n#### Solution B\n\nAlternatively we can use Equations 18 and 19 to obtain $\\cos\\theta = -1/\\sqrt{2\\os} \\quad\\text{and}\\quad\\sin\\theta = -1/\\sqrt{2\\os}$. The only angles in the range −π < θπ that satisfy the first equation are θ = (3π/4) rad or θ = (−3π/4) rad, while the only angles that satisfy the second equation are θ = (π/4) rad or θ = (3π/4) rad. Thus the required angle is θ = (3π/4) rad.\n\nNotice that the argument of z = x + iy is not defined when x and y are both zero; in other words, the argument of z = 0 is not defined.\n\nThe polar representation of a complex number is not unique. For example, both $\\sqrt{2\\os}[\\cos(\\pi/4) + i\\,\\sin(\\pi/4)]\\;\\text{and}\\;\\sqrt{2\\os}[\\cos(9\\pi/4) + i\\,\\sin(9\\pi/4)]$ represent the same complex number 1 + i. We can, however, make the representation unique if we insist that the argument takes its principal value. Notice that $-2[\\cos(\\pi/)3 + i\\,\\sin(\\pi/3)]$ is not in polar form. In fact from Equation 16,\n\nr(cosθ + isinθ) × ρ(cosϕ + isinϕ) = ρr[cos(θ + ϕ) + isin(θ + ϕ)](Eqn 16)\n\n−2[cos(π/3) + isin(π/3)] = 2(cosπ + isinπ)[cos(π/3) + isin(π/3)] = 2[cos(4π/3) + isin(4π/3)]\n\nand this final result is in polar form.",
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"Figure 1 See Question R3.\n\nQuestion T4\n\nFor each of the following complex numbers, find the principal value of the argument:\n\n(a) $-1 + \\sqrt{3\\os}\\,i$, (b) 1 - $\\sqrt{3\\os}\\,i$, (c) $\\sqrt{3\\os} + i$, (d) 3 + 2i.\n\n[Hint: You may find Figure 1 helpful.]",
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"You will find it is useful to draw an Argand diagram for such problems.\n\n(a) The position of the point representing $-1 + \\sqrt{3\\os}\\,i$ on an Argand diagram is shown in Figure 23. The angle made by the line joining the point to the origin with the negative real axis is (π/3) rad since cos(π/3) = 1/2. The principal value of arg(z) is the angle made with the positive real axis which we can see from the diagram to be (2π/3) rad.\n\n(b) The position of the point representing $1 - \\sqrt{3\\os}\\,i$ on an Argand diagram is shown in Figure 24. The angle made by the line joining the point to the origin with th positive real axis is (π/3) rad since cos(π/3) = 1/2. The principal value of arg(z) is −π/3 since the angle is measured anticlockwise.\n\n(c) The position of the point representing $\\sqrt{3\\os} + i$ on an Argand diagram is shown in Figure 25. The angle made by the line joining the point to the origin with the positive real axis is (π/6) rad since cos(π/6) = $\\sqrt{3\\os}$/2. This is the principal value of arg(z).\n\n(d) A sketch shows that the complex number 3 + 2i lies in the first\n\ntanθ = y/x(Eqn 20)\n\ntanθ = 2/3. It therefore follows that θ ≈ 0.5880 rad.\n\n## 2.5 The exponential form\n\nYou should be familiar with the following functions, and their series expansions i\n\n$\\displaystyle {\\rm e}^x = \\sum_{n=0}^{\\infty} \\dfrac{x^n}{n!} = 1 + \\dfrac{x}{1!} + \\dfrac{x^2}{2!} + \\dfrac{x^3}{3!} + \\dots$(Eqn 3) i\n\n$\\displaystyle \\sin x = \\sum_{n=0}^{\\infty} \\dfrac{(-1)^n x^{2n+1}}{(2n+1)!} = x - \\dfrac{x^3}{3!} + \\dfrac{x^5}{5!} - \\dfrac{x^7}{7!} + \\dots$(Eqn 4)\n\n$\\displaystyle \\cos x = \\sum_{n=0}^{\\infty} \\dfrac{(-1)^n x^{2n}}{(2n)!} = 1 - \\dfrac{x^2}{2!} + \\dfrac{x^4}{4!} - \\dfrac{x^6}{6!} + \\dots$(Eqn 5)\n\nEach of these functions may be extended so that they apply to a complex variable z (rather than the real variable x), but, since real numbers are just a special case of complex numbers, the new functions must agree with the old ones in the special case when z is real. For example, in order to define ez we simply replace x by z in Equation 3,\n\n$\\displaystyle {\\rm e}^z = \\sum_{n=0}^{\\infty} \\dfrac{z^n}{n!} = 1 + \\dfrac{z}{1!} + \\dfrac{z^2}{2!} + \\dfrac{z^3}{3!} + \\dots$(21) i\n\nNow let us consider the special case of z = , where θ is real and therefore z is imaginary\n\n$\\displaystyle {\\rm e}^{i\\theta} = 1 + \\dfrac{{i\\theta}}{1!} + \\dfrac{({i\\theta})^2}{2!} + \\dfrac{({i\\theta})^3}{3!} + \\dfrac{({i\\theta})^4}{4!} + \\dfrac{({i\\theta})^5}{5!} + \\dots$\n\nThis expression can be simplified by using i2 = −1 to give\n\n$\\displaystyle {\\rm e}^{i\\theta} = 1 + \\dfrac{{i\\theta}}{1!} - \\dfrac{\\theta^2}{2!} + \\dfrac{i\\theta^3}{3!} - \\dfrac{\\theta^4}{4!} + \\dfrac{i\\theta^5}{5!} - \\dots$\n\nWe can see that the terms are alternately real and imaginary, so it is useful to split the series into two\n\n$\\displaystyle {\\rm e}^{i\\theta} = \\left(1 - \\dfrac{\\theta^2}{2!} + \\dfrac{\\theta^4}{4!} - \\dfrac{\\theta^6}{6!} + \\dots\\right) + i\\left(\\dfrac{{\\theta}}{1!} - \\dfrac{\\theta^3}{3!} + \\dfrac{\\theta^5}{5!} - \\dfrac{\\theta^7}{7!} + \\dots\\right)$\n\nIf we compare the right–hand side of this equation with the series for sinθ and cosθ we see that e can be written as\n\ne = cosθ + isinθ (Euler’s formula)(22)\n\nThis important formula, known as Euler’s formula, gives us the real and imaginary parts of e. i\n\nQuestion T5\n\nPlot einπ/8 on an Argand diagram for n = 0, 1, 2, ... 15. What geometrical shape do you think would describe the position of the points representing z = e where θ can take any real value?",
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"There are two ways to answer this question.\n\n(a) Euler’s formula enables us to write\n\nz = enπi/8 = cos(/8) + isin(/8)\n\nThen use a calculator to evaluate the sine and cosine for n = 0, 1, 2, ... 15 and plot the points on an Argand diagram, as in Figure 26. Notice that the points all lie on a circle of radius, 1, with the origin as the centre.\n\nThe following alternative method is somewhat easier.\n\n(b) Notice that if we compare\n\nz = enπi/8 = cos(/8) + isin(/8)\n\nwith the polar form\n\nz = r(cosθ + isinθ)\n\nthen we have r = 1 and arg(z) = /8. The value of r tells us that all points are a distance of 1 from the origin; that is all points lie on a circle of radius 1 centred on the origin. The θ coordinate is the value of arg(z) for each n and points can therefore be plotted directly on the Argand diagram.\n\nThe second approach also shows that all points representing z = e, where θ takes any real value, lie on a circle of radius 1, whose centre is the origin. (This circle is sometimes known as the unit circle.)\n\nIf we put θ = π in Euler’s formula then, since cos(π) = −1 and sin(π) = 0, we find i\n\ne = −1(23)\n\nThis identity is quite remarkable since it relates:\n\n• the numerical constant e, which originates from problems of growth and decay;\n• the numerical constant π, which originates from the ratio of the circumference to the diameter of a circle;\n• the number 1, which has the special property that 1 × n = n for any number n;\n• the symbol i, which has the property i2 = −1 and was originally introduced in order to solve equations such as x2 + 1 = 0.\n\nQuestion T6\n\nUse Euler’s formula to prove the following important relations (Equations 24 and 25):\n\n$\\sin\\theta = \\dfrac{{\\rm e}^{i\\theta} - {\\rm e}^{-i\\theta}}{2i}$(24)\n\n$\\cos\\theta = \\dfrac{{\\rm e}^{i\\theta} + {\\rm e}^{-i\\theta}}{2}$(25)\n\nWe can use Euler’s formula and the fact that cos(−θ) = cosθ and sin(−θ) = −sinθ to obtain\n\ne = cosθ + isinθ\n\ne = cosθisinθ\n\nAddition of the two identities gives e + e = 2cosθ\n\nand therefore\n\n$\\cos\\theta = \\dfrac{{\\rm e}^{i\\theta}+{\\rm e}^{-i\\theta}}{2}$\n\nSubtraction of the two identities gives e − e = 2isinθ\n\n$\\sin\\theta = \\dfrac{{\\rm e}^{i\\theta}-{\\rm e}^{-i\\theta}}{2i}$\n\nNow let us consider a general complex number, z = x + iy, and write it in terms of polar coordinates by substituting x = rcosθ and y = rsinθ\n\nz = x + iy = rcosθ + irsinθ = r(cosθ + isinθ)\n\nwhich can be written more compactly, using Euler’s equation, to obtain\n\nz = re(26)\n\nwhich is known as the exponential_form_of_a_complex_numberexponential form (or exponential_representation_of_a_complex_numberexponential representation) of a complex number. Notice that r is (by definition) non-negative.\n\nQuestion T7\n\nFind the exponential representation for the following complex numbers:\n\n(a) $\\sqrt{2\\os}(1+ i)$, (b) $3(1+ i\\sqrt{3\\os})$, (c) $2(\\sqrt{3\\os} + i)$, (d) 0.2 + 2.3i.",
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"Initially we want to write each number in the form\n\nz = r(cosθ + isinθ)\n\nand we can do this by ensuring that the sum of the squares of the real and imaginary parts within the parentheses is 1. This can be achieved in each case by dividing the complex number in parentheses by its modulus; for example, the complex number (1 + i) has modulus $\\sqrt{2\\os}$ and we therefore write (1 + i) = $\\sqrt{2\\os}\\left(\\dfrac{1}{\\sqrt{2\\os}}+\\dfrac{i}{\\sqrt{2\\os}}\\right)$\n\n(a) $\\sqrt{2\\os}(1+i) = 2\\left(\\dfrac{1}{\\sqrt{2\\os}}+\\dfrac{i}{\\sqrt{2\\os}}\\right)$\n\nThe value of r is 2 and θ is π/4 rad since cos(π/4) = 1/$\\sqrt{2\\os}$ and sin(π/4) = 1/$\\sqrt{2\\os}$. To check these values either use a calculator or, much better, consider a right–angled triangle with two sides of equal length, as in Question R4. So the exponential form is 2e/4.\n\n(b) $3(1+i\\sqrt{3\\os}) = 6\\left(\\dfrac{1}{2}+\\dfrac{i\\sqrt{3\\os}}{2}\\right)$\n\nThe value of r is 6. To obtain θ we need to solve the equations cosθ = 1/2 and sinθ = $\\sqrt{3\\os}$/2, and from Figure 1 (see Question R3) we see that the result is θ = (π/3) rad. So the exponential form is 6e/3.\n\n(c) $2(\\sqrt{3\\os}+i) = 4\\left(\\dfrac{\\sqrt{3\\os}}{2}+\\dfrac{i}{2}+\\right)$\n\nWe have r = 4 and θ is the solution of cosθ = $\\sqrt{3\\os}$/2 and sinθ = 1/2. From Figure 1 (see Question R3) we get θ = (π/6) rad and therefore the exponential form is 4e/6.\n\n(d) The modulus of 0.2 + 2.3i is $\\sqrt{(0.2)^2+(2.3)^2} \\approx 2.309$ and since the point lies in the first quadrant its argument is arctan(2.3/0.2) ≈ 1.484 rad. Hence 0.2 + 2.3i ≈ 2.309e1.484i.\n\n✦ Express the complex numbers i and 2 in exponential form.\n\n✧ From Euler’s formula i = e/2 (because sin(π/2) = 1 and cos(π/2) = 0) and 2 = 2 × 1 = 2ei0 (because sin(0) = 0 and cos(0) = 1).\n\n# 3 Arithmetic of complex numbers\n\n## 3.1 Products and quotients\n\nMultiplication of complex numbers in exponential form is very easy, however in this form addition is more difficult.\n\n### Products\n\nOne important property of real powers of any real quantity is the identity\n\nasat = as + t(27) i\n\nwhich we will assume is also true if any (or all) of the quantities a, s and t are complex. This identity allows us to multiply complex numbers easily in exponential form since, if z = re and w = ρe, then the product is given by\n\nre × ρe = ei(θ + ϕ)(28)\n\nwhich is closely related to the result quoted in Equation 16,\n\nr(cosθ + isinθ) × ρ(cosϕ + isinϕ) = ρr[cos(θ + ϕ) + isin(θ + ϕ)](Eqn 16)\n\nNotice that in Equation 28 the moduli i of the two complex numbers are multiplied whereas the arguments are added (as in Equation 16).\n\nQuestion T8\n\nFind zw in exponential form (choosing the principal value of the argument in each case) for each of the following:\n\n(a) z = 2e/4 w = 2e/4\n\n(b) z = 3e w = 2e/4\n\n(c) z = 2e/16 w = ½ e/16\n\n(a) zw = 2e/4 × 2e/4 = 4e/2\n\n(b) zw = 3e × 2e/4 = 6e5/4 = 6e5/4 × e−2 = 6e−3/4\n\nNotice that we have used the result e−2 = 1 to make the argument of zw consistent with the range −π < arg(zw) ≤ π.\n\n(c) zw = 2e/16 × ½ e/16 = e0 = 1\n\n### Quotients\n\nFor real numbers we have the general result that $\\dfrac{a^m}{b^n} = a^mb^{-n}$ where b is non-zero.\n\nExtending this result to complex numbers, we find that simplifying a quotient of two complex numbers in exponential form is a straightforward variation of multiplication. So if z = re and w = ρe, then z/w is given by $\\dfrac{z}{w} = \\dfrac{r{\\rm e}^{i\\theta}}{\\rho{\\rm e}^{i\\phi}} = \\dfrac{r}{\\rho}{\\rm e}^{i(\\theta-\\phi)}$ that is, we divide the moduli and subtract the arguments.\n\nQuestion T9\n\nFind z/w in exponential form (choosing the principal value of the argument in each case) for each of the following:\n\n(a) z = 2e/4 w = 4e/8\n\n(b) z = 3e/4 w = 2e/2\n\n(c) z = 2e/16 w = 2e/16\n\n(a) $\\dfrac{z}{w} = \\dfrac{2{\\rm e}^{i\\pi/4}}{4{\\rm e}^{-i\\pi/8}} = \\dfrac{1}{2}{\\rm e}^{3i\\pi/8}$\n\n(b) $\\dfrac{z}{w} = \\dfrac{3{\\rm e}^{i\\pi/4}}{2{\\rm e}^{i\\pi/2}} = \\dfrac{3}{2}{\\rm e}^{-i\\pi/4}$\n\n(c) $\\dfrac{z}{w} = \\dfrac{2{\\rm e}^{-i\\pi/16}}{2{\\rm e}^{i\\pi/16}} = {\\rm e}^{-i\\pi/8}$\n\n## 3.2 Sums and differences\n\nSuppose that we are given two complex numbers in exponential form, ae and be, we can certainly write their sum in exponential form\n\nae + be = ce(29) i\n\nbut it is not particularly easy to find the values of c and γ directly. First we will show you a direct method of finding the sum, then an alternative method which is often easier.\n\n### Method 1\n\nTo find c we can write\n\nc2 = (ce)(ce) = (ae + be)(ae + be)\nc2 = a2 + b2 + ab[ei(α − β) + ei(α − β)]\nc2 = a2 + b2 + 2abcos(α − β)\n\nSo we have an equation for c\n\n$c= \\sqrt{\\smash[b]{a^2+b^2+2ab\\cos(\\alpha-\\beta)}}$(30) i\n\nTo find γ we can use Euler’s formula to write e, e and e in polar form, and Equation 29 then becomes\n\na(cosα + isinα) + b(cosβ + isinβ) = c(cosγ + isinγ)\n\nand equating real and imaginary parts gives us:\n\n$\\cos\\gamma = \\dfrac{a\\cos\\alpha + b\\cos\\beta}{c}$\n\n$\\sin\\gamma = \\dfrac{a\\sin\\alpha + b\\sin\\beta}{c}$\n\nSo if we are given a, b, α and β we can first find c, then cosγ and sinγ. Then the condition, −π < γπ uniquely fixes γ.\n\n✦ Given that z = ae = e2/3 and w = be = e/3, find z + w in exponential form.\n\n✧ If z + w = ce\n\nthen c2 = a2 + b2 + 2abcos(αβ)\n\nthen c2 = 12 + 12 + 2 × 1 × 1 × cos(2π/3 − π/3)\n\nthen c2 = 12 + 12 + 2 × 1 ×1 × cos(π/3) = 3\n\nwhich gives $c = \\sqrt{3\\os}$.\n\nThe angle, γ, can be obtained from\n\n$\\cos\\gamma = \\dfrac{a\\cos\\alpha+b\\cos\\beta}{c}$\n\n$\\phantom{\\cos\\gamma }= \\dfrac{\\cos(2\\pi/3)+\\cos(\\pi/3)}{\\sqrt{3\\os}}$\n\n$\\phantom{\\cos\\gamma }= \\dfrac{1}{\\sqrt{3\\os}}\\left(-\\dfrac{1}{2}+\\dfrac{1}{2}\\right) = 0$\n\nand$\\sin\\gamma = \\dfrac{a\\sin\\alpha+b\\sin\\beta}{c}$\n\n$\\phantom{\\cos\\gamma }= \\dfrac{\\sin(2\\pi/3)+\\sin(\\pi/3)}{\\sqrt{3\\os}}$\n\n$\\phantom{\\cos\\gamma }= \\dfrac{1}{\\sqrt{3\\os}}\\left(\\dfrac{\\sqrt{3\\os}}{2}+\\dfrac{\\sqrt{3\\os}}{2}\\right) = 1$\n\nThe only angle γ in the range −π < γπ for which cosγ = 0 and sinγ = 1 is γ = π/2 and therefore\n\ne2/3 + e/3 = 3e/24\n\n### Method 2\n\nThe alternative method of finding the sum in exponential form relies on the fact that addition in Cartesian form is very straightforward. So if z and w are given in exponential form, we first convert them into Cartesian form, then find the sum, and finally convert the answer back into exponential form. We can use the previous example to illustrate the method.\n\nGiven that z = e2/3 and w = e/3, we can use Euler’s formula (Equation 22)\n\ne = cosθ + isinθ(Eqn 22)\n\nto write z and w in Cartesian form\n\n$z = \\dfrac{-1+i}{\\sqrt{3\\os}}{2}$ and $w = \\dfrac{1+i}{\\sqrt{3\\os}}{2}$\n\nfrom which it is straightforward to find the sum\n\n$z + w = \\dfrac{-1+i}{\\sqrt{3\\os}}{2} +\\dfrac{1+i}{\\sqrt{3\\os}}{2} = i\\sqrt{3\\os}$\n\nSince $i\\sqrt{3\\os} = \\sqrt{3\\os}\\,{\\rm e}^{i\\pi/2}$ this result for z + w agrees with our previous result, but you should now be convinced that addition (and subtraction) are much easier using the Cartesian rather than exponential form of complex numbers.\n\nQuestion T10\n\nExpress e − e/2 in exponential form.\n\n${\\rm e}^{i\\pi} - {\\rm e}^{i\\pi/2} = -1 - i = \\sqrt{2\\os}{\\rm e}^{-3i\\pi/4}$\n\nQuestion T11\n\nUse the exponential representation to show that for any complex numbers z1 and z2\n\n|z1| + |z2| ≥ |z1 + z2| i\n\n[Hint: Use Equation 30 and the fact that the cosine of any angle is less than or equal to one.]\n\n$c= \\sqrt{\\smash[b]{a^2+b^2+2ab\\cos(\\alpha-\\beta)}}$(Eqn 30)\n\nWe write z1 and z2 in exponential form as z1 = ae and z2 = be, so we immediately have |z1| + |z2| = a + b. Now let z1 + z2 = ce, then, from Equation 30, we have\n\n$c = \\sqrt{\\smash[b]{a^2+b^2+2ab\\cos(\\alpha-\\beta)}}$(Eqn 30)\n\nBut cos(αβ) ≤ 1, so we have\n\n|z1 + z2| = c ≤ $\\sqrt{a^2+b^2+2ab}$ = a + b = |z1| + |z2|\n\nand therefore |z1| + |z2| ≥ |z1+ z2|.\n\n## 3.3 Powers, roots and reciprocals\n\nThe meaning of an expression such as (1 + 2i)3 is clear enough, i however the meaning of an expression such as (1 + 2i)π is by no means obvious. In this subsection we will attempt to attach a sensible meaning to such expressions. The following results are certainly true for real numbers a and b\n\n(uv)a = uava and (ua)b = uab\n\nand we assume that they also hold for complex numbers. So to raise the complex number z = re to the power α we have\n\nz = (re)α = rαeiαθ(31)\n\nFor example, if z = 2e/4 then\n\nz2 = 4e/2 = 4[cos(π/2) + isin(π/2)] = 4i\n\nWe can check this result by first putting z into Cartesian form\n\nz = 2e/4 = 2[cos(π/4) + isin(π/4)] = $\\dfrac{2}{\\sqrt{2\\os}}(1 + i) = \\sqrt{2\\os}(1+i)$\n\nand then evaluating z2 to give z2 = 2(1 + 2i + i2) = 4i.\n\nQuestion T12\n\nFind z2 and z3, where z = 2e/3. Plot z and z2 and z3 on an Argand diagram and use it to explain the movement of the point representing zn for successive integer values of n.",
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"z2 = (2e/3)2 = 22e2/3 = 4e2/3\n\nz3 = (2e/3)3 = 23e3/3 = −8e3/3 = −8 (since e = −1)\n\nIf we plot the result of multiplying any complex number by z on an Argand diagram, then the distance from the origin will increase by a factor of 2 and the point will rotate about the origin through an angle of (π/3) rad. Therefore multiplying by z2 will increase the distance by a factor of 4 and rotate the point through an angle of (2π/3) rad. This is confirmed by Figure 27.\n\nIt is certainly possible to calculate powers of a complex number in Cartesian form, but it must be done with some care if we are to keep the algebra under control.\n\n✦ Express (1 + i)8 in Cartesian form.\n\n✧ (1 + i)2 = (1 + 2i + i2) = 2i\n\nso that(1 + i)4 = (2i)2 = −4\n\nand(1 + i)8 = (−4)2 = 16.\n\nVery often a better method would be to express the complex number in exponential form, then raise it to the power, and finally convert the answer back into Cartesian form. Using this approach to evaluate (1 + i)8 we have\n\n$(1 + i) = \\sqrt{2\\os}\\,{\\rm e}^{i\\pi/4}$ so that $(1 + i)^8 = (\\sqrt{2\\os}\\,{\\rm e}^{i\\pi/4})^8 = (\\sqrt{2\\os})^8\\,{\\rm e}^{2\\pi i} = 16$\n\nQuestion T13\n\nEvaluate i $(1 + \\sqrt{3\\os}\\,i)^3$ and hence express $(1 + \\sqrt{3\\os}\\,i)^{10}$ in Cartesian form. Also express $z = 1 + \\sqrt{3\\os}\\,i$ in exponential form and use this result to evaluate $(1 + \\sqrt{3\\os}\\,i)^{10}$.\n\nFirst we have $(1 + \\sqrt{3\\os}\\,i)^2 = (1 - 3 + 2\\sqrt{3\\os}\\,i) = -2 + \\sqrt{3\\os}\\,i$\n\nWe then use the result to calculate $(1 + \\sqrt{3\\os}\\,i)^3$\n\n$(1 + \\sqrt{3\\os}\\,i)^3 = (-2 + 2\\sqrt{3\\os}\\,i)(1+ 3i) = -2\\times 1- 2\\times 3+i\\,(-2\\times 3 + 2\\sqrt{3\\os}\\,i\\times 1) = -8$\n\nSo we have\n\n$(1 + \\sqrt{3\\os}\\,i)^{10} = (1 + \\sqrt{3\\os}\\,i)^9(1 + \\sqrt{3\\os}\\,i) = (-8)^3(1 + \\sqrt{3\\os}\\,i) = -512(1 + \\sqrt{3\\os}\\,i)$\n\nNow compare this calculation with the following which uses the exponential form of a complex number.\n\nUsing cos(π/3) = 1/2 and sin(π/3) = $\\sqrt{3\\os}$/2 we have\n\n$z = 1+\\sqrt{3\\os} = {\\rm e}^{i\\pi/3}$\n\nand therefore\n\n$z^{10} = 2^{10}{\\rm e}^{10i\\pi/3} = 2^{10}{\\rm e}^{-2i\\pi/3} = 2^{10}[\\cos(2\\pi/3) -i\\sin(2\\pi/3)]$\n\n$\\phantom{z^{10} }= 2^{10}(-1/2-i\\sqrt{3\\os}/2) = -512(1 + \\sqrt{3\\os}\\,i)$\n\nThis is consistent with the previous method but is a little easier.\n\nQuestion T14\n\nThe complex number, u, is defined by\n\nu = (1.1)e2πi/15\n\nUse an Argand diagram to plot un for n = 1, 2, 3, ... 15. What sort of curve would you expect to get if larger (integer) values of n were plotted and the points joined by a smooth curve?",
null,
"The argument of un is 2πn/15. The point representing un for n = 1 lies on a line from the origin which makes an angle of (2π/15) rad with the positive real axis. For any integer n this angle increases to (2/15) rad.\n\nFor n = 1, the distance of the point from the origin is 1.1, and in general the distance is (1.1)n. The result is the series of points shown in Figure 28. Notice that the points lie on a spiral curve.\n\nThe following example illustrates an area of physics that uses complex numbers.\n\n✦ The propagation constant of a cable carrying an alternating current of angular frequency ω is given by\n\n$\\sigma = \\sqrt{(R+i\\omega L)(G+i\\omega C)\\os}$ i\n\nwhere R, L, G and C are, respectively, the resistance, inductance, conductance and capacitance of the cable i\n\nEvaluate σ if R = 90 Ω, L = 0.002 H, G = 5 × 10−5 S, C = 0.05 × 10−6 F and ω = 5000 s−1.\n\nR + L = 90 Ω + [(5000) × (0.002)i] Ω = (90 + 10i) Ω\n\nG + iωC = [5 × 10−5 + (5000) × (0.05 × 10−6)i] S = (5 + 25i) × 10−5 S\n\nIt follows that\n\n(R + iωL)(G + iωC) = (90 + 10i) Ω × (5 + 25i) × 10−5 Ω−1\n\n(R + iωL)(G + iωC) = (0.2 + 2.3i) × 10−2 ≈ (2.309) e1.484i × 10−2 (see Question T7(d))\n\nTherefore$\\sigma = \\sqrt{(R+i\\omega L)(G+i\\omega C)}$ ≈ [(2.309)e1.484i]1/2 × 10−1 ≈ (0.1519)e0.742i\n\n### Complex powers\n\nThe meaning of a complex power of a complex number becomes clear if we use the exponential, rather than Cartesian, form. For example\n\nz = (e/4)i = eπ/4\n\nQuestion T15\n\nUse suitable exponential representations to reduce the following to simpler (or at least, more familiar) expressions:\n\n(a) ii, (b) $\\left(\\dfrac{1+\\sqrt{3\\os}\\,i}{2}\\right)^i$, (c) $\\left(\\dfrac{1+\\sqrt{3\\os}\\,i}{2}\\right)^{i+1}$.\n\n(a) Using e/2 = cos(π/2) + isin(π/2) = i we obtain\n\nii = (e/2)i = e−π/2\n\nComment There is a deeper side to this question. Since e2πin = 1 for any integer, n, we also have\n\nii = (e/2e2πin)i = eπ/2−2πn\n\nSo ii takes an infinity of values. You may find this surprising, but the nature of the result is similar to the fact that the square root of any positive number takes two values. A complete understanding of such results would take us far beyond the scope of this module and into a subject area known as complex analysis.\n\n(b) Using $1+\\sqrt{3\\os}\\,i = 2{\\rm e}^{i\\pi/3}$ we obtain\n\n$\\left(\\dfrac{1+\\sqrt{3\\os}\\,i}{2}\\right)^i = \\left({\\rm e}^{i\\pi/3}\\right)^i = {\\rm e}^{-\\pi/3}$\n\nAgain, introducing a factor of e2πin would show that there is an infinity of possible results.\n\n(c) $\\left(\\dfrac{1+\\sqrt{3\\os}\\,i}{2}\\right)^{i+1} = \\left({\\rm e}^{i\\pi/3}\\right)^{i+1} = {\\rm e}^{-\\pi/3}{\\rm e}^{i\\pi/3} = {\\rm e}^{-i\\pi/3}[\\cos(\\pi/3)+i\\sin(\\pi/3) = \\frac12{\\rm e}^{-\\pi/3}(1+\\sqrt{3\\os}\\,i)$\n\n### Roots\n\nThe exponential form is also convenient for working out roots of complex numbers since roots are fractional powers. As an example, if we require z1/2, where z = 2e/2, then we can write\n\n$z^{1/2} = 2^{1/2}{\\rm e}^{i\\pi/4} = \\dfrac{\\sqrt{2\\os}\\,(1+i)}{\\sqrt{2\\os}} = 1+i$ i\n\nThis result can be checked by realizing that\n\nz = 2e/2 = 2[cos(π/2) + isin(π/2)] = 2i\n\nand that(z1/2)2 = (1 + i)2 = 1 + 2i + i2 = 2i\n\nQuestion T16\n\nUse a suitable exponential representation to express i1/2 in Cartesian form. Check your answer by means of explicit multiplication.\n\nUsing $i = {\\rm e}^{i\\pi/2}$ we find\n\n$i^{1/2} = \\left({\\rm e}^{i\\pi/2}\\right)^{1/2} = {\\rm e}^{i\\pi/4} = \\dfrac{1+i}{\\sqrt{2\\os}}$\n\nand we can check this result by means of explicit multiplication\n\n$\\left(\\dfrac{1+i}{\\sqrt{2\\os}}\\right)^2 = \\dfrac{1+2i-1}{2} = i$\n\nBecause ${\\rm e}^{2\\pi in} = 1$ for any integer n, there is also another root. Taking n = 1, we have\n\n$i^{1/2} = \\left({\\rm e}^{\\pi i/2}{\\rm e}^{2\\pi i}\\right)^{1/2} = {\\rm e}^{5i\\pi/4} = \\cos(5\\pi/4)+i\\sin(5\\pi/4) = \\dfrac{-1-i}{\\sqrt{2\\os}}$\n\nThis is clearly the previous solution multiplied by −1 and therefore squaring will again give i. It can be shown that other values of n in ${\\rm e}^{2\\pi in}$ do not lead to any new values for i1/2 so that, as one would expect, there are just two distinct values.\n\n### Reciprocals\n\nThe reciprocal i of a complex number is a special case of a power, so, if z = re with r non-zero, we have\n\n$z^{-1} = (r\\,{\\rm e}^{i\\theta})^{-1} = \\dfrac{{\\rm e}^{-i\\theta}}{r}$\n\nFor example, if z = e/3 then z−1 = e/3. We can compare this result with the equivalent calculation using the Cartesian form for z.\n\nSincez = e/3 = $\\dfrac{1+\\sqrt{3\\os}\\,i}{2}$\n\n$z^{-1} = \\dfrac{2}{1+\\sqrt{3\\os}} = \\dfrac{2(1-\\sqrt{3\\os})}{(1+\\sqrt{3\\os})(1-\\sqrt{3\\os})} = \\dfrac{2(1-\\sqrt{3\\os})}{1+3} = \\dfrac{1-\\sqrt{3\\os}}{2} = {\\rm e}^{-i\\pi/3}$\n\nAs you can see, the exponential form provides a somewhat easier method of calculating reciprocals than does the Cartesian form.\n\nQuestion T17\n\nIf z = 2e(i + 1)π/4 what are the exponential and Cartesian forms of z−1?\n\nIf $z = 2{\\rm e}^{(i+1)\\pi/4}$ then\n\n$z^{-1} = \\left[2{\\rm e}^{(i+1)\\pi/4}\\right]^{-1} = \\dfrac{1}{2{\\rm e}^{\\pi/4}}{\\rm e}^{-i\\pi/4}$ (exponential form)\n\n$\\phantom{z^{-1} }= \\dfrac{1}{2{\\rm e}^{\\pi/4}}\\dfrac{(1-i)}{\\sqrt{2\\os}} = \\dfrac{\\sqrt{2\\os}}{4{\\rm e}^{\\pi/4}}(1-i)$ (Cartesian form)\n\n## 3.4 Complex conjugates\n\nThe rule for finding the complex conjugate is to change i to −i, as in\n\n(2 + 3i)* = 2 − 3i\n\nso for any complex number in exponential form, z = re, we have\n\nz* = re(33)\n\nFrom this result we see that the product of any complex number with its complex conjugate is real\n\nzz* = re × re = r2\n\nBut from Subsection 2.3 we know that r is actually the modulus of z, i.e. |z| and so we have the identity\n\nzz* = |z|2 (34)\n\nand therefore, for non–zero values of r, we have\n\n$z^{-1} = r^{-1}\\,{\\rm e}^{-i\\theta} = \\dfrac{r\\,{\\rm e}^{-i\\theta}}{r^2}$\n\nso that\n\n$z^{-1} = \\dfrac{z\\cc}{\\lvert\\,z\\,\\rvert^2}$(35) i\n\nEquation 34 can often be useful if you wish to check that a complicated expression is real and positive (which is often the case in quantum mechanics, for example), for you simply need to recognize that the complicated expression is a product of a complex number with its conjugate. It can also be useful if you wish to establish a result involving moduli (as in the following example).\n\n✦ Show that for any two complex numbers z and w\n\n|z + w|2 + |zw|2 = 2|z|2 + 2|w|2\n\n✧ From Equation 34,\n\nzz* = |z|2(Eqn 34)\n\n|z + w|2 = (z + w)(z* + w*) = zz* + ww* + wz* + zw* |zw|2\n\n|z + w|2 = (zw)(z* − w*) = zz* + ww* − wz* − zw*\n\nand therefore\n\n|z + w|2 + |zw|2 = 2zz* + 2ww* = 2|z|2 + 2|w|2\n\nThe next question establishes some results which you have probably already assumed to be true.\n\nQuestion T18\n\nFor any complex numbers z and w show that:\n\n(a) (zw)* = z*w*, (b) |z−1| = |z|−1, (c) |zw| = |z||w|.\n\n(a) It is certainly possible to establish this result by expressing the complex numbers in Cartesian form as follows:\n\n(zw)* = [(x + iy)(u + iv)]* = [(xuyv) + i(yu + xv)]* = [(xuyv) − i(yu + xv)] = [(xiy)(uiv)] = z*w*\n\nHowever, it is slightly easier to write z = re and w = ρe, then we can write\n\n(zw)* = (reρe)* = [ei(θ + ϕ)]* = [ei(θ + ϕ)] = reρe = z*w*\n\n(b) If we write z = re then we find\n\n|z−1| = |r−1 e| = r−1\n\nand|z|−1 = r−1\n\nand therefore |z−1| = |z|−1\n\nAlternatively, using Equation 35,\n\n$z^{-1} = \\dfrac{z\\cc}{\\lvert\\,z\\,\\rvert^2}$(Eqn 35)\n\nand the fact that |z*| = |z|\n\n$\\lvert\\,z^{-1}\\,\\rvert = \\dfrac{z\\cc}{\\lvert\\,z\\,\\rvert^2} = \\dfrac{\\lvert\\,z\\,\\rvert}{\\lvert\\,z\\,\\rvert^2} = \\lvert\\,z\\,\\rvert^{-1}$\n\n(c) We write z and w in exponential form as re and w = ρe, where r, ρ, θ and ϕ are all real. This means that |z| = r and |w| = ρ, which enables us to write\n\n|zw| = |reρe| = |ei(θ + ϕ)| = = |z||w|\n\nAlternatively:\n\n|zw|2 = (zw)(zw)* = (zz*)(ww*) = |z|2|w|2\n\nand the result follows (because the moduli are positive).\n\n## 3.5 Applications\n\nIn this subsection we consider some applications of the polar and exponential representations which are of particular relevance to physics. You do not need to be familiar with the physics involved.\n\n### Example 2\n\nTwo complex numbers, Z1 and Z2 are\n\nZ1 = 2 + 2i\n\nZ2 = 1 + 2i\n\nIf Z = Z1 + Z2 find |Z| and the principal value of arg(Z). i\n\n#### Solution\n\nZ = (2 + 2i) + (1 + 2i) = 3 + 4i\n\n$\\lvert\\,Z\\,\\rvert = \\sqrt{3^2+4^2} = 5$\n\nIf θ = arg(Z), then sinθ = 4/5 and cosθ = 3/5 which implies that θ ≈ 0.927 rad.\n\n### Example 3\n\nRepeat Example 2 with Z1 and Z2 as before, but this time suppose that Z is given by\n\n$\\dfrac{1}{Z} = \\dfrac{1}{Z_1} + \\dfrac{1}{Z_2}$ i\n\n#### Solution\n\n$Z = \\dfrac{Z_1 Z_2}{Z_1 + Z_2} = \\dfrac{(2+2i)(1+2i)}{3+4i} = \\dfrac{(2-4) +i(2+4)}{3+4i}$\n\n$\\phantom{Z}= \\dfrac{(-2+6i)(3-4i)}{25} = \\dfrac{18+26i}{25}$\n\n$\\lvert\\,Z\\,\\rvert = \\dfrac{\\sqrt{(18)^2+(26)^2}}{25} \\approx 1.26$\n\nIf θ = arg(Z), then\n\n$\\sin\\theta = \\dfrac{26}{\\sqrt{(18)^2+(26)^2}}$ and $\\sin\\theta = \\dfrac{18}{\\sqrt{(18)^2+(26)^2}}$\n\nwhich implies that θ ≈ 0.965 rad.\n\n### Example 4\n\nThe function\n\nf(ϕ) = eimϕ(36)\n\nwhere ϕ is an angle (and therefore real) and m is a real number, occurs in quantum theory. What are the possible values of m, if we require that for every value of ϕ:\n\nf(ϕ) = f(ϕ + 2π)\n\n#### Solution\n\nIf f(ϕ) = f(ϕ + 2π) then\n\neimϕ = eim(ϕ + 2π) = eimϕe2mπi\n\nWe can cancel the factor eimϕ (since it is non-zero) giving\n\ne2imϕ = 1\n\nUsing Euler’s formula, this can be written as\n\ncos(2πm) + isin(2πm) = 1\n\nso thatcos(2πm) = 1 and sin(2πm) = 0\n\nWe recall that cosθ = 1 if θ = 0, ±2π, ±4π, ... and sinθ = 0 if θ = 0, ±π, ±2π, ...\n\nand, since both conditions must apply simultaneously, we have:\n\n2πm = 0, ±2π, ±4π, ...\n\nit therefore follows that:\n\nm = 0, ±1, ±2, ±3, ...\n\nIn other words, the condition f(ϕ) = f(ϕ + 2π) ensures that only integer values of m are acceptable.\n\n### Example 5\n\nGiven that $a = \\dfrac{{\\rm e}^{-i\\phi t}-1}{\\phi}$, with ϕ and t real, show that\n\n$\\lvert\\,a\\,\\rvert^2 = \\dfrac{4}{\\phi^2}\\sin^2\\left(\\dfrac{\\phi t}{2}\\right)$ i\n\n#### Solution\n\nWe could certainly calculate |a|2 by using Equation 35,\n\n$z^{-1} = \\dfrac{z\\cc}{\\lvert\\,z\\,\\rvert^2}$(Eqn 35)\n\nand writing\n\n$\\lvert\\,a\\,\\rvert^2 = \\dfrac{({\\rm e}^{-i\\phi t}-1)({\\rm e}^{i\\phi t}-1)}{\\phi^2}$\n\nand then simplifying the result (using various trigonometric identities); however if you notice that the required expression for |a|2 involves only (ϕt/2) then you might think of the following (more elegant) method.\n\nWe force the expression for a to involve terms in (ϕt/2) by extracting a factor eiϕt/2, so that\n\n$a = \\dfrac{{\\rm e}^{-i\\phi t/2}}{\\phi}\\left({\\rm e}^{-i\\phi t/2} - {\\rm e}^{i\\phi t/2}\\right) = \\dfrac{{\\rm e}^{-i\\phi t/2}}{\\phi}\\left[-2i\\sin\\left(\\dfrac{\\phi t}{2}\\right)\\right] = (-2i)\\left[\\dfrac{\\sin(\\phi t/2)}{\\phi}{\\rm e}^{-i\\phi t/2}\\right]$\n\nIn the right–hand expression, −2i has a modulus of 2, while the term in square brackets is in exponential form\n\nre with $r = \\dfrac{\\sin(\\phi t/2)}{\\phi}$, so it follows that\n\n$\\lvert\\,a\\,\\rvert^2 = \\left[\\dfrac{2}{\\phi}\\sin\\left(\\dfrac{\\phi t}{2}\\right)\\right]^2 = \\dfrac{4}{\\phi^2}\\sin^2\\left(\\dfrac{\\phi t}{2}\\right)$ i\n\n# 4 Closing items\n\n## 4.1 Module summary\n\n1\n\nA complex number is equivalent to an ordered pair of real numbers, (x, y). The addition and subtraction of complex numbers obey the same rules as of two–dimensional vectors\n\n(x, y) + (a, b) = (x + a, y + b)(Eqn 8)\n\nMultiplication of two complex numbers obeys the rule\n\n(a, b) × (x, y) = [(axby), (ay + bx)](Eqn 9)\n\nIn practice, a complex number is more usually written as x + iy with i having the property that i2 = −1.\n\n2\n\nA complex number, z = x + iy, is said to be in Cartesian form or a Cartesian representation.\n\n3\n\nA complex number, z = r(cosθ + isinθ) is said to be in Subsection 2.2polar form or a Subsection 2.2polar representation.\n\nThe polar form r(cosθ + isinθ) of a given complex number z is not unique. However, we can make it so by chosing the principal value of the argument of z, i.e. if −π < θπ. (Note that r = |z| ≥ 0).\n\n4\n\nWe can convert from Cartesian into polar form by using\n\n$r = \\sqrt{x^2+y^2}$(Eqn 13)\n\n$\\cos\\theta = \\dfrac{x}{\\sqrt{x^2+y^2}}$(Eqn 14)\n\n$\\cos\\theta = \\dfrac{y}{\\sqrt{x^2+y^2}}$Eqn (15)\n\nand from polar to Cartesian form by means of x = rcosθ\n\nx = rcosθ(Eqn 10)\n\ny = rsinθ(Eqn 11)\n\n5\n\nA complex number can be represented by a point on an Argand diagram by using (x, y) as the Cartesian coordinates or (r, θ) as the Subsection 2.2polar coordinates of the point. By convention, θ is measured anticlockwise from the positive real axis.\n\n6\n\nIf a complex number is represented by a point on an Argand diagram, then multiplication by z = r(cosθ + isinθ) corresponds to a change in the distance of the point from the origin by a factor of r, together with an anticlockwise rotation through an angle θ.\n\n7\n\nIf a complex number, z, is represented in polar form by z = r(cosθ + isinθ) then the modulus of z is given by |z| = r, and θ is known as the Subsection 2.4argument of z (written as arg(z) ). If z is represented by a point on an Argand diagram then r is the ‘distance’ of the point from the origin and θ is the angle made by a line from the point to the origin with the positive real axis. If θ satisfies −π < θπ, then θ is known as the principal value of the argument of z.\n\n8\n\nEuler’s formula states that\n\ne = cosθ + isinθ(Eqn 22)\n\n9\n\n9 If a complex number, z, is written as z = re, with r ≥ 0, then z is said to be in exponential form or exponential representation. Euler’s formula provides a direct connection between the polar and exponential forms since\n\nre = r(cosθ + isinθ)\n\n10\n\nThe following operations can be carried out on complex numbers in exponential form:\n\nmultiplication\n\nre × ρe = ei(θ + ϕ)\n\nsimplifying quotients\n\n$\\dfrac{r\\,{\\rm e}^{i\\theta}}{\\rho\\,{\\rm e}^{i\\phi}} = \\dfrac{r}{\\rho}{\\rm e}^{i(\\theta-\\phi)}$\n\nfinding real powers\n\n(re)α = rαeiαθ\n\nfinding reciprocals\n\n(re)−1 = r−1e\n\nfinding complex conjugates\n\n(re)* = re\n\nWe may also calculate complex powers of a complex number. The same values apply as for real powers, i.e.\n\nzazb = zab and (za)b = zab\n\nfor complex numbers a, b and z.\n\n11\n\nThe addition and subtraction of complex numbers in either exponential or polar form are complicated in comparison to the same operations on complex numbers in the Cartesian form. Specifically, the sum of ae and be can be written as\n\nae + be = ce(Eqn 29)\n\nwhere$c = \\sqrt{\\smash[b]{a^2+b^2+2ab\\cos(\\alpha-\\beta)}}$(Eqn 30)\n\n$\\cos\\gamma = \\dfrac{a\\cos\\alpha + b\\cos\\beta}{c}$\n\n$\\sin\\gamma = \\dfrac{a\\sin\\alpha + b\\sin\\beta}{c}$\n\nWhere possible, it is better to use the Cartesian form for addition and subtraction.\n\n## 4.2 Achievements\n\nHaving completed this module, you should be able to:\n\nA1\n\nDefine the terms that are emboldened and flagged in the margins of the module.\n\nA2\n\nConvert a complex number between the Cartesian, polar and exponential forms.\n\nA3\n\nRepresent a complex number (in either Cartesian, exponential or polar form) by means of a point on an Argand diagram, and describe geometrically the effect of complex addition or multiplication.\n\nA4\n\nFind the modulus, argument and complex conjugate of complex numbers.\n\nA5\n\nFind powers and reciprocals of complex numbers.\n\nStudy comment You may now wish to take the following Exit test for this module which tests these Achievements. If you prefer to study the module further before taking this test then return to the topModule contents to review some of the topics.\n\n## 4.3 Exit test\n\nStudy comment Having completed this module, you should be able to answer the following questions, each of which tests one or more of the Achievements.\n\nQuestion E1 (A2)\n\nIf Re(z) = 1 and Im(z) = − 3, express z in (a) Cartesian form, (b) polar form using the principal value of the argument, (c) exponential form.\n\n(a) $z = 1 - i\\sqrt{3\\os}$\n\n(b) We have $r = \\sqrt{1+3\\os} = 2$. We also have cosθ = 1/2 and sinθ = −$\\sqrt{3\\os}$/2 and therefore θ = −(π/3) rad.\n\nSo in polar form we have\n\nz = 2[cos(−π/3) + isin(−π/3)]\n\n(c) Using the answer to part (b), together with Euler’s formula, we have z = 2e/3.\n\nQuestion E2 (A2, A4 and A5)\n\nExpress $z = 1 - i\\sqrt{3\\os}$ and w =1 + i in exponential form and use your results to express R in exponential form, where R is given by\n\n$R = \\dfrac{1}{w}\\left(\\dfrac{z}{2}\\right)^{12}$\n\nMake sure that you give the principal value of arg(R).\n\n[Hint: You may find the answers to Questions Question F1F1 and E1 helpful.]\n\nWe have\n\n$z = 1 - i\\sqrt{3\\os} = 2{\\rm e^{-i\\pi/3}}$\n\n$w = 1 + i = \\sqrt{2\\os}{\\rm e}^{+i\\pi/4}$\n\n$R = \\dfrac{1}{w}\\left(\\dfrac{z}{2}\\right)^{12} = \\dfrac{1}{\\sqrt{2\\os}{\\rm e}^{i\\pi/4}}\\left({\\rm e}^{-i\\pi/3}\\right)^{12} = \\dfrac{{\\rm e}^{-i 12\\pi/3}}{\\sqrt{2\\os}}\\rm e{^{i\\pi/4}} = \\dfrac{1}{\\sqrt{2\\os}}{\\rm e}^{-4/pi i}{\\rm e}^{-i/pi} = \\dfrac{1}{\\sqrt{2\\os}}{\\rm e}^{-i\\pi/4}$\n\nNotice that we can factor out multiples of e2πi (since e2πi = 1) in order to ensure that −π < θπ and so obtain the principal value of the argument.\n\n(Reread Subsection 2.4Subsections 2.4, Subsection 2.52.5, Subsection 3.13.1 and Subsection 3.33.3 if you had difficulty with this question.)\n\nQuestion E3 (A3)\n\nIf z is given by\n\n$z = \\dfrac{{\\rm e}^{i\\theta}}{1+\\theta}$\n\nwhere θ can take any non–negative real value, sketch the curve on which any point corresponding to z must lie on an Argand diagram. Justify the main features of the curve.",
null,
"For θ = 0, we have z = 1. As θ increases, the point representing z on an Argand diagram rotates anticlockwise about the origin, with one complete rotation for every change of 2π in θ. The distance of the point from the origin is |z| = (1 + θ)−1, so as θ increases from zero, this distance decreases from 1. As θ becomes very large, the point representing z spirals towards the origin and the resulting curve is shown in Figure 29.\n\n(Reread Subsection 2.2Subsections 2.2 and Subsection 2.42.4 if you had difficulty with this question.)\n\nQuestion E4 (A3)\n\n(a) Show how the addition of complex numbers z = 1 + i and w = 2 + 4i can be considered as vector addition on an Argand diagram.\n\n(b) A complex number z is defined by z = e2πi/n for some fixed positive integer value of n. Show (giving a sketch) how the series\n\n$\\displaystyle S = \\sum_{k=1}^n z^k$\n\ncan be considered as the sum of n vectors on an Argand diagram. Hence determine the value of S.",
null,
"",
null,
"(a) The vector addition of z + w is given on the Argand diagram shown in Figure 30. Therefore we have z = 3 + 5i.\n\n(b) If z = e2πi/n then zk = e2πki/n which is a complex number with modulus 1 and argument 2πk/n. If we define ϕ = 2π/n, then as we add each successive vector it makes an angle, ϕ, with the previous one. Since there are n such vectors, and each is of length 1, we proceed round the sides of a regular polygon, ending back where we started! The result for S is therefore zero. Figure 31 shows the result of adding vectors defined by zk = e2πki/n for the case n = 9. This result can also be shown algebraically since the right–hand side is a geometric series and\n\n$\\displaystyle S = \\sum_{k=1}^n z^k = z + z^2 + \\dots + z^n = \\dfrac{z(1-z^n)}{1-z} = 0$\n\nbecause zn = e2πi = 1.\n\nQuestion E5 (A2)\n\nShow that (−1)n = einπ, where n is any integer.\n\nUsing Euler’s formula we can write\n\neinπ = cos() + isin()\n\nBut sin(ϕ) = 0 for ϕ = 0, ±π, ±2π, ... and so sin() = 0 for n = 0, ±1, ±2, ... . This means that the imaginary part of einπ is zero. We also have cosθ = 1 for θ = 0, ± 2π, ± 4π, ... and cosθ = −1 for θ = 0, ±π, ±3π, ±5π, ... , which shows that cos() = (−1)n. Putting these results together we find (−1)n = einπ.\n\n(Reread Subsection 2.4Subsections 2.4, Subsection 2.52.5 and Subsection 3.33.3 if you had difficulty with this question.)\n\nStudy comment This is the final Exit test question. When you have completed the Exit test go back and try the Subsection 1.2Fast track questions if you have not already done so.\n\nIf you have completed both the Fast track questions and the Exit test, then you have finished the module and may leave it here."
]
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_13.png",
null,
"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_14.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_1.png",
null,
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_18.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_19.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_20.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_21.png",
null,
"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_5.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_6.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_9.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_8.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_7.png",
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null,
"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_6.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_5.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_12.png",
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"https://www.physics.brocku.ca/PPLATO/h-flap/math3_2f_1.png",
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https://www.chemistry4students.com/2018/11/molar-mass.html | [
"-->\n\n# Zumdahl chapter 3: Molar Mass\n\nMolar mass (molecular weight) of a substance is the mass in grams of 1 mole of compound.\nThe molar mass of known substance is obtained by summing the masses of the atoms.\n\nMethane is a molecular compound—its components are molecules. Many substances are ionic—they contain simple ions or polyatomic ions. Examples are NaCl (contains Na⁺ and Cl⁻) and CaCO₃ (contains Ca²⁺ and CO₃²⁻). Because ionic compounds do not contain molecules, we need a special name for the fundamental unit of these materials. Instead of molecule, we use the term formula unit. Thus CaCO₃ is the formula unit for calcium carbonate, and NaCl is the formula unit for sodium chloride."
]
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null
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https://flashgene.com/archives/242185.html | [
"## 1.1 大脑皮层中的局部检测器和平移不变性\n\nNeocognitron模型 [Fukushima 1971-1982]\n\nHMAX模型 [Poggio 2002-2006]\nfragment hierarchy模型 [Ullman 2002-2006]\nHMAX模型 [Lowe 2006]\n\n## 1.3 卷积神经网络(Convolutional neural network, CNN)\n\n输出 (如今我们在池化层很少用激活函数了)\n\n## 2.1 动机:\n\n#### 对于一维\n\n푥 和 푦 两个向量间的 余弦相似度(Cosine Similarity):\n\n#### 对于二维\n\n푥 和 푦 两个矩阵间的余弦相似度(Cosine Similarity):\n\n## 2.2 一维卷积\n\n### 三种卷积形式\n\n푓的长度: 푀, 푔的长度: 푁, 其中 푀 ≥ 푁\n\nValid卷积\n\nFull卷积\n\nSame卷积\n\n#### 例如:\n\nf=[0,1,2,-1,3] g=[1,1,0]\n\npython代码:\n\n```import numpy as np\nfrom scipy import signal\nf = np.array([0, 1, 2, -1, 3])\ng = np.array([1, 1, 0])\nh1 = signal.convolve(f, g, mode='valid')\nh2 = signal.convolve(f, g, mode='full')\nh3 = signal.convolve(f, g, mode='same')```\n\n## 2.3 二维卷积\n\nvalid:h的大小是 (M-K1+1)*(N-K2+1)\nfull:h的大小是 (M+K1-1)*(N+K2-1)\nsame:h的大小是 M*N\n\n#### python例子:\n\n```import numpy\nfrom scipy import signal\nA = numpy.array([[0, 0, 1, 2], [2, 2, 0, 0], [2, 1, 2, 2], [3, 0, 1, 1]])\nB = numpy.array([[0, 0, -1], [1, -1, 1], [-1, 1, 1]])\nC = signal.convolve2d(A, B, mode='full')\nprint(C)\nC = signal.convolve2d(A, B, mode='valid')\nprint(C)\nC = signal.convolve2d(A, B, mode='same')\nprint(C)```\n\n### 卷积核\n\nps:真正用卷积实现关联计算的话,应该先把卷积核翻转180°,再做卷积(因为卷积是交叉计算的),结果是一样的。相当于转了个弯,卷积:直接交叉计算,卷积表示关联计算:旋转再交叉计算。\n\n## 2.4 三维卷积\n\n— 可以通过翻转三维卷积核和三维卷积实现\n\n## 3.3 卷积神经网络的组成与实现\n\n### 组成\n\nSigmoid层, ReLU层, 其它激活层\n\n### 实现\n\n#### 示例:\n\nMNIST手写体数字识别 : ConvNetJS MNIST demo (stanford.edu)\n\nCIFAR-10数据集分类: ConvNetJS CIFAR-10 demo (stanford.edu)\n\n## 四、典型的卷积神经网络\n\n### VGG net\n\n3*3 卷积核被广 泛使用,GPU实现。\n\nRMSProp优化器.\n\nImageNet数据集上的结果"
]
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http://oeis.org/A266829 | [
"The OEIS Foundation is supported by donations from users of the OEIS and by a grant from the Simons Foundation.",
null,
"Hints (Greetings from The On-Line Encyclopedia of Integer Sequences!)\n A266829 Primes p such that a prime q < p exists with p^(q-1) == 1 (mod q^2) and q^(p-1) == 1 (mod p^2), i.e., primes that are the larger member of a double Wieferich prime pair. 5\n 1093, 4871, 18787, 318917, 1006003, 1645333507 (list; graph; refs; listen; history; text; internal format)\n OFFSET 1,1 COMMENTS There are no further terms less than 10^6 (cf. Ernvall, Metsänkylä, 1997, p. 1360). There are no further terms p less than 2^(1/3)*10^10 with p*q <= 10^15 and p and q both odd. (cf. Logan, Mossinghoff, results 4.2.). - Felix Fröhlich, May 29 2016 [Corrected. Felix Fröhlich, Aug 05 2018] Primes that occur in column 2 of A282293. - Felix Fröhlich, Aug 05 2018 LINKS R. Ernvall and T. Metsänkylä, On the p-divisibility of Fermat quotients, Math. Comp., Volume 66, Number 219 (1997), 1353-1365. B. Logan and M. J. Mossinghoff, Double Wieferich pairs and circulant Hadamard matrices, ResearchGate, 2015. MATHEMATICA fQ[p_] := Block[{q = 2}, While[q < p && (PowerMod[p, q - 1, q^2] != 1 || PowerMod[q, p - 1, p^2] != 1), q = NextPrime@ q]; If[q < p, True, False]]; p = 3; lst = {}; While[p < 1000000, If[fQ@ p, AppendTo[lst, p]]; p = NextPrime@ p]; lst (* Robert G. Wilson v, Jan 04 2016 *) PROG (PARI) forprime(p=3, , forprime(q=2, p-1, if(Mod(p, q^2)^(q-1)==1 && Mod(q, p^2)^(p-1)==1, print1(p, \", \"); break({1})))) CROSSREFS Cf. A124122, A282293, A317724 (smallest existing q). Sequence in context: A331021 A270833 A273471 * A203858 A115192 A307220 Adjacent sequences: A266826 A266827 A266828 * A266830 A266831 A266832 KEYWORD nonn,hard,more AUTHOR Felix Fröhlich, Jan 04 2016 EXTENSIONS a(5)-a(6) from Felix Fröhlich, May 29 2016 Removed three comments. - Felix Fröhlich, Aug 21 2018 STATUS approved\n\nLookup | Welcome | Wiki | Register | Music | Plot 2 | Demos | Index | Browse | More | WebCam\nContribute new seq. or comment | Format | Style Sheet | Transforms | Superseeker | Recent\nThe OEIS Community | Maintained by The OEIS Foundation Inc.\n\nLast modified July 14 00:36 EDT 2020. Contains 335716 sequences. (Running on oeis4.)"
]
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"http://oeis.org/banner2021.jpg",
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https://www.freepatentsonline.com/y2006/0063048.html | [
"Title:\nOptimal temperature tracking for necessary and accurate thermal control of a fuel cell system\nKind Code:\nA1\n\nAbstract:\nA temperature control scheme for a fuel cell stack thermal sub-system in a fuel cell system. The thermal sub-system includes a coolant loop directing the cooling fluid through the stack, a pump for pumping the cooling fluid through the coolant loop, a radiator for cooling the cooling fluid outside of the fuel cell stack and a bypass valve for selectively directing the cooling fluid in the coolant loop through the radiator or around the radiator. The control scheme generates an optimal model of the thermal sub-system using non-linear equations, and controls the speed of the pump and a position of the bypass valve in combination.\n\nInventors:\nKolodziej, Jason R. (West Henrietta, NY, US)\nApplication Number:\n10/948402\nPublication Date:\n03/23/2006\nFiling Date:\n09/23/2004\nExport Citation:\nPrimary Class:\nOther Classes:\n429/452, 429/442\nInternational Classes:\nH01M8/04\nView Patent Images:\nRelated US Applications:\n 20060057463 Composite materials of nano-dispersed silicon and tin and methods of making the same March, 2006 Gao et al. 20050034905 Industrial truck with an electrical drive, a fuel cell system and a heating device for an operator's position February, 2005 Gunther et al. 20090000837 SADDLE RIDING TYPE FUEL CELL VEHICLE January, 2009 Horii et al. 20060240315 Vent valve for acid batteries October, 2006 Imhof et al. 20100003556 PLASMA-CATALYZED FUEL REFORMER January, 2010 Hartvigsen et al. 20070253875 Hydrogen supply for micro fuel cells November, 2007 Koripella et al. 20050266300 Electrical energy supply methods and electrical energy power supplies December, 2005 Lamoreux et al. 20070077481 Metallic structures for solid oxide fuel cells April, 2007 Chatterjee et al. 20050039959 Vehicle with an air-conditioning system and a heat source February, 2005 Fruhauf et al. 20050136325 Sealed prismatic battery June, 2005 Fujihara et al. 20090068535 FUEL CELL BIPOLAR PLATE EXIT FOR IMPROVED FLOW DISTRIBUTION AND FREEZE COMPATIBILITY March, 2009 Owejan et al.\n\nPrimary Examiner:\nALEJANDRO, RAYMOND\nAttorney, Agent or Firm:\nMILLER IP GROUP, PLC (BLOOMFIELD HILLS, MI, US)\nClaims:\nWhat is claimed is:\n\n1. A method for controlling the temperature of a fuel cell stack in a fuel cell system, said fuel cell system including a coolant loop directing a cooling fluid through the stack, a pump for pumping the cooling fluid through the coolant loop, a radiator for cooling the cooling fluid outside of the stack and a bypass valve for selectively directing the cooling fluid in the coolant loop through the radiator or around the radiator, said method comprising: determining a first matrix that is representative of the temperature of the cooling fluid coming out of the stack and the temperature of the cooling fluid coming out of the radiator; determining a second matrix based on a desired temperature set-point of the fuel cell stack; determining a third matrix based on the output power of the fuel cell stack; and generating a control matrix for controlling the speed of the pump and the position of the bypass valve by combining the first, second and third matrices.\n\n2. The method according to claim 1 wherein determining the first matrix includes calculating the first matrix based on a state matrix that defines the physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an output matrix that defines variables being measured, a matrix tuned to a desired response and an R matrix.\n\n3. The method according to claim 2 wherein determining the first matrix includes calculating the first matrix as:\n0=−KA−ATK+KBR−1BTK−CTQC, where K is the first matrix, A is the state matrix that defines the physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, C is the output matrix that defines variables being measured and Q is the matrix tuned to a desired response.\n\n4. The method according to claim 1 wherein determining a second matrix includes calculating the second matrix based on a state matrix that defines physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an output matrix that defines variables being measured and a matrix tuned to a desired response.\n\n5. The method according to claim 4 wherein determining a second matrix includes calculating the second matrix as:\nh=(BR−1BT−AT)−1CTQZ, where h is the second matrix, A is the state matrix that defines physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, C is the output matrix that defines variables being measured, Q is the matrix tuned to a desired response, and z is the desired temperature set-point of the fuel cell stack.\n\n6. The method according to claim 1 wherein determining a third matrix includes calculating the third matrix using the first matrix, a state matrix that defines physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an input matrix that defines the effect of stack power and an R matrix.\n\n7. The method according to claim 6 wherein determining a third matrix includes calculating the third matrix as:\nf=−(BR−1BT−AT)−1KEd, where f is the third matrix, K is the first matrix, A is the state matrix that defines physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, E is the input matrix that defines the effect of stack power and d is the output power of the fuel cell stack.\n\n8. The method according to claim 1 wherein generating a control matrix includes adding the first, second and third matrices and multiplying by the inverse of an R matrix and the transpose of an input matrix that defines input effects on the system as:\nu=−R−1BT(Kx(t)+f(t)+h(t)), where u is the control matrix, K is the first matrix, h is the second matrix, f is the third matrix and B is the input matrix that defines input effects on the system.\n\n9. The method according to claim 1 wherein the pump and the bypass valve are positioned downstream from an output of the radiator in the coolant loop.\n\n10. The method according to claim 9 wherein the bypass valve is positioned farther downstream than the pump.\n\n11. The method according to claim 1 wherein the fuel cell system is on a vehicle.\n\n12. A method for controlling the temperature of a fuel cell stack in a fuel cell system, said method comprising: developing a model of the fuel cell system that employs non-linear equations; and controlling the speed of a pump for pumping a cooling fluid through a coolant loop in the fuel cell system and a position of a bypass valve that selectively directs the cooling fluid in the cooling loop through the radiator or around the radiator, wherein controlling the speed of the pump and the position of the bypass valve includes combining the control of the speed of the pump and the position of the bypass valve.\n\n13. The method according to claim 12 wherein controlling the speed of the pump and the position of the bypass valve includes determining a first matrix that is representative of the temperature of the cooling fluid coming out of the stack and the temperature of the cooling fluid coming out of the radiator, determining a second matrix based on a desired temperature set-point of the fuel cell stack, determining a third matrix based on the output power of the fuel cell stack and generating a control matrix for controlling the speed of the pump and the position of the bypass valve by combining the first, second and third matrices.\n\n14. A fuel cell system comprising: a fuel cell stack; a radiator; a coolant loop directing a cooling fluid through the fuel cell stack and the radiator and receiving the cooling fluid from the fuel cell stack and the radiator, said coolant loop including a bypass portion; a pump for pumping the cooling fluid through the coolant loop, the fuel cell stack and the radiator; a bypass valve for selectively directing the cooling fluid through the radiator and the bypass portion around the radiator; an input temperature sensor for measuring the temperature of the cooling fluid entering the fuel cell stack; an output temperature sensor for measuring the temperature of the cooling fluid exiting the fuel cell stack; and a controller for controlling the bypass valve and the pump based on the temperature of the cooling fluid, said controller controlling the bypass valve and the pump in combination.\n\n15. The system according to claim 14 wherein the controller determines a first matrix that is representative of the temperature of the cooling fluid coming out of the stack and the temperature of the cooling fluid coming out of the radiator, determines a second matrix based on a desired temperature set-point of the fuel cell stack, determines a third matrix based on the output power of the fuel cell stack, and generates a control matrix for controlling the speed of the pump and the position of the bypass valve by combining the first, second and third matrices.\n\n16. The system according to claim 15 wherein the controller determines the first matrix based on a state matrix that defines the physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an output matrix that defines variables being measured, a matrix tuned to a desired response and an R matrix.\n\n17. The system according to claim 16 wherein the controller determines the first matrix as:\n0=−KA−ATK+KBR−1BTK−CTQC, where K is the first matrix, A is the state matrix that defines the physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, C is the output matrix that defines variables being measured and Q is the matrix tuned to a desired response.\n\n18. The system according to claim 15 wherein the controller determines the second matrix based on a state matrix that defines physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an output matrix that defines variables being measured and a matrix tuned to a desired response.\n\n19. The system according to claim 18 wherein the controller determines the second matrix as:\nh=(BR−1BT−AT)−1CTQZ, where h is the second matrix, A is the state matrix that defines physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, C is the output matrix that defines variables being measured, Q is the matrix tuned to a desired response, and z is the desired temperature set-point of the fuel cell stack.\n\n20. The system according to claim 15 wherein the controller determines the third matrix using the first matrix, a state matrix that defines physical properties of the fuel cell system, an input matrix that defines input effects on the fuel cell system, an input matrix that defines the effect of stack power and an R matrix.\n\n21. The system according to claim 20 wherein the controller determines the third matrix as:\nf=−(BR−1BT−AT)−1KEd, where f is the third matrix, K is the first matrix, A is the state matrix that defines physical properties of the fuel cell system, B is the input matrix that defines input effects on the fuel cell system, E is the input matrix that defines the effect of stack power and d is the output power of the fuel cell stack.\n\n22. The system according to claim 15 wherein the controller generates the control matrix by adding the first, second and third matrices and multiplying by the inverse of an R matrix and the transpose of an input matrix that defines input effects on the system as:\nu=−R−1BT(Kx(t)+f(t)+h(t)), where u is the control matrix, K is the first matrix, h is the second matrix, f is the third matrix and B is the input matrix that defines input effects on the system.\n\n23. The system according to claim 14 wherein the pump and the bypass valve are positioned downstream from an output of the radiator in the coolant loop.\n\n24. The system according to claim 23 wherein the bypass valve is positioned farther downstream than the pump.\n\n25. The system according to claim 14 wherein the fuel cell system is on a vehicle.\n\nDescription:\n\n# BACKGROUND OF THE INVENTION\n\n1. Field of the Invention\n\nThis invention relates generally to a fuel cell system and, more particularly, to a control scheme for controlling the temperature and flow rate of a cooling fluid flowing through a fuel cell stack in a fuel cell system.\n\n2. Discussion of the Related Art\n\nHydrogen is a very attractive fuel because it is clean and can be used to efficiently produce electricity in a fuel cell. The automotive industry expends significant resources in the development of hydrogen fuel cells as a source of power for vehicles. Such vehicles would be more efficient and generate fewer emissions than today's vehicles employing internal combustion engines.\n\nA hydrogen fuel cell is an electrochemical device that includes an anode and a cathode with an electrolyte therebetween. The anode receives hydrogen gas and the cathode receives oxygen or air. The hydrogen gas is disassociated in the anode to generate free hydrogen protons and electrons. The hydrogen protons pass through the electrolyte to the cathode. The hydrogen protons react with the oxygen and the electrons in the cathode to generate water. The electrons from the anode cannot pass through the electrolyte, and thus are directed through a load to perform work before being sent to the cathode. The work acts to operate the vehicle.\n\nProton exchange membrane fuel cells (PEMFC) are a popular fuel cell for vehicles. A PEMFC generally includes a solid polymer electrolyte proton conducting membrane, such as a perfluorosulfonic acid membrane. The anode and cathode typically include finely divided catalytic particles, usually platinum (Pt), supported on carbon particles and mixed with an ionomer. The catalytic mixture is deposited on opposing sides of the membrane. The combination of the anode catalytic mixture, the cathode catalytic mixture and membrane define a membrane electrode assembly (MEA). MEAs are relatively expensive to manufacture and require certain conditions for effective operation. These conditions include proper water management and humidification, and control of catalyst poisoning constituents, such as carbon monoxide (CO).\n\nMany fuel cells are typically combined in a fuel cell stack to generate the desired power. For example, a typical fuel cell stack for an automobile may have two hundred stacked fuel cells. The fuel cell stack receives a cathode input gas, typically a flow of air forced through the stack by a compressor. Not all of the oxygen in the air is consumed by the stack and some of the air is output as a cathode exhaust gas that may include water as a stack by-product. The fuel cell stack also receives an anode hydrogen input gas that flows into the anode side of the stack.\n\nThe fuel cell stack includes a series of bipolar plates positioned between the several MEAs in the stack. The bipolar plates include an anode side and a cathode side for adjacent fuel cells in the stack. Anode gas flow channels are provided on the anode side of the bipolar plates that allow the anode gas to flow to the MEA. Cathode gas flow channels are provided on the cathode side of the bipolar plates that allow the cathode gas to flow to the MEA. The bipolar plates are made of a conductive material, such as stainless steel, so that they conduct the electricity generated by the fuel cells out of the stack. The bipolar plates also include flow channels through which a cooling fluid flows.\n\nIt is necessary that a fuel cell operate at an optimum relative humidity and temperature to provide efficient stack operation and durability. The temperature provides the relative humidity within the fuel cells in the stack for a particular stack pressure. Excessive stack temperature above the optimum temperature may damage fuel cell components, reducing the lifetime of the fuel cells. Also, stack temperatures below the optimum temperature reduces the stack performance.\n\nFuel cell systems employ thermal sub-systems that control the temperature within the fuel cell stack. Particularly, a cooling fluid is pumped through the cooling channels in the bipolar plates in the stack. The known thermal sub-systems in the fuel cell system attempt to control the temperature of the cooling fluid being input into the fuel cell stack and the temperature difference between the cooling fluid into the stack and the cooling fluid out of the stack, where the cooling fluid flow rate controls the temperature difference.\n\nFIG. 1 is a schematic plan view of a fuel cell system 10 including a thermal sub-system for providing cooling fluid to a fuel cell stack 12. The cooling fluid that flows through the stack 12 flows through a coolant loop 14 outside of the stack 12 where it either provides heat to the stack 12 during start-up or removes heat from the stack 12 during fuel cell operation to maintain the stack 12 at a desirable operating temperature, such as 60° C.-80° C. An input temperature sensor 16 measures the temperature of the cooling fluid in the loop 14 as it enters the stack 12 and an output temperature sensor 18 measures the temperature of the cooling fluid in the loop 14 as it exits the stack 12.\n\nA pump 20 pumps the cooling fluid through the coolant loop 14, and a radiator 22 cools the cooling fluid in the loop 14 outside of the stack 12. A fan 24 forces ambient air through the radiator 22 to cool the cooling fluid as it travels through the radiator 22. A bypass valve 26 is positioned within the coolant loop 14, and selectively distributes the cooling fluid to the radiator 22 or around the radiator 22 depending on the temperature of the cooling fluid. For example, if the cooling fluid is at a low temperature at system start-up or low stack power output, the bypass valve 26 will be controlled to direct the cooling fluid around the radiator 22 so that heat is not removed from the cooling fluid and the desired operating temperature of the stack 12 can be maintained. As the power output of the stack 12 increases, more of the cooling fluid will be routed to the radiator 22 to reduce the cooling fluid temperature. A controller 28 controls the position of the bypass valve 28, the speed of the pump 20 and the speed of the fan 24 depending on the temperature signals from the temperature sensors 16 and 18, the power output of the stack 12 and other factors.\n\nThe known temperature control schemes for fuel cell thermal sub-systems independently controlled the speed of the pump 20 and the position of the bypass valve 26. Particularly, the speed of pump 20 is used to control the difference between the input temperature of the cooling fluid provided to the stack 12 and the output temperature of the cooling fluid out of the stack 12 at some nominal value. The bypass valve 26 is used to control the temperature of the cooling fluid sent to the stack 12. Because the speed of the pump 20 and the position of the bypass valve 26 are independently controlled, fluctuations in the temperature of the stack 12 may significantly deviate from the optimum temperature, and thus the performance and durability of the system 10 may be reduced.\n\n# SUMMARY OF THE INVENTION\n\nIn accordance with the teachings of the present invention, a temperature control scheme for a fuel cell stack thermal sub-system in a fuel system is disclosed that provides an optimum stack temperature. The thermal sub-system includes a coolant loop directing a cooling fluid through the stack, a pump for pumping the cooling fluid through the coolant loop, a radiator for cooling the cooling fluid outside of the fuel cell stack and a bypass valve for selectively directing the cooling fluid in the coolant loop through the radiator or around the radiator. In one embodiment, the pump and the bypass valve are positioned downstream from an output of the radiator.\n\nA controller controls the position of the bypass valve and the speed of the pump in combination with each other by solving differential equations based on a system model. The system model is used to determine a first matrix that is representative of the temperature of the cooling fluid coming out of the stack and the temperature of the cooling fluid coming out of the radiator. The system model is also used to determine a second time-varying matrix based on the desired temperature set point of the fuel cell stack. The system model is also used to determine a third time-varying matrix based on the output power of the fuel cell stack. The first, second and third matrices are used to generate a control matrix for controlling the speed of the pump and the position of the bypass valve.\n\nAdditional advantages and features of the present invention will become apparent from the following description and appended claims, taken in conjunction with the accompanying drawings.\n\n# BRIEF DESCRIPTION OF THE DRAWINGS\n\nFIG. 1 is a schematic plan view of a cooling system for a fuel cell stack in a fuel cell system of the type known in the art;\n\nFIG. 2 is a schematic plan view of a cooling system for a fuel cell stack in a fuel cell system, according to an embodiment of the present invention; and\n\nFIG. 3 is a block diagram of a controller for the system shown in FIG. 2.\n\n# DETAILED DESCRIPTION OF THE EMBODIMENTS\n\nThe following discussion of the embodiments of the invention directed to a control scheme for a thermal sub-system in a fuel cell system is merely exemplary in nature, and is in no way intended to limit the inventions or its application or uses. For example, the discussion herein describes a control scheme for a fuel cell system on a vehicle. However, the control scheme may have application for fuel cells for other uses.\n\nAccording to the invention, an optimal controller for a thermal sub-system of the fuel cell system 10 is described and includes developing a model of the system 10. By performing an energy balance of the components in the system 10 and applying well-known thermodynamics, the non-linear equations shown in equations (1)-(3) below represent the dynamics of the system 10. $ⅆ ⅆt[(ρ(Vol)Cp)coolTstk,out]=m.stkCp,c(1-X)(Trad,out-Tstk,out)+Q.gen(1)ⅆ ⅆt[(ρ(Vol)Cp)coolTrad,out]=m.stkCp,c(1-X)(Tstk,out-Trad,out)-QITD(Trad,in-Tair,in)(2)ⅆ ⅆt[(ρ(Vol)Cp)airTair,out]=m.airCp,a(Tair,in-Tair,out)+QITD(Trad,in-Tair,in)(3)$\n\nWhere, p is the density of the coolant and air;\n\nVol is the volume of the stack 12 and the radiator 22;\n\nCp is the specific heat of the coolant air;\n\nTstk,out is the temperature of the cooling fluid out of the stack 12 and is a state variable;\n\nTrad,out is the temperature of the cooling fluid out of the radiator 22 and is a state variable;\n\nTair,out is the temperature of the air out of the radiator 22 and is a state variable;\n\nTair,in is the temperature of the air into the radiator 22 and is an input variable;\n\nTrad,in is the temperature of the cooling fluid into the radiator 22 and is a state variable;\n\n{dot over (m)}stk is the coolant flow through the stack 12 and is an input reflective of the pump commanded flow;\n\n{dot over (m)}air is the airflow through the radiator 22;\n\nX is the position of the bypass valve 26 and varies between 0 and 1;\n\nQ/ITD (heat rejection/inlet temperature difference) is a family of curves representing the performance of the radiator 22; and\n\n{dot over (Q)}gen represents the energy generated by the fuel cell stack 12.\n\nStack thermal mass is not considered to simplify the equations (1)-(3), thereby increasing the controllability analysis. Inflated volume numbers can be used to account for an increased thermal lag while eliminating a dynamic equation. No thermal losses are assumed through the piping of the system 10. Either the plumbing is well insulated or the distances are short.\n\nThe equations (1)-(3) are based on the physics of the system 10. The control system design becomes important when deciding what variable to control. It is universally accepted that a temperature of the cooling fluid flowing into or out of the fuel cell stack 12, as well as the temperature across the stack 12, is of paramount important when accurate relative humidity control is required. This gives the following equations (4) and (5) from the above model.\n\nA problem with the equations (4) and (5) is the presence of the position of the bypass valve 26. This implies that one of the inputs directly affects both of the desired outputs. While this is not necessarily bad, it does add two more non-linear equations to the control problem causing further complexity when attempting to apply linearization and/or linear control techniques. In addition, a non-minimum phase system can result, which leads to stability problems, slow responses and difficulty in tracking control.\n\nKnown control techniques typically employ coupled PID loops. One loop controls the change in temperature of the cooling fluid between the fluid input and output of the stack 12 with the coolant flow {dot over (m)}stk, while the other loop controls Tstk,in with the position of the bypass valve 26. From the coupled non-linear equations (4) and (5), it is clear that two decoupled loops will interact with each other causing less than optimal, and sometimes unstable, behavior.\n\nAs will be discussed below, by optimizing the combined control of the pump 20 and the bypass valve 26, the system 10 can anticipate temperature changes to the fuel cell stack 12, and can increase the speed of the pump 20 or redirect more flow to the radiator 22 using the bypass valve 26 before the temperature actually increases.\n\nFIG. 2 is a schematic block diagram of a fuel system 36, according to an embodiment of the present invention. The fuel cell system 36 is similar to the system 10 discussed above, where like elements are identified by the same reference numeral. The fuel cell system 36 includes a controller 38 that optimizes the performance of the thermal sub-system by using a system model to develop an optimal control law combines the control of the pump 20 and the bypass valve 26, as will be discussed in detail below. According to the invention, the control scheme will anticipate changes in the temperature of the cooling fluid and provide a desirable control before the temperature change occurs.\n\nAccording to one embodiment of the invention, the pump 20 and the bypass valve 26 are positioned at a different location in the cooling loop 14 than in the system 10, as shown. This position for the pump 20 and the bypass valve 26 is by way of a non-limiting example in that the control scheme described below has application for any suitable position for the pump 20 and the bypass valve 26, including the positions shown in the system 10.\n\nThere are only very subtle differences between the fuel cell systems 10 and 36, which is essential because there is no increase in system cost. The main problem with the system 10 is that the bypass valve 26 set the blending of the two coolant loops before going into the stack inlet. The new location of the bypass valve 26 in the system 36 either allows cooling fluid from the radiator 22 or does not allow cooling fluid from the radiator 22, which means that the cooling fluid temperature out of the radiator 22 is the cooling fluid temperature into the stack 12. The location of the bypass valve 26 essentially sets the location of the pump 20.\n\nBased on the model developed above, the resulting non-linear dynamic equations (6)-(8) for the system 36 are: $ⅆ ⅆt[(ρ(Vol)Cp)coolTstk,out]=m.radCp,c(X)(Trad,out-Tstk,out)+Qgen(6)ⅆ ⅆt[(ρ(Vol)Cp)coolTrad,out]=m.radCp,c(X)(Tstk,out-Trad,out)-QITD(Trad,in-Tair,in)(7)ⅆ ⅆt[(ρ(Vol)Cp)airTair,out]=m.airCp,a(Tair,in-Tair,out)+QITD(Trad,in-Tair,in)(8)$\n\nNote that the thermal dynamic equations (6)-(8) for the system 36 are nearly the same as the equations (1)-(3) for the system 10. They are again non-linear, but this is unavoidable, and it is in the desired output equations where the greatest impact is seen.\n\nFor the equations (9) and (10), the desired outputs result in linear combinations of state variables, thus eliminating the bypass valve input directly affecting the output. Further simplification provides:\ny2=Tstk,out (12)\nThe Tstk,out set-point is the desired Tstk,in+ΔTdes.\n\nBy using the two dynamic equations (11) and (12), two linearization techniques can be applied, particularly feedback linearization and a Taylor series linearization. Since Taylor series approximation can be unreliable when the operating point deviates from the linearization point, it is advantageous to apply feedback linearization first, although either method would result in a linear model of the system 36.\n\nTaking the set of state equations (6)-(8) and defining two new inputs, v and w, gives: $v=m.radCp,c(X)(Trad,out-Tstk,out)(13)w=QITD(Trad,in-Tair,in)(14)QITD=f(m.rad,-Tair,in,geometry)(15)$\nWhich yields: $[ⅆ ⅆt[(ρ(Vol)Cp)coolTstk,out]ⅆ ⅆt[(ρ(Vol)Cp)coolTrad,out]]=[Tstk,outTrad,out]+[10-1-1][vw]+Q.gen(16)$\n\nThe equation (8) is dropped because it does not affect the desired outputs. It can still be included, but it will only give the air temperature outside of the radiator 22. The resulting output equation is: $[y1y2]=[Tstk,outTrad,out]+[vw]+Q.gen(17)$\n\nThis completes the linearization portion of the control strategy. From this point it is possible to apply any number of linear control schemes including, but not limited to, optimal control, robust control and pole placement.\n\nThe controller 38 provides an optimal control based on a tracking linear quadratic regulator (LQR) with a known disturbance. LQR has been well documented in linear control literature where the goal is to return (regulate) the state variable to zero, but subject to a system disturbance. In the system 36, a state output of zero is not desirable. It is rather desirable to have the thermal sub-system outputs Tstk,out and Tstk,in track a given temperature set-point based on a calculation from a desired relative humidity. In addition, the tracking controller has a known disturbance {dot over (Q)}gen that is also included in the control law.\n\nReplacing the equations (16) and (17) with variables representing matrices results in:\n{dot over (x)}=Ax+Bu+Ed (18)\ny=Cx (19)\nIn the equations (18) and (19), A is a state matrix that defines the physical properties of the system 36, B is an input matrix that defines the input effects on the system 36, C is an output matrix that defines what variables are being measured, and E is an input matrix that is a disturbance influence on the system 36 and defines the effect of stack power. $x_=[Tstk,outTrad,out]u=[vw]d=Q.geny=[Tstk,inTstk,out]A=B=[10-1-1]E=C=$\n\nThe following series of equations are not required to implement the control law. They are only the development of the control law. As with all optimal control laws, a cost function subject to constraints is defined as: $min J=12eFTFeF+12∫tot(eTQe+utRud τ)(20)s.t.x._=Ax_+Bu_+Ed(21)y=Cx_(22)$\nWhere the error e is defined as:\ne=z−y (23)\nWhere z is the desired temperature set-point and y is the output of the thermal sub-system.\n\nThe goal of the optimization in the equations (20)-(22) is to make the cost function as small as possible. Since the terminal condition is not important in this case, F=0, leaving just the integral as the cost function. This means that the designer must choose a positive semi-definite Q matrix and a positive definite R matrix that sufficiently balances the integral so that the optimization penalizes the error e between the set-point and the output Q and the controller action u through the R matrix. The constraint in this optimization problem is the dynamic state equations themselves. This essentially forces the determined control law to be applicable to the system under consideration.\n\nForming the Hamiltonian and inserting the co-state variable A gives: $H=12(eTQe+uTRu)+λT(Ax+Bu+Ed)(24)$\n\nSubstituting the equation (23) into the equation (24) gives: $H=12((z-Cx)TQ(z-Cx)+uTRu)+λT(Ax+Bu+Ed)(25)$\n\nSolving for the state equation (25) gives: $x.=∂H∂λ=Ax+Bu+Ed (26)$\n\nThe co-state equation is given as: $λ.=∂H∂x=CTQ(z-Cx)-ATλ(27)$\n\nSolving for the controller output u gives: $∂H∂u=0=12(2Ru)+BTλ(28)u=-R-1BTλ(29)$\n\nSubstituting the equations (28) and (29) into the equations (26) and (27) gives:\n{dot over (x)}=Ax−BR−1BTλ+Ed (30)\n{dot over (λ)}=CTQz−CTQCx−ATλ (31)\n\nPutting the equations (30) and (31) in a state-space form gives: $[x.λ.]=[A-BR-1BT-CTQC-AT][xλ]+[E0OCTQ][dz](32)$\n\nSolving for the boundary conditions gives: $[x(T)λ(T)]=[Φ11Φ12Φ21Φ22][x(t)λ(t)]+∫tot[Φ11(t,τ)Φ12(t,τ)Φ21(t,τ)Φ22(t,τ)][EzCTQd] ⅆτ(33)$\n\nExpanding the equation (33) defines four dummy variables: $x(T)=Φ11x(t)+Φ12λ(t)+∫Φ11(t,τ)Ezⅆτ+ ∫Φ12(t,τ)CTQⅆⅆτ=Φ11x(t)+Φ12λ(t)+f1+h1(34)f1=∫Φ11(t,τ)Ezⅆτ(35)h1=∫Φ12(t,τ)CTQⅆⅆτ(36)λ(T)=Φ21x(t)+Φ22λ(t)+∫Φ21(t,τ)Ezⅆτ+∫Φ22(t,τ)CTQⅆⅆτ=Φ21x(t)+Φ22λ(t)+f2+h2(37)f2=∫Φ21(t,τ)Ezⅆτ(38)h2=∫Φ22(t,τ)CTQⅆⅆτ(39)$\n\nFurther applying boundary conditions (F=0) gives: $λ(T)=∂J∂x(T)=12eFTFeF=12(z-Cx)TF(z-Cx)=12[z(-CT)F(z-Cx)] (40)λ(T)=-CTFz(T)+CTFCx(T)(41)$\n\nSubstitution the equations (40) and (41) into the equations (37)-(39) gives:\nCTFz(T)+CTFCx(T)=Φ21x(t)+Φ22λ(t) +f2+h2 (42)\n\nSubstituting the equations (34)-(36) into the equation (42) and simplifying for λ (t) gives: $-CTFz(T)+CTFC[Φ11x(t)+Φ12λ(t)+f1+h1]=Φ21x(t)+Φ22λ(t)+f2+h2(43)λ(t)=(CTFCΦ12-Φ22)-1[(Φ21-CTFCΦ11)x(t)-CTFz(t)+CTFCf1-f2+CTFCh1-h2](44)$\n\nDefining three new variables K, f(t) and h(t) gives:\nλ(t)=Kx(t)+f(t)+h(t) (45)\nWhere,\nK=(CTFCΦ12−Φ22)−121−CTFCΦ11) (46)\nf(t)=(CTFCΦ12−Φ22)−1(−CTFz(t)+CTFCf1−f2) (47)\nh(t)=(CTFCΦ12−Φ22)−1(CTFCh1−h2) (48)\n\nSubstituting the equation (45) into the equations (28)-(32) gives the optimal control law for set-point tracking subject to a known disturbance input as:\nu=−R−1BT(Kx(t)+f(t)+h(t)) (49)\n\nDifferentiating the equation (45) gives:\n{dot over (λ)}(t)={dot over (K)}x(t)+K{dot over (x)}(t)+{dot over (f)}(t)+{dot over (h)}(t) (50)\n\nSubstituting the equation (44) into the equation (32) gives: $x.=Ax-BR-1BT[Kx(t)+f(t)+h(t)]+Ed=(A-BR-1BTK)x(t)-BR-1BTf(t)=BR-1BTh(t)+Ed(51)$\n\nSubstituting the equation (51) into the equation (50) gives:\n{dot over (λ)}(t)={dot over (K)}x(t)+K[(A−BR−1BTK)x(t)−BR−1BTf(t)=BR−1BTh(t)+Ed]+f(t)+{dot over (h)}(t) (52)\n{dot over (λ)}(t)=[{dot over (K)}+K(A−BR−1BTK)]x−KBR−1BTf(t)+{dot over (f)}(t)−KBR−1 BTh(t)+{dot over (h)}(t)+KEd (53)\n\nFrom the equation (32), substituting the equation (45) and combining like terms with the equations (52) and (53) gives: $λ.=CTQz-CTQCx+AT[Kx(t)+f(t)+h(t)](54)[K.+K(A-BR-1BTK)]x-KBR-1BTf(t)+f.(t)-KBR-1BTh(t)+h.(t)+KEd=(ATK-CTQC)x+CTQz+AT[f(t)+h(t)](55)$\n\nFor x(t):\n{dot over (K)}=−KA−ATK+KBR−1BTK−CtQC (56)\n\nFor f(t), where the disturbance is accounted for, gives:\n{dot over (f)}(t)=(BR−1BT−AT)f(t)−KEd (57)\n\nFor h(t), where the desired set-point is accounted for, gives:\n{dot over (h)}(t)=(BR1BT−AT)(t)+CTQz (58)\n\nThe final conditions K(T), f(T) and h(T) can be solved in a similar manner from the equations (40), (41) and (44). $λ(T)=Kx(T)+f(T)+h(T)(59)λ(T)=-CFz(T)+CTFCx(T)(60)K(T)=CTFC(61)f(T)=0(62)h(T)=-CTFz(T)(63)$\n\nWith this step the derivation of the equations used to solve the optimal control problem are complete. What remains is the non-linear differential equation (56) and the two ordinary first order differential equations (57) and (58). From the equation (56) it is clear that it is in the form of the Differential Riccati equation, independent of f(t) and h(t). However, only the final conditions are known for the equations (56), (57) and (58) meaning that one must integrate backward in time if time-varying matrices are required for K(t), f(t) and h(t). Since the goal of the controller 38 is to have an autonomous non-varying solution, the gain matrices are constant, requiring d(K)/dt=df/dt=dh/dt=0. This results in the Algebraic Riccotti equation given as:\n0=−KA−ATK+KBR−1BTK−CTQC (64)\nf=−(BR−1BT−AT)−1KEd (65)\nh=(BR−1BT−AT)−1CTQz (66)\n\nAll that remains is to solve for K and substitute into the equations (64)-(66) as:\nu=−R−1BT(Kx(t)+f(t)+h(t)) (67)\n\nFIG. 3 is a block diagram of the controller 38 showing how the control output u is determined. A multiplier 42 generates the K matrix, a multiplier 44 generates the h matrix and a multiplier 46 generates the f matrix based on the equations discussed above. State variable feedback is applied to the multiplier 42, which generates the K matrix from the equation (64) that is then applied to an adder 52. The desired temperature set-point z of the stack 12 is applied to the multiplier 44. The multiplier 44 generates the h matrix from the equation (66), which is added to the K matrix in the adder 52. The disturbance d or output power of the stack 12 is applied to the multiplier 46 and the f matrix is calculated using the equation (65). The f matrix is subtracted from the K matrix and h matrix in the adder 52. Equation (67) is then solved for the control output from the addition of K(t), f(t) and h(t) which is multiplied by the inverse of R and the transpose of B.\n\nThe foregoing discussion discloses and describes merely exemplary embodiments of the present invention. One skilled in the art will readily recognize from such discussion and from the accompanying drawings and claims that various changes, modifications and variations can be made therein without departing from the spirit and scope of the invention as defined in the following claims."
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https://www.bossmaths.com/a18c/ | [
"# A18c – Solving quadratic equations using the quadratic formula\n\nThis is the students’ version of the page. Log in above for the teachers’ version.\n\n# The quadratic formula\n\n$${\\color{Black}{\\large \\text{If }ax^{2} + bx +c = 0}}$$\n\n_\n\n$${\\color{Black}{\\large \\text{then }x = \\dfrac{-b \\pm \\sqrt{b^{2}-4ac}}{2a}}}$$\n\n_\n\n$${\\large \\color{#e0e0e0}{\\text{then x }}\\color{Black}{= \\dfrac{-b}{2a} \\pm \\dfrac{\\sqrt{b^{2}-4ac}}{2a}}}$$\n\n_\n\n$${\\color{Black}{\\large \\text{The line }x = -\\dfrac{b}{2a}\\text{ is the line }}}$$$${\\color{Black}{\\large \\text{of symmetry for the curve }}}$$ $${\\color{Black}{\\large y=ax^{2} + bx +c}}$$\n\n_\n\n$${\\color{Black}{\\large \\text{Also, }\\dfrac{\\sqrt{b^{2}-4ac}}{a} \\text{ is the }}}$$ $${\\color{Black}{\\large \\text{distance between the }}}$$ $${\\color{Black}{\\large \\text{solutions of }ax^{2} + bx +c = 0 }}$$. $${\\color{Black}{\\large \\text{Can you see why?}}}$$\n\n# Solving quadratic equations using the quadratic formula\n\nTeacher resources\n\nLinks to past exam questions"
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https://math.stackexchange.com/questions/3092718/integral-int-infty-infty-frac-sinhxx-a-coshx2dx | [
"# Integral $\\int_{-\\infty}^{\\infty} \\frac{\\sinh(x)}{x [a+\\cosh(x)]^2}dx$\n\nI have difficulties with calculating the following integral:\n\n$$I(a)=\\int_{-\\infty}^{\\infty} \\frac{\\sinh(x)}{x [a+\\cosh(x)]^2} \\mathrm dx~~~~~~~,\\text{where } a>1$$\n\nFor the case with $$a=1$$ the solution is $$-28 \\zeta'(-2)$$.\n\n• Expand $\\frac{\\sinh(x)}{(a+\\cosh(x))^2} = \\sum_{k=1}^\\infty c_k(a) e^{-kx}$ then $\\int_0^\\infty x^{s-1} \\frac{\\sinh(x)}{(a+\\cosh(x))^2} dx = \\sum_{k=1}^\\infty c_k(a) k^{-s} \\Gamma(s)$ and $\\int_{-\\infty}^\\infty x^{s-1} \\frac{\\sinh(x)}{(a+\\cosh(x))^2} dx = 2\\lim_{s \\to 0} \\sum_{k=1}^\\infty c_k(a) k^{-s} \\Gamma(s)$. Things like $\\zeta'(-2)$ appear from the functional equation, or the residue theorem. Jan 29, 2019 at 21:14\n• What have you tried? Where did you struggle? Please show some effort you made and include it within your post with an edit :) Jan 29, 2019 at 21:15\n• Actually, I've tried an expansion but a very crude one. The solution by @reuns looks impressive. Jan 29, 2019 at 21:17\n\nI will do the case $$a=1$$ in order to give some insight:$$I=\\int_{-\\infty}^{\\infty} \\frac{\\sinh(x)}{x (1+\\cosh(x))^2}dx\\overset{x=\\ln t}=2\\int_0^\\infty \\frac{t-1}{(t+1)^3}\\frac{dt}{\\ln t}$$ We can consider the following integral and perform Feynman's trick: $$I(n)=2\\int_0^\\infty \\frac{t^{n-1}-1}{(t+1)^3}\\frac{dt}{\\ln t}$$ $$\\Rightarrow \\frac{d}{dn}I(n)=2\\int_0^\\infty \\frac{t^{n-1}}{(t+1)^3}dt=2B(n,3-n)=\\Gamma(n)\\Gamma(3-n)$$ $$=(2-n)(1-n)\\Gamma(n)\\Gamma(1-n)=\\pi\\frac{(1-n)(2-n)}{\\sin(\\pi n)}$$ $$I(1)=0 \\Rightarrow I(2)-I(1)=I =\\pi\\int_1^2 \\frac{(1-n)(2-n)}{\\sin(\\pi n)}dn$$ $$\\overset{n-1=x}=\\boxed{\\pi \\int_0^1 \\frac{x(1-x)}{\\sin(\\pi x)}dx = \\frac{7\\zeta(3)}{\\pi^2 }=-28\\zeta'(-2)}$$ The last integral can be found here.\nBy the same idea one gets: $$I(a)=\\int_{-\\infty}^\\infty \\frac{\\sinh x}{x(a+\\cosh x))^2}dx=2\\int_0^\\infty \\frac{x^2-1}{(x^2+2ax+1)^2}\\frac{dx}{\\ln x}$$ Now consider the same parameter take a derivative with respect to it, apply a Mellin transform, and try to carry on."
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https://cran.fhcrc.org/web/packages/JustifyAlpha/vignettes/Introduction_to_JustifyAlpha.html | [
"# Vignette Accompanying “Justify Your Alpha: A Primer on Two Practical Approaches”\n\nThe goal of JustifyAlpha is to provide ways for researchers to justify their alpha level when designing studies. Two approaches are currently implemented. The first function optimal_alpha allows users to computed balanced or minimized Type 1 and Type 2 error rates. The second approach uses the function ttestEvidence or ftestEvidence to lower the alpha level as a function of the sample size to prevent Lindley’s paradox.\n\n## Installation\n\nYou can install the released version of JustifyAlpha from GitHub with:\n\ndevtools::install_github(\"Lakens/JustifyAlpha\")\n\n# Minimizing Error Rates\n\nAssume we plan to perform an independent t-test, where our smallest effect size of interest is d = 0.5, and we are planning to collect 64 participants in each condition. We would normally calculate power as follows:\n\npwr.t.test(d = 0.5, n = 64, sig.level = 0.05, type = 'two.sample', alternative = 'two.sided')$power This analysis tells us that we have 80% power with a 5% alpha level for our smallest effect size of interest, d = 0.5, when we collect 64 participants in each condition. If we design 2000 studies like this, the number of Type 1 and Type 2 errors we make depend on how often the null hypothesis is true, and how often the alternative hypothesis is true. Let’s assume both are equally likely. This means that in 0.5 × 2000 = 1000 studies the null hypothesis is true, and we will make 0.05 × 1000 = 50 Type 1 errors, so in 50 studies we will find a significant result, even though there is no true effect. In 0.5 × 2000 = 1000 studies the alternative hypothesis is true, and with 80% power we will make 0.2 × 1000 = 200 Type 2 errors, so in 200 studies we will not observe a significant result even if there is a true effect. Combining Type 1 and Type 2 errors, in the long run, we should expect 50 + 200 = 250 of our 2000 studies to yield an error. The combined error rate is therefore 250/2000 = 0.125. The goal in Neyman-Pearson hypothesis testing is to control the number of errors we make, as we perform hypothesis tests. Researchers often rely on convention when setting error rates, and there is no special reason to set the Type 1 error rate at 5% and the Type 2 error rate at 20%. Indeed, there might be better choices when designing studies. For example, when collecting 64 participants per condition, we can set the Type 1 and Type 2 error rates in a way that reduced the number of errors we make, such that from the 2000 studies less than 250 studies yield misleading conclusions. We can use the optimal_alpha function to compute the minimized error rates. The optimal_alpha function takes as input a power function, the relative cost of Type 1 and Type 2 errors (the default is 1, meaning both errors are equally costly), The prior odds of H1 versus H0 (the default is 1, meaning H1 and H0 are believed to be equally likely). We can convert odds to probabilities by calculating $$odds/(1+odds)$$. For example, if the prior odds are 1, the prior probability is 1/(1+1) = 0.5. If the prior odds of H1 compared to H0 are 2, the prior probability of H1 is 2/(2+1) = 0.66. Analogous, we can convert from probability to odds by dividing the probability by 1 minus the probability. For example, if the prior probability of H1 is 0.66. The prior odds of H1 compared to H0 are 0.66/(1-0.66) = 2. Apart from the prior odds, we also need to specify whether to compute the minimized combined error rate (“minimize”) or balanced error rates (“balanced”), and whether to provide output for each iteration of the optimization function or not, and a plot or not. An example of the us of the function is provided below: res1 <- optimal_alpha(power_function = \"pwr.t.test(d=0.5, n=64, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"minimize\",\ncostT1T2 = 1,\npriorH1H0 = 1,\nverbose = FALSE,\nprintplot = TRUE)",
null,
"res1$alpha ## 0.09978841 res1$beta\n## 0.1215426\nres1$errorrate ## 0.1106655 The output indicates that given the specific settings (e.g., weighing Type 1 and Type 2 errors equally, expecting H1 and H0 to be equally likely to be true) the combined error rate is minimized when (rounding to 3 decimal places) the alpha level is set to 0.10 (indicated by res$alpha), and the Type 2 error rate is set to 0.122 (indicated by res$beta). The expected error rate is then 0.111. In other words, if a researcher is interested in effects of d = 0.5, and plans to collect 64 participants in each condition, setting the Type 1 error rate to 10% will increase the power to 87.8%. If we would perform 2000 studies designed with these error rates, we would observe 0.5 (the prior probability that H0 is true) × 0.100 (the alpha level) × 2000 = 100 Type 1 errors, and 0.5 (the prior probability that H1 is true) × 0.122 (the Type 2 error rate) × 2000 = 122 Type 2 errors, for a total of 222 errors instead of 250. The combined error rate is therefore 222/2000 = 0.111. Indeed ,this is the value provided as the errorrate. In other words, by choosing a more optimal alpha level, we can design lines of research more efficiently, because we are less likely to make errors in our statistical inferences. This did increase the probability of making a Type 1 error (because we increased the alpha level), but this is compensated by reducing the probability of a Type 2 error even more. The figure below recreates Figure 2 in Mudge et al. (2012). # Note that printing plots is suppressed with rmarkdown here and it is simply used to generate the data. resplot1 <- optimal_alpha(power_function = \"pwr::pwr.t.test(d = 1, n = 3, sig.level = x, type = 'two.sample', alternative = 'two.sided')$power\", error = \"minimize\", costT1T2 = 1, printplot = TRUE)\nresplot2 <- optimal_alpha(power_function = \"pwr::pwr.t.test(d = 1, n = 10, sig.level = x, type = 'two.sample', alternative = 'two.sided')$power\", error = \"minimize\", costT1T2 = 1, printplot = TRUE) resplot3 <- optimal_alpha(power_function = \"pwr::pwr.t.test(d = 1, n = 30, sig.level = x, type = 'two.sample', alternative = 'two.sided')$power\", error = \"minimize\", costT1T2 = 1, printplot = TRUE)\nplot_data <- rbind(resplot1$plot_data, resplot2$plot_data, resplot3$plot_data) plot_data$n <- as.factor(rep(c(3, 10, 30), each = 9999))\n\nw_c_alpha_plot <- ggplot(data=plot_data, aes(x=alpha_list, y=w_c_list)) +\ngeom_line(size = 1.3, aes(linetype = n)) +\ngeom_point(aes(x = resplot1$alpha, y = (1 * resplot1$alpha + 1 * (resplot1$beta)) / (1 + 1)), color=\"red\", size = 3) + geom_point(aes(x = resplot2$alpha, y = (1 * resplot2$alpha + 1 * (resplot2$beta)) / (1 + 1)), color=\"red\", size = 3) +\ngeom_point(aes(x = resplot3$alpha, y = (1 * resplot3$alpha + 1 * (resplot3$beta)) / (1 + 1)), color=\"red\", size = 3) + theme_minimal(base_size = 16) + scale_x_continuous(\"alpha\", seq(0,1,0.1)) + scale_y_continuous(\"weighted combined error rate\", seq(0,1,0.1), limits = c(0,1)) w_c_alpha_plot",
null,
"## Balancing Error Rates You can choose to minimize the combined error rates, but you can also decide that it makes most sense to balance the error rates. For example, you might think a Type 1 error is just as problematic as a Type 2 error, and therefore, you want to design a study that has balanced error rates for a smallest effect size of interest (e.g., a 5% Type 1 error rate and a 95% Type 2 error rate). The optimal_alpha function can compute the alpha level that would lead to a balanced Type 2 error rate. res2 <- optimal_alpha(power_function = \"pwr.t.test(d=0.5, n=64, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"balance\",\ncostT1T2 = 1,\npriorH1H0 = 1,\nverbose = FALSE,\nprintplot = TRUE)",
null,
"res2$alpha ## 0.1111217 res2$beta\n## 0.1110457\nres2$errorrate ## 0.1110837 This balances the Type 1 and Type 2 error rates (with a maximum difference between the two of 0.0001). The alpha level is 11.11%, and the power is 88.9% (or the Type 2 error rate is 11.1%). Choosing to balance error rates is only slightly less efficient than minimizing the combined error rate in this example, with a combined error rate when balancing Type 1 and 2 errors of 22.22% compared to a minimized error rate of 22.13%. # Relative costs of Type 1 and Type 2 errors So far we have assumed a Type 1 error and Type 2 error are equally costly. This means that we consider the consequences of a false positive just as bad as the consequences of a false negative. This is not the default in psychology, where researchers typically treat Type 1 errors as 4 times as bad as Type 2 errors. This is based on Cohen (1988), who proposed to aim for 80% power, because we use an alpha of 5%. The optimal_alpha function users to set the relative cost of Type 1 and Type 2 errors, costT1T2. By default this parameter is set to 1, meaning both types of errors are weighed equally. Changing the value to 4 means that Type 1 errors are weighed 4 times as much as Type 2 errors, or 4:1. This will change the weight of Type 1 errors compared to Type 2 errors, and thus also the alpha level at which combined costs of Type 1 and Type 2 errors are minimized. res3 <- optimal_alpha(power_function = \"pwr.t.test(d=0.5, n=64, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"minimize\",\ncostT1T2 = 4,\npriorH1H0 = 1,\nverbose = FALSE,\nprintplot = TRUE)",
null,
"res3$alpha ## 0.03268853 res3$beta\n## 0.2524248\nres3$errorrate ## 0.07663579 Now, the alpha level that minimizes the combined Type 1 and Type 2 error rates is 3.27%. With 64 participants in each condition of an independent t-test the Type 2 error is 25.24%, and the expected combined error rate is 7.66%. If we would perform 2000 studies designed with these error rates, we would observe 0.5 (the prior probability that H0 is true) × 0.033 (the alpha level) × 2000 = 33 Type 1 errors, and 0.5 (the prior probability that H1 is true) × 0.252 (the Type 2 error rate) × 2000 = 252 Type 2 errors. Since we weigh Type 1 errors 4 times as much as Type 2 errors, we multiple the cost of the 33 Type 1 errors by 4, which makes 4×33 = 132, and to keep the weighted error rate between 0 and 1, we also multiple the 1000 studies where we expect H0 to be true by 4, such that the weighted combined error rate is (132+252)/(4000 + 1000) = 0.0768. If we choose to compute balanced error rates, we not surprisingly get, with n = 64 per conditions, which gives us 80% power with an alpha of 5%, exactly these error rates, as this scenario actually put the cost of a Type 1 error are 4 times the cost of a Type 2 error. res4 <- optimal_alpha(power_function = \"pwr.t.test(d=0.5, n=64, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"balance\",\ncostT1T2 = 4,\npriorH1H0 = 1,\nverbose = FALSE,\nprintplot = TRUE)",
null,
"res4$alpha ## 0.04974484 res4$beta\n## 0.1991642\nres4$errorrate ## 0.07962871 If we would perform 2000 studies designed with these error rates, we would observe 0.5 (the prior probability that H0 is true) × 0.05 (the alpha level) × 2000 = 50 Type 1 errors, and 0.5 (the prior probability that H1 is true) × 0.200 (the Type 2 error rate) × 2000 = 200 Type 2 errors, for a total of 250 errors. However, we weigh Type 1 errors 4 times as much as Type 2 errors (or 4:1). So the cost is or the 50 Type 1 errors is 4 × 50 = 200 (hence the balanced error rates, as the costs of Type 1 errors is now balanced with the cost for Type 2 errors). Because Type 1 errors are weighed four times as much as Type 2 errors, 0.8 of the weight is determined by Type 1 errors, and 0.2 of the weight is determined by Type 2 errors, and the weighted combined error rate is (0.8 × 0.05 + 0.2 × 0.20) = 0.08. # Prior probabilities of H0 and H1 So far, we have assumed that H0 and H1 are equally likely. We can change the prior probabilities that H0 is true (and you will observe a Type 1 error), or that the alternative hypothesis (H1) is true (and you will observe a Type 2 error). By incorporating these expectations, you can minimize or balance error rates in the long run (assuming your priors are correct). Priors can be specified using the priorH1H0 argument, which by default is 1 (H1 and H0 are equally likely). Setting it to 4 means you think the alternative hypothesis (and hence, Type 2 errors) are 4 times more likely than that the null hypothesis is true (and hence, Type 1 errors). res5 <- optimal_alpha(power_function = \"pwr.t.test(d=0.5, n=64, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"minimize\",\ncostT1T2 = 1,\npriorH1H0 = 4,\nverbose = FALSE,\nprintplot = TRUE)",
null,
"res5$alpha ## 0.2461469 res5$beta\n## 0.04831345\nres5$errorrate ## 0.08788013 If you think H1 is four times more likely to be true than H0, you need to worry less about Type 1 errors, and now the alpha that minimizes the weighted error rates is 24.6%, with a power of 4.8%. If we would perform 2000 studies designed with these error rates, and we expect H1 is true 4 times as often as H0, then we expect H0 to be true in 20% (or 400) of the studies, and H1 to be true in 80% (or 1600) of the studies (as 1:4 = 20:80 = 400:1600). So, we should expect to observe 0.2 (the prior probability that H0 is true) × 0.246 (the alpha level) × 2000 = 98.4 Type 1 errors, and 0.8 (the prior probability that H1 is true) × 0.0483 (the Type 2 error rate) × 2000 = 77.3 Type 2 errors, for a total of 175.7 errors. Because we expect H1 to be four times as likely as H0, we weigh Type 2 errors for 0.8, and Type 1 errors for 0.2. The weighted combined error rate is (0.2 × 0.246 + 0.8 × 0.0483) = 0.08784. The decision about priors is always subjective, as is the case in any decision under uncertainty. The more certain you are about auxiliary hypotheses and the stronger the theory, the higher your prior might be that you are right. Also, when you conduct a replication study, the prior probability of the hypothesis should usually be higher than when attempting to find a novel effect. The more a prediction goes against things we know or expect to be true, the more likely H0 should be. But when designing any study, we need to consider prior probabilities. You always make a choice - even if you choose to assume H0 is equally likely as H1. # Sample Size Justification So far we have only discussed how to justify the alpha level given a fixed sample size. However, in practice researchers usually want to conduct power analysis. This can be incorporated smoothly when minimizing or balancing error rates. To do so, you simply need to specify the weighted combined error rate you are aiming for and the function optimal_sample will return the sample size as well as the alpha and beta required to achieve the desired weighted combined error rate. res6 <- optimal_sample(power_function = \"pwr.t.test(d=0.5, n = sample_n, sig.level = x, type='two.sample', alternative='two.sided')$power\",\nerror = \"minimize\",\nerrorgoal = 0.05,\ncostT1T2 = 1,\npriorH1H0 = 1)\n\nres6\n## $alpha ## 0.046575 ## ##$beta\n## 0.05311184\n##\n## $errorrate ## 0.04984342 ## ##$objective\n## 0.04984342\n##\n## $samplesize ## 105 Using the code above, we see that if we aim to achieve a combined error rate of 0.05, we need 105 participants in each of two conditions for an independent t-test. # Specifying power functions So far we have used only one function from the pwr package to specify the power function. However, any function can be entered. Below we illustrate some additional approaches. The trickiest part is entering the correct power function. You can provide an analytic power function, either programmed yourself, or from an existing package loading on the server. Then, make sure the alpha value is not set, but specified as x, and that the function itself returns a single value, the power of the test. Finally, if you use existing power functions the shiny app needs to know which package this function is from, and thus the call to the function needs to be precended by the package and ‘::’, so ‘pwr::’ or ‘TOSTER::’. Some examples that work are provided below. res <- optimal_alpha(power_function = \"TOSTER::powerTOSTtwo(alpha=x, N=200, low_eqbound_d=-0.4, high_eqbound_d=0.4) \", error = \"minimize\", costT1T2 = 1, priorH1H0 = 1) res$alpha\nres$beta res$errorrate\nres$plot For a more challenging power function, we can use the Superpower package by Daniel Lakens and Aaron Caldwell. The power function in the ANOVAexact function is based on a simulation, which takes a while to perform. The optimization function used in this Shiny app needs to perform the power calculation multiple times. Thus, the result takes a minutes to calculate. Press calculate, and check the results 5 to 10 minutes later. Furthermore, the output of the ANOVA_exact function prints power as 80%, not 0.8, and thus we actually have to divide the power value by 100 for the Shiny app to return the correct results. Nevertheless, it works if you are very patient (this code is not run to prevent . res <- optimal_alpha(power_function = \"Superpower::ANOVA_exact( (Superpower::ANOVA_design(design = '2b', n = 64, mu = c(0, 0.5), sd = 1, plot = FALSE)), alpha_level = x, verbose = FALSE)$main_results$power/100\", error = \"minimize\", costT1T2 = 1, priorH1H0 = 1) res$alpha\nres$beta res$errorrate\nres$plot # Avoiding the Lindley Paradox Sometimes we don’t know the prior odds or the effect size of interest. In this case we can justify the alpha level by aiming to avoid the Lindley paradox. The Lindley paradox arises from the difference between error rate control and likelihood ratios in statistics. When the power is high, it is possible that a significant p-value is actually more likely to occur under the alternative than under the null hypothesis. This situation, where we reject the null hypothesis because p < alpha, but the evidence based on the likelihood suggests the observed data is more likely under the null hypothesis than the alternative hypothesis, is considered the Lindley paradox. The figure below shows that the steeper the p-value distribution (which occurs as the sample size increases) the more to the left the point where the expected p-value distribution under the alternative will cross the uniform p-value distribution under H0. The solution to prevent Lindley’s paradox is to lower the alpha level as a function of the sample size.",
null,
"P-value distributions for a two-sided independent t-test with N = 150 and d = 0.5 (black curve) or d = 0 (horizontal dashed line) which illustrates how p-values just below 0.05 can be more likely when there is no effect than when there is an effect. A Bayes factor and a p-value are directly related, given a prior, and a sample size. They can both be computed directly from the t-value. In the plot below we see the Bayes factor (plotted on the vertical axis) and the p-value (plotted on the horizontal axis) for an independent t-test with 100 participants in each condition. n1 <- 100 n2 <- 100 loops <- seq(from = 0, to = 3, by = 0.001) p <- numeric(length(loops)) bf <- numeric(length(loops)) d <- numeric(length(loops)) tval <- numeric(length(loops)) i <- 0 for(t in loops){ i <- i+1 bf[i] <- exp(BayesFactor::ttest.tstat(t, n1, n2)$bf)\np[i] <- 2*pt(t, ((n1 + n2) - 2), lower=FALSE)\ntval[i] <- t\nd[i] <- t * sqrt((1/n1)+(1/n2))\n}\n\nplot(p, bf, type=\"l\", lty=1, lwd=2, log = \"y\")\nabline(v = seq(0,1,0.1), h = c(0, 1/10, 1/3, 1, 3, 10), col = \"gray\", lty = 1)",
null,
"We can easily see which Bayes factor threshold corresponds to a specific p-value. For a Bayes factor of 1, we get a p-value of:\n\np[which.min(abs(bf-1))]\n## 0.0462172\n\nSo, as long as the observed p-value is smaller than 0.046 the data will provide stronger support for H1 than for H0.\n\nJustifyAlpha allows users to directly compute the alpha level that enables them to avoid the Lindley paradox through the functions ftestEvidence and ttestEvidence, which calculate the alpha level that is needed so that a significance p-value is always more likely under the alternative hypothesis than under the null hypothesis, based on a specification of a prior for the alternative model. For a two sample t-test with 100 participants per group, we can do this using the following function.\n\nres8 <- ttestEvidence(\"lindley\", 100, 100)[]\nres8\n## 0.04625576\n\nThis shows that an alpha level of at least 0.046 would be required to avoid the Lindley paradox. Of course, researchers can also use an informed prior, or use the the likelihood of the data under the effect size of the alternative hypothesis. There are many approaches to prevent Lindley’s paradox. All boil down to lowering the alpha level as a function of the sample size, but they differ slightly the relation between the sample size and the alpha level."
]
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null,
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pBq1osprf2QCdBkl1SJJpcDiEKnCzfENS8LIG11DisVhaCSmznFEBeBzhTfbVZlBGgqOdH5Nxx3QrX+MRHkuL2prwteVg+kr1DGloTs6ObW81lQ5Mxa3k6nABreGVUFEusDVRAdBK4762KCTmdviGteHkCa+kDkufGn6xuF70A0w9BRvH79mryE+sP6TqezN8Q1LzMSTdcHos6NP71mFQsimqF52rxORVxCxw2m5lP0cpcy0vpAF8T6QMRxTy/WrI6Np5tBciACpGVm9AzUTeOtGwGv0VvrWpi6lPHH8JLVsfHaNitIvB7JDE7Bdbt7Q1zz8gE63N2SI0DKYurpr6+/tDrtydhme4Csr9vdG+KalwtQfNjKuUcnKxfzEJH5QApA7NgUCVCNsS+oRhUAdDcIFhOAhJ3NUwYoVcZPLb8lNDWZAdoPzj1MYtBvVvJbU+0AImXfaxpmYfbX7e4jwTUvcy0s+CRbxBDqAzUCkE0cqPC63b0hrnmZSxkROylAwloYua2nfoBqTOdotRFeeGsFSJnGxwJAXnv56RwpOmI6B3VuPADy2stfTE0AkhdTiXPjAZDXXh5A0fT94l9Xzn2nLqaq58YDIK+9zEDigWYxlS0A5KiXv5h6IcJHOmzFTm2HuKAmVARQ3UIP5KiX1wMdTvbyvNkq/HkbASBHvfw4kPLPSgJAjnqrAiQl1SvnxqsprrQAkKPe0gApW5uFfWFySqua4qoRAHLUW74H2hf5OZ+fx8uRaCoyTQsAOeqt+ggTJa+FUWtjtACQo17eWtiNK2T8R16Np4tuth2hgJqQESCd5HwgumZi278a1IQKABo8+3CkK/qEMk3VVkp4hDnqZS6mrk5G0bnhEACaPS8PoDtB8M43D1JtoQeaZS9vEL1JnxJmN4gu0wwA1HUvpvHtNcILL7MH0gCEQOLMeXljoB3dQZdySiuWMnz38gAabM7dJK3KufHfYzHVb2/5xdSk0HhS20UtNM4XAHLUWx4gU6FxK7UdI4WakBagwe4DUUqRFwgS1URONOSxABBUSWogUTyx5+cP22gV5IyISLQ0kP4R9WMQlIrY1pOd1nN/Mfho79vLte1PhbxU4Wk9OzWVq4f8VOFpPYwje6AZUuHGwrp2F0J+qvC0HgAEmUQWmHo+/pdUaROCJBWc1jO4u4B5PGRQwWk9UrXxEiqzk77MQVKy9/jLMFz+QpNUojTidlimEdoKbLK3lx4fS5qpDyL83KYNp+umY2mV6z62/4CTz+Er0pq9c+5XMddAKCgwNbjBKTMVq8xO+jIHSUne7PDoS3Rmv2SOrlqmEfHF6VbQvxxtlrxnt5Lv6Uxy0WsGiL6u1e+WXVibCyh++ubEwWmthZVJgC1zkJTkjT626A/p+Fb4K5tG9MKoqzq+NqrwWNCI5J6QrZC9pp0Fahvi7+kG0x9Sz+pD64fvR9+vW/1u27H37LHub1T89AtSl6cFUJkU/DIHSUnebHPRaI+R2ZzdZ/qGEA3sLWtaIXs1b0+3IelO6J8gPyTNtgXZm2aJ9kkwlQ8t21BDXlj+9As2T0gZiUuPhMVUdkZimU1AZQ6S0lyHvh+0+b/r1BOB8EZNoFuheI/WyA6Q8hqsdHsz4gq9BoBk73hLH9lvSp9+0fYtKSMxOaSnQkbiuBUltiGWOYVDcx36D48yR8PdqPu28cav0K1QvP3wejSU/9zmutEVX1yz9GYNJolTvEdr8SOMfDyrNyNjQrsnNPd7F20glTISt54LWYnsjMRmAYo+PPJviTBvf0oPYFVv/C9LgLJJmM3N64efasfFVHuzm23h/U88nVi2au92PBaMxkC1A1SfGgXoaI0cOuretEfNKAgoNnStIG7IL5MbYnHdfhh7/3fbqg1DXd9KeOOZeSQqoEH0Vgnvv5geQMSRl+XUJEDJvMbWPNR03bI3HatYAlTiuhkQVl7iPfTeEcQEb+p14+DZZ0/0ZQ0qAkQeeVlOlQbRsawH0dFcWzeH1r0p9VnI3uypRD6Xqlz3aG3D2js0zO80A2MSTE17DcEH7iA6FX3kZUlVmcbH0sWAlSm/JgREmbPxxCk5DZO8JoC002LqM6bjDvQAVv0g9IeRVLluSq/u6Si9bZlpfCLNkZclVS2QqP/k1JgY7dOY40BiiSCephVVrjvyUvdDbUOPHt2p3ugP6QvdOIwIZn7wcvhCM3JMf2Aj9+9ygUTdkZdlVWYnfZmDpERvtpKhifbLF85C+EXLCJO7pu0H+dfNllOs2musviR5s0+ChoJur77rzn5vmxoI9icWllSZnfRlDpISvf3Rk4b+oJVGmBZT1UboF1Ml7/Ft/Yqu0obHa/RkifIa1kioNtDxJfpz+IlhMVUAyFwDYWoAQbMh+yMvIYhQiSMvIUhViSMvIUhVE0deQh6r5iMvoVkTqnNAlURM4+ev/otyQhAhujrH3MXv2mgM5J6IR9ib3yWj6CW6VisE5UWPgQbPLicnFv4e42jILP0g+oevK+REe6xc8YCxpOOJZ0kagPb+crlSUr3HAkCCiEr1P/xuMY0jvvMNpmOqAJAgTY3E+SsoEa0RABJEAoRJvKxkUpHG5lOA9oO3/n0/mq1eTKrYxgA9jfrt8zcVu+9S0znuJw+w+auAaKK72epgnN4yBui36YM+PtsoAuinqeMT2e67yEF0Ngo6fxVFohPtB3MfR39adxM+RgAFwbvPh282gzRzKgjeS76LmRHsvks7jU8gmtknu6g76e6CwWb8dQzQ25PXDrIyXAcL8f8T7L5LC9Dh/VUAJEoEKBtKJzsPUnCkAfYMAzR49nU6DsI0fqTBDw9uLAZ5gLIBTjIBG83CxgBN7L5LBSgbAC3dnIERoK2eLk7OfbAAKG/3XeQ0HovxoqIBz9zSlW/2Nu0AEuy+izitBw8uSaPBjDgGysaH2RgoB5Bo913ISCzWaH/c/oIwC8tRIgAk2n0XACpW9FR/+/lwEAee8wAlkZ/V5FEmAZS3+y4AZKGdLLB8L479jACaX5xsXRHHQILddwEgG8XTqvmP0/HOZC3sboRPut5FzMJGdt8FgHiaCThsBIB4AkCZABBPACgTAOIJAGUCQDwBoEwACKokAARVEgCCKgkAQZUEgKBKAkBQJQEgqJIAEFRJAAiqJAAEVRIAgirp//SL9BiFTJJZAAAAAElFTkSuQmCC",
null,
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",
null,
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pBq1osprf2QCdBkl1SJJpcDiEKnCzfENS8LIG11DisVhaCSmznFEBeBzhTfbVZlBGgqOdH5Nxx3QrX+MRHkuL2prwteVg+kr1DGloTs6ObW81lQ5Mxa3k6nABreGVUFEusDVRAdBK4762KCTmdviGteHkCa+kDkufGn6xuF70A0o6ijeP36tfyy+sP6TqezN8Q1LzMSTdcHos6NP71mFQsimqF92kTe16nEl3XcYGo+RS93KSOtD3RBrA9EHPf0Ys3q2Hi6GRoO8gBpmRk9A3XTeOtGwGv01roWpi5l/DG8ZHVsvLbNNBevRyrscgDQlL18gA53t+QIkLKYevrr6y+tTnsyttkeIOvrdveGuOblAhQftnLu0cnKxTxEZD6QAhA7NkUCVGPsC6pRBQDdDYLFBCBhZ/OUAcop46eOS0FTkRmg/eDcwyQG/WYlvzXVDiBSJXtYehZmf93uPhJc8zLXwoJPskUMoT5QcwAVxIEKr9vdG+Kal7mUEbGTAiSshZHbeqYEUDVvd2+Ia95aAVKm8bEAkNde5iNs7g8ZOmI6B3VuPADy2stfTE0AkhdTiXPjAZDXXh5A0fT94l9Xzn2nLqaq58YDIK+9zEDigWYxlS0A5KiXv5h6IcJHOmzFTm2HuKAmVARQ3UIP5KiX1wMdTvbyvNkq/HkbASBHvfw4kPLPSgJAjnqrAiQl1SvnxqsprrQAkKPe0gApW5uFfWFySqua4qoRAHLUW74H2hf5OZ+fx8uRaCoyTQsAOeqt+ggTJa+FUWtjtACQo17eWtiNK2T8R16Np4tuth2hgJqQESCd5HwgumZi278a1IQKABo8+3CkK/qEMk3VVkp4hDnqZS6mrk5G0bnhEACaPS8PoDtB8M43D1JtoQeaZS9vEL1JnxJmN4gu0wwA1HUvpvHtNcILL7MH0gCEQOLMeXljoB3dQZdySiuWMnz38gAabM7dJK3KufHfYzHVb2/5xdSk0HhS20UtNM4XAHLUWx4gU6FxK7UdI4WakBagwe4DUUqRFwgS1URONOSxABBUSWogUTyx5+cP22gV5IyISLQ0kP4R9WMQlIrY1pOd1nN/Mfho79vLte1PhbxU4Wk9OzWVq4f8VOFpPYwje6AZUuHGwrp2F0J+qvC0HgAEmUQWmHo+/pdUaROCJBWc1jO4u4B5PGRQwWk9UrXxEiqzk77MQVKy9/jLMFz+QpNUojTidlimEdoKbLK3lx4fS5qpDyL83KYNp+umY2mV6z62/4CTz+Er0pq9c+5XMddAKCgwNbjBKTMVq8xO+jIHSUne7PDoS3Rmv2SOrlqmEfHF6VbQvxxtlrxnt5Lv6Uxy0WsGiL6u1e+WXVibCyh++ubEwWmthZVJgC1zkJTkjT626A/p+Fb4K5tG9MKoqzq+NqrwWNCI5J6QrZC9pp0Fahvi7+kG0x9Sz+pD64fvR9+vW/1u27H37LHub1T89AtSl6cFUJkU/DIHSUnebHPRaI+R2ZzdZ/qGEA3sLWtaIXs1b0+3IelO6J8gPyTNtgXZm2aJ9kkwlQ8t21BDXlj+9As2T0gZiUuPhMVUdkZimU1AZQ6S0lyHvh+0+b/r1BOB8EZNoFuheI/WyA6Q8hqsdHsz4gq9BoBk73hLH9lvSp9+0fYtKSMxOaSnQkbiuBUltiGWOYVDcx36D48yR8PdqPu28cav0K1QvP3wejSU/9zmutEVX1yz9GYNJolTvEdr8SOMfDyrNyNjQrsnNPd7F20glTISt54LWYnsjMRmAYo+PPJviTBvf0oPYFVv/C9LgLJJmM3N64efasfFVHuzm23h/U88nVi2au92PBaMxkC1A1SfGgXoaI0cOuretEfNKAgoNnStIG7IL5MbYnHdfhh7/3fbqg1DXd9KeOOZeSQqoEH0Vgnvv5geQMSRl+XUJEDJvMbWPNR03bI3HatYAlTiuhkQVl7iPfTeEcQEb+p14+DZZ0/0ZQ0qAkQeeVlOlQbRsawH0dFcWzeH1r0p9VnI3uypRD6Xqlz3aG3D2js0zO80A2MSTE17DcEH7iA6FX3kZUlVmcbH0sWAlSm/JgREmbPxxCk5DZO8JoC002LqM6bjDvQAVv0g9IeRVLluSq/u6Si9bZlpfCLNkZclVS2QqP/k1JgY7dOY40BiiSCephVVrjvyUvdDbUOPHt2p3ugP6QvdOIwIZn7wcvhCM3JMf2Aj9+9ygUTdkZdlVWYnfZmDpERvtpKhifbLF85C+EXLCJO7pu0H+dfNllOs2musviR5s0+ChoJur77rzn5vmxoI9icWllSZnfRlDpISvf3Rk4b+oJVGmBZT1UboF1Ml7/Ft/Yqu0obHa/RkifIa1kioNtDxJfpz+IlhMVUAyFwDYWoAQbMh+yMvIYhQiSMvIUhViSMvIUhVE0deQh6r5iMvoVkTqnNAlURM4+ev/otyQhAhujrH3MXv2mgM5J6IR9ib3yWj6CW6VisE5UWPgQbPLicnFv4e42jILP0g+oevK+REe6xc8YCxpOOJZ0kagPb+crlSUr3HAkCCiEr1P/xuMY0jvvMNpmOqAJAgTY3E+SsoEa0RABJEAoRJvKxkUpHG5lOA9oO3/n0/mq1eTKrYxgA9jfrt8zcVu+9S0znuJw+w+auAaKK72epgnN4yBui36YM+PtsoAuinqeMT2e67yEF0Ngo6fxVFohPtB3MfR39adxM+RgAFwbvPh282gzRzKgjeS76LmRHsvks7jU8gmtknu6g76e6CwWb8dQzQ25PXDrIyXAcL8f8T7L5LC9Dh/VUAJEoEKBtKJzsPUnCkAfYMAzR49nU6DsI0fqTBDw9uLAZ5gLIBTjIBG83CxgBN7L5LBSgbAC3dnIERoK2eLk7OfbAAKG/3XeQ0HovxoqIBz9zSlW/2Nu0AEuy+izitBw8uSaPBjDgGysaH2RgoB5Bo913ISCzWaH/c/oIwC8tRIgAk2n0XACpW9FR/+/lwEAee8wAlkZ/V5FEmAZS3+y4AZKGdLLB8L479jACaX5xsXRHHQILddwEgG8XTqvmP0/HOZC3sboRPut5FzMJGdt8FgHiaCThsBIB4AkCZABBPACgTAOIJAGUCQDwBoEwACKokAARVEgCCKgkAQZUEgKBKAkBQJQEgqJIAEFRJAAiqJAAEVRIAgirp/xHV84zz020VAAAAAElFTkSuQmCC",
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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null
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http://oj.gdsyzx.edu.cn/problem.php?id=1430 | [
"## 1430: 自然数的拆分问题\n\n[上一题][提交][讨论版][状态][下一题]\n\n7=1+1+1+1+1+1+1\n\n7=1+1+1+1+1+2\n\n7=1+1+1+1+3\n\n7=1+1+1+2+2\n\n7=1+1+1+4\n\n7=1+1+2+3\n\n7=1+1+5\n\n7=1+2+2+2\n\n7=1+2+4\n\n7=1+3+3\n\n7=1+6\n\n7=2+2+3\n\n7=2+5\n\n7=3+4\n\n## 样例输入\n\n7\n\n## 样例输出\n\n1+1+1+1+1+1+1\n1+1+1+1+1+2\n1+1+1+1+3\n1+1+1+2+2\n1+1+1+4\n1+1+2+3\n1+1+5\n1+2+2+2\n1+2+4\n1+3+3\n1+6\n2+2+3\n2+5\n3+4\n\n\n## 标签\n\n[上一题][提交][讨论版][状态][下一题]"
]
| [
null
]
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https://ch.mathworks.com/matlabcentral/profile/authors/1297420 | [
"Community Profile",
null,
"Varun Gandhi\n\nMathWorks\n\nLast seen: Today Active since 2012\n\nStatistics\n\nAll\n•",
null,
"•",
null,
"•",
null,
"•",
null,
"•",
null,
"•",
null,
"•",
null,
"Content Feed\n\nView by\n\nSubmitted\n\nMACOPEN\nMACOPEN can be used to open a file or directory outside MATLAB on Mac OSX\n\nSubmitted\n\nTranslate strings from one language to another\nTRANSLATE uses translate.google.com to translate a string from one language to another",
null,
"Submitted\n\nENDTASK is used to close tasks/processes running in Windows/Linux by providing the process name.\n\nSubmitted\n\nISPROCESS\nISPROCESS checks if the given process name is running on the system\n\nSubmitted\n\nUISETSCREENPIXELSPERINCH\nTool that can be used to easily set the Root Property: 'ScreenPixelsPerInch'",
null,
"Solved\n\nMost nonzero elements in row\nGiven the matrix a, return the index r of the row with the most nonzero elements. Assume there will always be exactly one row th...\n\n10 years ago\n\nSolved\n\nRemove any row in which a NaN appears\nGiven the matrix A, return B in which all the rows that have one or more <http://www.mathworks.com/help/techdoc/ref/nan.html NaN...\n\n10 years ago\n\nSolved\n\nRemove the vowels\nRemove all the vowels in the given phrase. Example: Input s1 = 'Jack and Jill went up the hill' Output s2 is 'Jck nd Jll wn...\n\n10 years ago\n\nSolved\n\nFind the numeric mean of the prime numbers in a matrix.\nThere will always be at least one prime in the matrix. Example: Input in = [ 8 3 5 9 ] Output out is 4...\n\n10 years ago\n\nSolved\n\nCheck if sorted\nCheck if sorted. Example: Input x = [1 2 0] Output y is 0\n\n10 years ago\n\nSolved\n\nFinding Perfect Squares\nGiven a vector of numbers, return true if one of the numbers is a square of one of the other numbers. Otherwise return false. E...\n\n10 years ago\n\nSolved\n\nFibonacci sequence\nCalculate the nth Fibonacci number. Given n, return f where f = fib(n) and f(1) = 1, f(2) = 1, f(3) = 2, ... Examples: Inpu...\n\n10 years ago\n\nSolved\n\nWeighted average\nGiven two lists of numbers, determine the weighted average. Example [1 2 3] and [10 15 20] should result in 33.333...\n\n10 years ago\n\nSolved\n\nMake a checkerboard matrix\nGiven an integer n, make an n-by-n matrix made up of alternating ones and zeros as shown below. The a(1,1) should be 1. Example...\n\n10 years ago\n\nSolved\n\nDetermine whether a vector is monotonically increasing\nReturn true if the elements of the input vector increase monotonically (i.e. each element is larger than the previous). Return f...\n\n10 years ago\n\nSolved\n\nSwap the first and last columns\nFlip the outermost columns of matrix A, so that the first column becomes the last and the last column becomes the first. All oth...\n\n10 years ago\n\nSolved\n\nTriangle Numbers\nTriangle numbers are the sums of successive integers. So 6 is a triangle number because 6 = 1 + 2 + 3 which can be displa...\n\n10 years ago\n\nSolved\n\nFind all elements less than 0 or greater than 10 and replace them with NaN\nGiven an input vector x, find all elements of x less than 0 or greater than 10 and replace them with NaN. Example: Input ...\n\n10 years ago\n\nSolved\n\nColumn Removal\nRemove the nth column from input matrix A and return the resulting matrix in output B. So if A = [1 2 3; 4 5 6]; and ...\n\n10 years ago\n\nSolved\n\nGiven a and b, return the sum a+b in c.\n\n10 years ago\n\nSolved\n\nDetermine if input is odd\nGiven the input n, return true if n is odd or false if n is even.\n\n10 years ago\n\nSolved\n\nFind the sum of all the numbers of the input vector\nFind the sum of all the numbers of the input vector x. Examples: Input x = [1 2 3 5] Output y is 11 Input x ...\n\n10 years ago\n\nSolved\n\nTimes 2 - START HERE\nTry out this test problem first. Given the variable x as your input, multiply it by two and put the result in y. Examples:...\n\n10 years ago\n\nSolved\n\nSelect every other element of a vector\nWrite a function which returns every other element of the vector passed in. That is, it returns the all odd-numbered elements, s...\n\n10 years ago\n\nSolved\n\nMake the vector [1 2 3 4 5 6 7 8 9 10]\nIn MATLAB, you create a vector by enclosing the elements in square brackets like so: x = [1 2 3 4] Commas are optional, s...\n\n10 years ago"
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https://electronics.stackexchange.com/questions/142112/balun-matching-network-question | [
"# Balun/matching network question\n\nI am having problem to verify what an app note (AN068) explains to calculate Balun values. I would appreciate if someone could tell me what/where am I doing wrong?\n\nThe summary of the RF part:",
null,
"Blue part is the DC blocking cap, C10-L1 and L3-C11 are Balun, the grey part is PI network. The IC's (CC2500) datasheet defines the optimum load at RF_P and RF_N as 80+j74 ohm.\n\nFrom figure 6 on page 7, it shows the differential circuit, and the below figure (figure 7) shows the single part where the impedance is divided by 2.",
null,
"\"It ignores the dc blocking cap as the values are large\". It marks the trace to take the impedance of the trace in calculation. 20 + j0 is the Thevenin equivalent impedance (Zout).\n\nHere is the Gerber view of the design:",
null,
"The app note suggests to calculate the impedance of the traces (from pad to pad) for the balun part. Both paths have the same length. The left path: C9 to L3: 0.192mm; L3 to C11: 0.177 mm; C11 to C12 = 0.185 mm; the total length is 0.554 mm. The width of the trace is 0.254 mm, the gerber document says that the FR4 thickness is 1.6 mm. The app note says to enter permittivity for 2.45Gz as 4.1, tan loss 0.0155.\n\nI enter the values measured from the Gerber files and the app note to NI's line calculator:",
null,
"It shows 135.674 ohm impedance and 2.67941 degree electrical length.\n\nThen as the app note suggests, I define the source impedance as 40 + j37 ohm (blue circle) and load impedance as 20 + j0 ohm (red circle) on the Smith Chart (there is a small circuit representation on the left bottom side). After that, I added a transmission line and define the parameters from the line calculator (135.674 ohm, 2.67941 degree) (the program does not allow to enter precise numbers, therefore I select the closest possible values). Finally, I added a shunt capacitor with 1pF and 1.2nH series inductor as the final design uses those values.",
null,
"However, it get a different smith chart that the impedance doesn't match as the app note shows.",
null,
"I get the it matched if I enter 335 ohm for impedance of TL and keep the other values the same. I need to enter weird values in order to get the 335 impedance on the line calculator.\n\nWhere do I do wrong?\n\nEDIT 1: I guess the app note says to measure the length from the radio pins, then MCU to C9 is 0.506 mm. The total length is 1.06 mm. It only changes the electrical length to 5.12667 degree which is almost the same smith chart as I was using 4 degree (smallest possible on the program I use) on the above smith chart.\n\n• The smith chart from the white paper shows info on the transmission line. It's 50ohms and 25.566deg long. That makes the cap roughly 1.33pF and the inductor 2.4nH. – curtis Jan 14 '15 at 8:55\n• What did TI say when you asked them? They have forums staffed by people who know the chip very well. Note that there are also pre-made baluns available by Johanson, Anaren, etc. – Fix It Until It's Broken Feb 11 '15 at 16:56"
]
| [
null,
"https://i.stack.imgur.com/LIEla.png",
null,
"https://i.stack.imgur.com/mWTqJ.png",
null,
"https://i.stack.imgur.com/F8gKd.png",
null,
"https://i.stack.imgur.com/2XVpr.png",
null,
"https://i.stack.imgur.com/Oq39i.png",
null,
"https://i.stack.imgur.com/lAj8z.png",
null
]
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https://www.hackmath.net/en/math-problem/1799 | [
"# The hall\n\nThe hall had a rectangular ground plan, one dimension 20 m longer than the other. After rebuilding, the length of the hall declined by 5 m, and the width increased by 10 m. The floor area increased by 300 m2. What were the original dimensions of the hall?\n\na = 50 m\nb = 30 m\n\n### Step-by-step explanation:",
null,
"Did you find an error or inaccuracy? Feel free to write us. Thank you!\n\nTips for related online calculators\nAre you looking for help with calculating roots of a quadratic equation?\nDo you have a linear equation or system of equations and looking for its solution? Or do you have a quadratic equation?\nDo you want to convert length units?\n\n#### Grade of the word problem:\n\nWe encourage you to watch this tutorial video on this math problem:"
]
| [
null,
"https://www.hackmath.net/img/99/lucerna.jpg",
null
]
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https://www.geomesa.org/documentation/2.0.2/user/convert/json.html | [
"# 17.4. JSON Converter¶\n\nThe JSON converter handles JSON files. To use the JSON converter, specify type = \"json\" in your converter definition.\n\n## 17.4.1. Configuration¶\n\nThe JSON converter supports parsing files in single-line mode or in multi-line mode. In single-line mode, each line of an input file should be a valid JSON document; in multi-line mode, the entire input file should be a single valid JSON document. In order to support JSON path expressions, each JSON document is fully parsed into memory. For large documents, this may take considerable time and memory. Thus, it is usually better to use single-line mode when possible. Line mode may be specified by options.line-mode = \"single\" or options.line-mode = \"multi\" in your converter definition. If nothing is specified, single-line mode is used.\n\nSince a single JSON document may contain multiple features, the JSON parser supports a JSONPath expression pointing to each feature element. This can be specified using the feature-path element.\n\nThe fields element in a JSON converter supports two additional attributes, path and json-type. path should be a JSONPath expression, which is relative to the feature-path, if defined (above). For absolute paths, root-path may be used instead of path. json-type should specify the type of JSON field being read. Valid values are: string, float, double, integer, long, boolean, geometry, array and object. The value will be appropriately typed, and available in the transform element as $0. Geometry types can handle either WKT strings or GeoJSON geometry objects. ## 17.4.2. Transform Functions¶ The transform element supports referencing the JSON element through $0. Each column will initially be typed according to the field’s json-type. Most types will be converted to the equivalent Java class, e.g. java.lang.Integer, etc. array and object types will be raw JSON elements, and thus usually require further processing (e.g. jsonList or jsonMap, below).\n\nIn addition to the standard functions in Transformation Function Overview, the JSON converter provides the following JSON-specific functions:\n\n### 17.4.2.1. jsonToString¶\n\nThis will convert a JSON element to a string. It can be useful for quickly representing a complex object, for example in order to create a feature ID based on the hash of a row.\n\n### 17.4.2.2. jsonList¶\n\nThis function converts a JSON array element into a java.util.List. It requires two parameters; the first is the type of the list elements as a string, and the second is a JSON array. The type of list elements must be one of the types defined in GeoTools Feature Types. See below for an example.\n\n### 17.4.2.3. jsonMap¶\n\nThis function converts a JSON object element into a java.util.Map. It requires three parameters; the first is the type of the map key elements as a string, the second is the type of the map value elements as a string, and the third is a JSON object. The type of keys and values must be one of the types defined in GeoTools Feature Types. See below for an example.\n\n### 17.4.2.4. mapToJson¶\n\nThis function converts a java.util.Map into a JSON string. It requires a single parameter, which must be a java.util.Map. It can be useful for storing complex JSON as a single attribute, which can then be queried using GeoMesa’s JSON attribute support. See JSON Attributes for more information.\n\n## 17.4.3. Example Usage¶\n\nAssume the following SimpleFeatureType:\n\ngeomesa.sfts.example = {\nattributes = [\n{ name = \"name\", type = \"String\" }\n{ name = \"age\", type = \"Integer\" }\n{ name = \"weight\", type = \"Double\" }\n{ name = \"hobbies\", type = \"List[String]\" }\n{ name = \"skills\", type = \"Map[String,Int]\" }\n{ name = \"source\", type = \"String\" }\n{ name = \"geom\", type = \"Point\" }\n]\n}\n\n\nAnd the following JSON document:\n\n{\n\"DataSource\": { \"name\": \"myjson\" },\n\"Features\": [\n{\n\"id\": 1,\n\"name\": \"phil\",\n\"physicals\": {\n\"age\": 32,\n\"weight\": 150.2\n},\n\"hobbies\": [ \"baseball\", \"soccer\" ],\n\"languages\": {\n\"java\": 100,\n\"scala\": 70\n},\n\"geometry\": { \"type\": \"Point\", \"coordinates\": [55, 56] }\n},\n{\n\"id\": 2,\n\"name\": \"fred\",\n\"physicals\": {\n\"age\": 33,\n\"weight\": 150.1\n},\n\"hobbies\": [ \"archery\", \"tennis\" ],\n\"languages\": {\n\"c++\": 10,\n\"fortran\": 50\n},\n\"geometry\": { \"type\": \"Point\", \"coordinates\": [45, 46] }\n}\n]\n}\n\n\nYou could ingest with the following converter:\n\ngeomesa.converters.myjson = {\ntype = \"json\"\nid-field = \"$id\" feature-path = \"$.Features[*]\"\noptions = {\nline-mode = \"multi\"\n}\nfields = [\n{ name = \"id\", json-type = \"integer\", path = \"$.id\", transform = \"toString($0)\" }\n{ name = \"name\", json-type = \"string\", path = \"$.name\", transform = \"trim($0)\" }\n{ name = \"age\", json-type = \"integer\", path = \"$.physicals.age\", } { name = \"weight\", json-type = \"double\", path = \"$.physicals.weight\" }\n{ name = \"hobbies\", json-type = \"array\", path = \"$.hobbies\", transform = \"jsonList('string',$0)\" }\n{ name = \"skills\", json-type = \"map\", path = \"$.languages\", transform = \"jsonMap('string','int',$0)\" }\n{ name = \"geom\", json-type = \"geometry\", path = \"$.geometry\", transform = \"point($0)\" }\n{ name = \"source\", json-type = \"string\", root-path = \"\\$.DataSource.name\" }\n]\n}"
]
| [
null
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