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| | [[File:Exp series.gif|right|thumb|An [[animation]] that shows how a Taylor series can be used to [[approximate]] a function. The blue line shows the [[exponential function]] <math>f(x)=e^{x}</math>. The red lines show the [[sum]] of ''n'' [[derivatives]] -- that is, ''n''+1 [[term]]s in the Taylor series. As ''n'' gets bigger, the red line gets closer to the blue line.]] | | [[File:Exp series.gif|right|thumb|An [[animation]] that shows how a Taylor series can be used to [[approximate]] a function. The blue line shows the [[exponential function]] <math>f(x)=e^{x}</math>. The red lines show the [[sum]] of ''n'' [[derivatives]] -- that is, ''n''+1 [[term]]s in the Taylor series. As ''n'' gets bigger, the red line gets closer to the blue line.]] |
| − | A '''Taylor series''' is an idea used in [[computer science]], [[calculus]], chemistry, physics and other kinds of higher-level [[mathematics]]. It is a [[Series (mathematics)|series]] that is used to create an [[estimate]] (guess) of what a [[Function (mathematics)|function]] looks like. There is also a special kind of Taylor series called a '''Maclaurin series'''. | + | A '''Taylor series''' is an idea used in [[computer science]], [[calculus]], chemistry, physics and other kinds of higher-level [[mathematics]]. It is a [[Series (mathematics)|series]] that is used to create an [[estimate]] (guess) of what a [[Function (mathematics)|function]] [[approximation theory|looks like]]. There is also a special kind of Taylor series called a '''Maclaurin series'''. |
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| | The theory behind the Taylor series is that if a point is chosen on the [[coordinate plane]] ([[x-axis|x-]] and [[y-axis|y-axes]]), then it is possible to guess what a function will look like in the area around that point. This is done by taking the [[Derivative (mathematics)|derivative]]s of the function and adding them all together. The idea is that it is possible to add the [[infinite]] number of derivatives and come up with a single [[finite]] sum. | | The theory behind the Taylor series is that if a point is chosen on the [[coordinate plane]] ([[x-axis|x-]] and [[y-axis|y-axes]]), then it is possible to guess what a function will look like in the area around that point. This is done by taking the [[Derivative (mathematics)|derivative]]s of the function and adding them all together. The idea is that it is possible to add the [[infinite]] number of derivatives and come up with a single [[finite]] sum. |
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| | The [[Ancient Greece|Ancient Greek]] [[philosopher]] [[Zeno of Elea]] first came up with the idea of this series. The [[paradox]] called "[https://en.m.wikipedia.org/wiki/Zeno's_paradoxes Zeno's paradox]" is the result. He believed that it would be impossible to add an [[infinity|infinite]] number of values and get a single [[finite]] value as a result. | | The [[Ancient Greece|Ancient Greek]] [[philosopher]] [[Zeno of Elea]] first came up with the idea of this series. The [[paradox]] called "[https://en.m.wikipedia.org/wiki/Zeno's_paradoxes Zeno's paradox]" is the result. He believed that it would be impossible to add an [[infinity|infinite]] number of values and get a single [[finite]] value as a result. |
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| − | Another Greek philosopher, [[Aristotle]], came up with an answer to the philosophical question. It was [[Archimedes]], however, who came up with a mathematical solution using his [[method of exhaustion]]. He was able to prove that when something is split up into an infinite number of tiny pieces, they will still add up to a single whole when all of them are added back together.<ref>{{cite book|last=Kline|first=M|year=1990|title=Mathematical Thought from Ancient to Modern Times|url=https://archive.org/details/mathematicalthou00klin|publisher=Oxford University Press|pages=[https://archive.org/details/mathematicalthou00klin/page/n438 35]-37}}</ref> The ancient [[China|Chinese]] [[mathematician]] [[Liu Hui]] proved the same thing several hundred years later.<ref>{{cite book|last1=Boyer|first1=C|last2=Merzbach|first2=U|year=1991|title=A History of Mathematics|url=https://archive.org/details/historymathemati00boye_328|publisher=John Wiley and Sons|pages=[https://archive.org/details/historymathemati00boye_328/page/n221 202]-203}}</ref> | + | Another Greek philosopher, [[Aristotle]], came up with an answer to the philosophical question. It was [[Archimedes]], however, who came up with a mathematical solution using his [[method of exhaustion]]. He was able to prove that when something is split up into an infinite number of tiny pieces, they will still add up to a single whole when all of them are added back together.<ref>{{cite book|last=Kline|first=M|year=1990|title=Mathematical Thought from Ancient to Modern Times|url=https://archive.org/details/mathematicalthou00klin|publisher=Oxford University Press|pages=[https://archive.org/details/mathematicalthou00klin/page/n438 35]-37|isbn=978-0-19-506136-9}}</ref> The ancient [[China|Chinese]] [[mathematician]] [[Liu Hui]] proved the same thing several hundred years later.<ref>{{cite book|last1=Boyer|first1=C|last2=Merzbach|first2=U|year=1991|title=A History of Mathematics|url=https://archive.org/details/historymathemati00boye_328|publisher=John Wiley and Sons|pages=[https://archive.org/details/historymathemati00boye_328/page/n221 202]-203|isbn=9780471543978}}</ref> |
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| | The earliest known examples of the Taylor series are the work of [[Mādhava of Sañgamāgrama]] in [[India]] in the 1300s.<ref name="MAT 314">{{cite web| publisher=Canisius College| work=MAT 314| url=http://www.canisius.edu/topos/rajeev.asp| title=Neither Newton nor Leibniz - The Pre-History of Calculus and Celestial Mechanics in Medieval Kerala| accessdate=2006-07-09| archive-date=2006-08-06| archive-url=https://web.archive.org/web/20060806040307/http://www.canisius.edu/topos/rajeev.asp| url-status=dead}}</ref> Later [[Indian mathematics|Indian mathematicians]] wrote about his work with the [[trigonometric functions]] of [[sine]], [[cosine]], [[tangent]], and [[arctangent]]. None of Mādhava's writings or records still exists today. Other mathematicians based their work on Mādhava's discoveries and worked more with these series until the 1500s. | | The earliest known examples of the Taylor series are the work of [[Mādhava of Sañgamāgrama]] in [[India]] in the 1300s.<ref name="MAT 314">{{cite web| publisher=Canisius College| work=MAT 314| url=http://www.canisius.edu/topos/rajeev.asp| title=Neither Newton nor Leibniz - The Pre-History of Calculus and Celestial Mechanics in Medieval Kerala| accessdate=2006-07-09| archive-date=2006-08-06| archive-url=https://web.archive.org/web/20060806040307/http://www.canisius.edu/topos/rajeev.asp| url-status=dead}}</ref> Later [[Indian mathematics|Indian mathematicians]] wrote about his work with the [[trigonometric functions]] of [[sine]], [[cosine]], [[tangent]], and [[arctangent]]. None of Mādhava's writings or records still exists today. Other mathematicians based their work on Mādhava's discoveries and worked more with these series until the 1500s. |
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| − | [[James Gregory (mathematician)|James Gregory]], a [[Scotland|Scottish]] mathematician, worked in this area in the 1600s. Gregory studied the Taylor series and published several Maclaurin series. In 1715, [[Brook Taylor]] discovered a general method for applying the series to all [[function (mathematics)|functions]]. (All of the previous research showed how to apply the method to only specific functions.)<ref>{{cite book|last=Taylor|first=Brook|title=Methodus Incrementorum Directa et Inversa|language=Latin|location=London|year=1715|chapter=Proposition VII, Theorem 3, Corollary 2|pages=21-23}} ''cited in'' {{cite book|last=Struik|first=D.J.|title=A Source Book in Mathematics 1200-1800|publisher=Harvard University Press|location=Cambridge, Massachusetts|year=1969|pages=329-332}}</ref> [[:en:Colin_Maclaurin|Colin Maclaurin]] published a special case of the Taylor series in the 1700s. This series, which is based around [[zero]], is called the ''Maclaurin series''. | + | [[James Gregory (mathematician)|James Gregory]], a [[Scotland|Scottish]] mathematician, worked in this area in the 1600s. Gregory studied the Taylor series and published several Maclaurin series. In 1715, [[Brook Taylor]] discovered a general method for applying the series to all [[function (mathematics)|functions]]. (All of the previous research showed how to apply the method to only specific functions.)<ref>{{cite book|last=Taylor|first=Brook|title=Methodus Incrementorum Directa et Inversa|language=Latin|location=London|year=1715|chapter=Proposition VII, Theorem 3, Corollary 2|pages=21–23}} ''cited in'' {{cite book|last=Struik|first=D.J.|title=A Source Book in Mathematics 1200-1800|url=https://archive.org/details/sourcebookinmath0000stru|publisher=Harvard University Press|location=Cambridge, Massachusetts|year=1969|pages=[https://archive.org/details/sourcebookinmath0000stru/page/329 329]–332}}</ref> [[:en:Colin_Maclaurin|Colin Maclaurin]] published a special case of the Taylor series in the 1700s. This series, which is based around [[zero]], is called the ''Maclaurin series''. |
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| | == Definition == | | == Definition == |
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| | Where <math>B_{n}</math> is the nth [[Bernoulli number]], and <math>\ln</math> is the [[natural logarithm]]. | | Where <math>B_{n}</math> is the nth [[Bernoulli number]], and <math>\ln</math> is the [[natural logarithm]]. |
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| − | == References cite 3 is missing. == | + | == References == |
| | {{reflist}} | | {{reflist}} |
| | {{authority control}} | | {{authority control}} |
| | [[Category:Calculus]] | | [[Category:Calculus]] |
| − | [[pl:Wzór Taylora#Szereg Taylora]] | + | [[Category:Sequences and series]] |