﻿{"id":4363,"date":"2013-12-16T06:05:45","date_gmt":"2013-12-15T21:05:45","guid":{"rendered":"http:\/\/fujiitoshiki.com\/improvesociety\/?p=4363"},"modified":"2014-08-01T19:17:43","modified_gmt":"2014-08-01T10:17:43","slug":"taylor-series","status":"publish","type":"post","link":"https:\/\/www.fujiitoshiki.com\/improvesociety\/?p=4363","title":{"rendered":"Taylor series"},"content":{"rendered":"<div class=\"theContentWrap-ccc\"><blockquote>\n<p>The Taylor series for f(x) about x = a is defined as<\/p>\n<p><img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+f%28x%29+%3D+f%28a%29+%2B+f%27%28a%29%28x+-+a%29+%2B+%5Cfrac%7Bf%27%27%28a%29%28x+-+a%29%5E2%7D%7B2%21%7D+%2B+%5Ccdots+%2B+%5Cfrac%7Bf%5E%7Bn+-1%7D%28a%29%28x+-+a%29%5E%7Bn-1%7D%7D%7B%28n+-1%29%21%7D+%2B+R_n&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle f(x) = f(a) + f&#039;(a)(x - a) + \\frac{f&#039;&#039;(a)(x - a)^2}{2!} + \\cdots + \\frac{f^{n -1}(a)(x - a)^{n-1}}{(n -1)!} + R_n' title='\\displaystyle f(x) = f(a) + f&#039;(a)(x - a) + \\frac{f&#039;&#039;(a)(x - a)^2}{2!} + \\cdots + \\frac{f^{n -1}(a)(x - a)^{n-1}}{(n -1)!} + R_n' class='latex' \/>(a)<br \/>\nwhere <img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+R_n+%3D+%5Cfrac%7Bf%5En%28x+-+n%29%5En%7D%7Bn%21%7D&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle R_n = \\frac{f^n(x - n)^n}{n!}' title='\\displaystyle R_n = \\frac{f^n(x - n)^n}{n!}' class='latex' \/>, x<sub>0<\/sub> between a and x.(b)<br \/>\nis called the reminder and where it is supposed that f(x) has derivatives of order n at least. The case where n = 1 is often called law of the mean or mean-value theorem and can be written as<br \/>\n<img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+%5Cfrac%7Bf%28x%29+-f%28a%29%7D%7Bx+-+a%7D+%3D+f%27%28x_0%29&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle \\frac{f(x) -f(a)}{x - a} = f&#039;(x_0)' title='\\displaystyle \\frac{f(x) -f(a)}{x - a} = f&#039;(x_0)' class='latex' \/>, x<sub>0<\/sub> between a and x (c)<\/p>\n<p>The infinite series corresponding to (a), also called the formal Taylor series for f(x), will converge in some interval if <img src='https:\/\/s0.wp.com\/latex.php?latex=%5Clim%5Climits_%7Bn+%5Crightarrow+%5Cinfty%7DR_n+%3D+0&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\lim\\limits_{n \\rightarrow \\infty}R_n = 0' title='\\lim\\limits_{n \\rightarrow \\infty}R_n = 0' class='latex' \/> in this interval. Some important Taylor series together with their intervals of convergence are as follows. <\/p>\n<ol>\n<li><img src='https:\/\/s0.wp.com\/latex.php?latex=%5Cdisplaystyle+e%5En+%3D+1+%2B+x+%2B+%5Cfrac%7Bx%5E2%7D%7B2%21%7D+%2B+%5Cfrac%7Bx%5E3%7D%7B3%21%7D+%2B%5Cfrac%7Bx%5E4%7D%7B4%21%7D+%2B+%5Ccdots%5C+-%5Cinfty+%3C+x+%3C+%5Cinfty%26%2391%3B%2Flatex%26%2393%3B%3C%2Fli%3E++%3Cli%3E%5Blatex%5D%5Cdisplaystyle+%5Csin+x+%3D+x+-+%5Cfrac%7Bx%5E3%7D%7B3%21%7D+%2B+%5Cfrac%7Bx%5E5%7D%7B5%21%7D+-+%5Cfrac%7Bx%5E7%7D%7B7%21%7D+%2B+%5Ccdots%5C+-%5Cinfty+%3C+x+%3C+%5Cinfty%26%2391%3B%2Flatex%26%2393%3B%3C%2Fli%3E++%3Cli%3E%5Blatex%5D%5Cdisplaystyle+%5Ccos+x+%3D+1+-+%5Cfrac%7Bx%5E2%7D%7B2%21%7D+%2B+%5Cfrac%7Bx%5E4%7D%7B4%21%7D+-+%5Cfrac%7Bx%5E6%7D%7B6%21%7D+%2B+%5Ccdots%5C+-%5Cinfty+%3C+x+%3C+%5Cinfty%26%2391%3B%2Flatex%26%2393%3B%3C%2Fli%3E++%3Cli%3E%5Blatex%5D%5Cdisplaystyle+%5Cln%281+%2B+x%29+%3D+x+-+%5Cfrac%7Bx%5E2%7D%7B2%21%7D+%2B+%5Cfrac%7Bx%5E3%7D%7B3%21%7D+-+%5Cfrac%7Bx%5E4%7D%7B4%21%7D+%2B+%5Ccdots%5C+-1+%3C+x+%5Cle+1%26%2391%3B%2Flatex%26%2393%3B%3C%2Fli%3E++%3Cli%3E%5Blatex%5D%5Cdisplaystyle+%5Ctan%5E%7B-1%7Dx+%3D+x+-+%5Cfrac%7Bx%5E3%7D%7B3%21%7D+%2B+%5Cfrac%7Bx%5E5%7D%7B5%21%7D+-+%5Cfrac%7Bx%5E7%7D%7B7%21%7D+%2B+%5Ccdots%5C+-1+%5Cle+x+%5Cle+1&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\displaystyle e^n = 1 + x + \\frac{x^2}{2!} + \\frac{x^3}{3!} +\\frac{x^4}{4!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\sin x = x - \\frac{x^3}{3!} + \\frac{x^5}{5!} - \\frac{x^7}{7!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\cos x = 1 - \\frac{x^2}{2!} + \\frac{x^4}{4!} - \\frac{x^6}{6!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\ln(1 + x) = x - \\frac{x^2}{2!} + \\frac{x^3}{3!} - \\frac{x^4}{4!} + \\cdots\\ -1 &lt; x \\le 1&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\tan^{-1}x = x - \\frac{x^3}{3!} + \\frac{x^5}{5!} - \\frac{x^7}{7!} + \\cdots\\ -1 \\le x \\le 1' title='\\displaystyle e^n = 1 + x + \\frac{x^2}{2!} + \\frac{x^3}{3!} +\\frac{x^4}{4!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\sin x = x - \\frac{x^3}{3!} + \\frac{x^5}{5!} - \\frac{x^7}{7!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\cos x = 1 - \\frac{x^2}{2!} + \\frac{x^4}{4!} - \\frac{x^6}{6!} + \\cdots\\ -\\infty &lt; x &lt; \\infty&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\ln(1 + x) = x - \\frac{x^2}{2!} + \\frac{x^3}{3!} - \\frac{x^4}{4!} + \\cdots\\ -1 &lt; x \\le 1&#091;\/latex&#093;&lt;\/li&gt;  &lt;li&gt;&lt;img src=&#039;https:\/\/s0.wp.com\/latex.php?latex&#038;bg=T&#038;fg=000000&#038;s=0&#039; alt=&#039;&#039; title=&#039;&#039; class=&#039;latex&#039; \/&gt;\\displaystyle \\tan^{-1}x = x - \\frac{x^3}{3!} + \\frac{x^5}{5!} - \\frac{x^7}{7!} + \\cdots\\ -1 \\le x \\le 1' class='latex' \/><\/li>\n<\/ol>\n<p>A series of the form <img src='https:\/\/s0.wp.com\/latex.php?latex=%5Csum_%7Bn%3D0%7D%5E%7B%5Cinfty%7Dc_n%28x+-+a%29%5En&#038;bg=T&#038;fg=000000&#038;s=0' alt='\\sum_{n=0}^{\\infty}c_n(x - a)^n' title='\\sum_{n=0}^{\\infty}c_n(x - a)^n' class='latex' \/> is often called a power series. Such power series are uniformly convergent in any interval which lies entirely within the interval of convergence. <\/p>\n<\/blockquote>\n<p><iframe src=\"\/\/rcm-fe.amazon-adsystem.com\/e\/cm?lt1=_blank&#038;bc1=000000&#038;IS2=1&#038;bg1=FFFFFF&#038;fc1=000000&#038;lc1=0000FF&#038;t=fujiitoshiki-22&#038;o=9&#038;p=8&#038;l=as4&#038;m=amazon&#038;f=ifr&#038;ref=ss_til&#038;asins=0071635408\" style=\"width:120px;height:240px;\" scrolling=\"no\" marginwidth=\"0\" marginheight=\"0\" frameborder=\"0\"><\/iframe><\/p>\n<\/div>","protected":false},"excerpt":{"rendered":"<p>The Taylor series for f(x) about x = a is defined as (a) where , x0 between a and x.(b) is called the reminder &hellip; <a href=\"https:\/\/www.fujiitoshiki.com\/improvesociety\/?p=4363\" class=\"more-link\"><span class=\"screen-reader-text\">&#8220;Taylor series&#8221; \u306e<\/span>\u7d9a\u304d\u3092\u8aad\u3080<\/a><\/p>\n","protected":false},"author":1,"featured_media":6040,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_crdt_document":"","_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[9],"tags":[],"class_list":["post-4363","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-mathematics"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4363","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=4363"}],"version-history":[{"count":5,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4363\/revisions"}],"predecessor-version":[{"id":6073,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/posts\/4363\/revisions\/6073"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=\/wp\/v2\/media\/6040"}],"wp:attachment":[{"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=4363"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=4363"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.fujiitoshiki.com\/improvesociety\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=4363"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}