{"id":405,"date":"2025-02-13T19:44:39","date_gmt":"2025-02-13T19:44:39","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus2\/chapter\/integration-using-substitution-learn-it-2\/"},"modified":"2025-02-13T19:44:39","modified_gmt":"2025-02-13T19:44:39","slug":"integration-using-substitution-learn-it-2","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus2\/chapter\/integration-using-substitution-learn-it-2\/","title":{"raw":"Integration using Substitution: Learn It 2","rendered":"Integration using Substitution: Learn It 2"},"content":{"raw":"\n<h2>Substitution for Definite Integrals<\/h2>\n<p id=\"fs-id1170573387843\">Substitution can be used with definite integrals, too. However, using substitution to evaluate a definite integral requires a change to the limits of integration. If we change variables in the integrand, the limits of integration change as well.<\/p>\n<section class=\"textbox keyTakeaway\">\n<div>\n<h3>substitution with definite integrals<\/h3>\n<p id=\"fs-id1170570999523\">Let [latex]u=g(x)[\/latex] and let [latex]{g}^{\\text{\u2032}}[\/latex] be continuous over an interval [latex]\\left[a,b\\right],[\/latex] and let [latex]f[\/latex] be continuous over the range of [latex]u=g(x).[\/latex] Then,<\/p>\n<div id=\"fs-id1170571189407\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{a}^{b}f(g(x)){g}^{\\prime }(x)dx={\\displaystyle\\int }_{g(a)}^{g(b)}f(u)du[\/latex]<\/div>\n<\/div>\n<\/section>\n<p id=\"fs-id1170573502228\">Although we will not formally prove this theorem, we justify it with some calculations here. From the substitution rule for indefinite integrals, if [latex]F(x)[\/latex] is an antiderivative of [latex]f(x),[\/latex] we have<\/p>\n<div id=\"fs-id1170571168095\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\displaystyle\\int f(g(x)){g}^{\\prime }(x)dx=F(g(x))+C[\/latex]<\/div>\n<p id=\"fs-id1170573420715\">Then<\/p>\n<div id=\"fs-id1170573388911\" class=\"equation\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{a}^{b}f\\left[g(x)\\right]{g}^{\\prime }(x)dx\\hfill &amp; ={F(g(x))|}_{x=a}^{x=b}\\hfill \\\\ &amp; =F(g(b))-F(g(a))\\hfill \\\\ &amp; ={F(u)|}_{u=g(a)}^{u=g(b)}\\hfill \\\\ \\\\ \\\\ &amp; ={\\displaystyle\\int }_{g(a)}^{g(b)}f(u)du,\\hfill \\end{array}[\/latex]<\/div>\n<p id=\"fs-id1170571100165\">and we have the desired result.<\/p>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{1}{x}^{2}{(1+2{x}^{3})}^{5}dx.[\/latex]<\/p>\n<p>[reveal-answer q=\"fs-id1170572587723\"]Show Solution[\/reveal-answer]<br>\n[hidden-answer a=\"fs-id1170572587723\"]<\/p>\n<p id=\"fs-id1170573440252\">Let [latex]u=1+2{x}^{3},[\/latex] so [latex]du=6{x}^{2}dx.[\/latex]<\/p>\n<p>Since the original function includes one factor of [latex]x^2[\/latex]&nbsp;and [latex]du=6{x}^{2}dx,[\/latex] multiply both sides of the <em>du<\/em> equation by [latex]\\frac{1}{6}.[\/latex]<\/p>\n<p>Then,<\/p>\n<div id=\"fs-id1170573362498\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{ccc}du\\hfill &amp; =\\hfill &amp; 6{x}^{2}dx\\hfill \\\\ \\frac{1}{6}du\\hfill &amp; =\\hfill &amp; {x}^{2}dx.\\hfill \\end{array}[\/latex]<\/div>\n<p id=\"fs-id1170571157085\">To adjust the limits of integration, note that when [latex]x=0,u=1+2(0)=1,[\/latex] and when [latex]x=1,u=1+2(1)=3.[\/latex]<\/p>\n<p>Then,<\/p>\n<div id=\"fs-id1170571303367\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{0}^{1}{x}^{2}{(1+2{x}^{3})}^{5}dx=\\frac{1}{6}{\\displaystyle\\int }_{1}^{3}{u}^{5}du.[\/latex]<\/div>\n<p id=\"fs-id1170571285285\">Evaluating this expression, we get<\/p>\n<div id=\"fs-id1170571285289\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{}\\frac{1}{6}{\\displaystyle\\int }_{1}^{3}{u}^{5}du\\hfill &amp; =(\\frac{1}{6})(\\frac{{u}^{6}}{6}){|}_{1}^{3}\\hfill \\\\ &amp; =\\frac{1}{36}\\left[{(3)}^{6}-{(1)}^{6}\\right]\\hfill \\\\ &amp; =\\frac{182}{9}.\\hfill \\end{array}[\/latex]<\/div>\n<p>Watch the following video to see the worked solution to this example.<\/p>\n<center><iframe title=\"YouTube video player\" src=\"https:\/\/www.youtube.com\/embed\/Ak_y3lsBNfE?controls=0&amp;start=519&amp;end=664&amp;autoplay=0\" width=\"750\" height=\"450\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-mce-fragment=\"1\"><\/iframe><\/center>\n<p>For closed captioning, open the video on its original page by clicking the Youtube logo in the lower right-hand corner of the video display. In YouTube, the video will begin at the same starting point as this clip, but will continue playing until the very end.<\/p>\n<p>You can view the <a href=\"https:\/\/oerfiles.s3.us-west-2.amazonaws.com\/Calculus\/Calculus1+Videos\/5.5Substitution519to664_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of \"5.5 Substitution\" here (opens in new window)<\/a>.[\/hidden-answer]<\/p>\n<\/section>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{1}x{e}^{4{x}^{2}+3}dx.[\/latex]<\/p>\n<p>[reveal-answer q=\"fs-id1170572587724\"]Show Solution[\/reveal-answer]<br>\n[hidden-answer a=\"fs-id1170572587724\"]<\/p>\n<p id=\"fs-id1170571347206\">Let [latex]u=4{x}^{3}+3.[\/latex] Then, [latex]du=8xdx.[\/latex]<\/p>\n<p>To adjust the limits of integration, we note that when [latex]x=0,u=3,[\/latex] and when [latex]x=1,u=7.[\/latex]<\/p>\n<p>So our substitution gives,<\/p>\n<div id=\"fs-id1170571052992\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{0}^{1}x{e}^{4{x}^{2}+3}dx\\hfill &amp; =\\frac{1}{8}{\\displaystyle\\int }_{3}^{7}{e}^{u}du\\hfill \\\\ \\\\ &amp; =\\frac{1}{8}{e}^{u}{|}_{3}^{7}\\hfill \\\\ &amp; =\\frac{{e}^{7}-{e}^{3}}{8}\\hfill \\\\ &amp; \\approx 134.568.\\hfill \\end{array}[\/latex][\/hidden-answer]<\/div>\n<\/section>\n<p id=\"fs-id1170571289709\">Substitution may be only one of the techniques needed to evaluate a definite integral. All of the properties and rules of integration apply independently, and trigonometric functions may need to be rewritten using a trigonometric identity before we can apply substitution. Also, we have the option of replacing the original expression for [latex]u[\/latex] after we find the antiderivative, which means that we do not have to change the limits of integration. These two approaches are shown in the following examples.<\/p>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}{ \\cos }^{2}\\theta d\\theta .[\/latex]<\/p>\n<p>[reveal-answer q=\"fs-id1170572587725\"]Show Solution[\/reveal-answer]<br>\n[hidden-answer a=\"fs-id1170572587725\"]<\/p>\n<p id=\"fs-id1170571030577\">Let us first use a trigonometric identity to rewrite the integral. The trig identity [latex]{ \\cos }^{2}\\theta =\\frac{1+ \\cos 2\\theta }{2}[\/latex] allows us to rewrite the integral as<\/p>\n<div id=\"fs-id1170571131164\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}{ \\cos }^{2}\\theta d\\theta ={\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\frac{1+ \\cos 2\\theta }{2}d\\theta .[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1170573351678\">Then,<\/p>\n<div id=\"fs-id1170573581363\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\left(\\frac{1+ \\cos 2\\theta }{2}\\right)d\\theta \\hfill &amp; ={\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\left(\\frac{1}{2}+\\frac{1}{2} \\cos 2\\theta \\right)d\\theta \\hfill \\\\ \\\\ \\\\ &amp; =\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta + \\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2} \\cos 2\\theta d\\theta .\\hfill \\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1170571374921\">We can evaluate the first integral as it is, but we need to make a substitution to evaluate the second integral. Let [latex]u=2\\theta .[\/latex] Then, [latex]du=2d\\theta ,[\/latex] or [latex]\\frac{1}{2}du=d\\theta .[\/latex] Also, when [latex]\\theta =0,u=0,[\/latex] and when [latex]\\theta =\\pi \\text{\/}2,u=\\pi .[\/latex] Expressing the second integral in terms of [latex]u[\/latex], we have<\/p>\n<div id=\"fs-id1170571244772\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{}\\\\ \\\\ \\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta +\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2} \\cos 2\\theta d\\theta \\hfill &amp; =\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta +\\frac{1}{2}(\\frac{1}{2}){\\displaystyle\\int }_{0}^{\\pi } \\cos udu\\hfill \\\\ &amp; =\\frac{\\theta }{2}{|}_{\\theta =0}^{\\theta =\\pi \\text{\/}2}+\\frac{1}{4} \\sin u{|}_{u=0}^{u=\\theta }\\hfill \\\\ &amp; =(\\frac{\\pi }{4}-0)+(0-0)=\\frac{\\pi }{4}.\\hfill \\end{array}[\/latex]<\/div>\n<p>Watch the following video to see the worked solution to this example.<\/p>\n<center><iframe title=\"YouTube video player\" src=\"https:\/\/www.youtube.com\/embed\/Ak_y3lsBNfE?controls=0&amp;start=774&amp;end=978&amp;autoplay=0\" width=\"750\" height=\"450\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-mce-fragment=\"1\"><\/iframe><\/center>\n<p>For closed captioning, open the video on its original page by clicking the Youtube logo in the lower right-hand corner of the video display. In YouTube, the video will begin at the same starting point as this clip, but will continue playing until the very end.<\/p>\n<p>You can view the <a href=\"https:\/\/oerfiles.s3.us-west-2.amazonaws.com\/Calculus\/Calculus1+Videos\/5.5Substitution774to978_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of \"5.5 Substitution\" here (opens in new window)<\/a>.[\/hidden-answer]<\/p>\n<\/section>\n<section class=\"textbox tryIt\">\n<p>[ohm_question hide_question_numbers=1]211747[\/ohm_question]<\/p>\n<\/section>\n","rendered":"<h2>Substitution for Definite Integrals<\/h2>\n<p id=\"fs-id1170573387843\">Substitution can be used with definite integrals, too. However, using substitution to evaluate a definite integral requires a change to the limits of integration. If we change variables in the integrand, the limits of integration change as well.<\/p>\n<section class=\"textbox keyTakeaway\">\n<div>\n<h3>substitution with definite integrals<\/h3>\n<p id=\"fs-id1170570999523\">Let [latex]u=g(x)[\/latex] and let [latex]{g}^{\\text{\u2032}}[\/latex] be continuous over an interval [latex]\\left[a,b\\right],[\/latex] and let [latex]f[\/latex] be continuous over the range of [latex]u=g(x).[\/latex] Then,<\/p>\n<div id=\"fs-id1170571189407\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{a}^{b}f(g(x)){g}^{\\prime }(x)dx={\\displaystyle\\int }_{g(a)}^{g(b)}f(u)du[\/latex]<\/div>\n<\/div>\n<\/section>\n<p id=\"fs-id1170573502228\">Although we will not formally prove this theorem, we justify it with some calculations here. From the substitution rule for indefinite integrals, if [latex]F(x)[\/latex] is an antiderivative of [latex]f(x),[\/latex] we have<\/p>\n<div id=\"fs-id1170571168095\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\displaystyle\\int f(g(x)){g}^{\\prime }(x)dx=F(g(x))+C[\/latex]<\/div>\n<p id=\"fs-id1170573420715\">Then<\/p>\n<div id=\"fs-id1170573388911\" class=\"equation\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{a}^{b}f\\left[g(x)\\right]{g}^{\\prime }(x)dx\\hfill & ={F(g(x))|}_{x=a}^{x=b}\\hfill \\\\ & =F(g(b))-F(g(a))\\hfill \\\\ & ={F(u)|}_{u=g(a)}^{u=g(b)}\\hfill \\\\ \\\\ \\\\ & ={\\displaystyle\\int }_{g(a)}^{g(b)}f(u)du,\\hfill \\end{array}[\/latex]<\/div>\n<p id=\"fs-id1170571100165\">and we have the desired result.<\/p>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{1}{x}^{2}{(1+2{x}^{3})}^{5}dx.[\/latex]<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1170572587723\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1170572587723\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1170573440252\">Let [latex]u=1+2{x}^{3},[\/latex] so [latex]du=6{x}^{2}dx.[\/latex]<\/p>\n<p>Since the original function includes one factor of [latex]x^2[\/latex]&nbsp;and [latex]du=6{x}^{2}dx,[\/latex] multiply both sides of the <em>du<\/em> equation by [latex]\\frac{1}{6}.[\/latex]<\/p>\n<p>Then,<\/p>\n<div id=\"fs-id1170573362498\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{ccc}du\\hfill & =\\hfill & 6{x}^{2}dx\\hfill \\\\ \\frac{1}{6}du\\hfill & =\\hfill & {x}^{2}dx.\\hfill \\end{array}[\/latex]<\/div>\n<p id=\"fs-id1170571157085\">To adjust the limits of integration, note that when [latex]x=0,u=1+2(0)=1,[\/latex] and when [latex]x=1,u=1+2(1)=3.[\/latex]<\/p>\n<p>Then,<\/p>\n<div id=\"fs-id1170571303367\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{0}^{1}{x}^{2}{(1+2{x}^{3})}^{5}dx=\\frac{1}{6}{\\displaystyle\\int }_{1}^{3}{u}^{5}du.[\/latex]<\/div>\n<p id=\"fs-id1170571285285\">Evaluating this expression, we get<\/p>\n<div id=\"fs-id1170571285289\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{}\\frac{1}{6}{\\displaystyle\\int }_{1}^{3}{u}^{5}du\\hfill & =(\\frac{1}{6})(\\frac{{u}^{6}}{6}){|}_{1}^{3}\\hfill \\\\ & =\\frac{1}{36}\\left[{(3)}^{6}-{(1)}^{6}\\right]\\hfill \\\\ & =\\frac{182}{9}.\\hfill \\end{array}[\/latex]<\/div>\n<p>Watch the following video to see the worked solution to this example.<\/p>\n<div style=\"text-align: center;\"><iframe loading=\"lazy\" title=\"YouTube video player\" src=\"https:\/\/www.youtube.com\/embed\/Ak_y3lsBNfE?controls=0&amp;start=519&amp;end=664&amp;autoplay=0\" width=\"750\" height=\"450\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-mce-fragment=\"1\"><\/iframe><\/div>\n<p>For closed captioning, open the video on its original page by clicking the Youtube logo in the lower right-hand corner of the video display. In YouTube, the video will begin at the same starting point as this clip, but will continue playing until the very end.<\/p>\n<p>You can view the <a href=\"https:\/\/oerfiles.s3.us-west-2.amazonaws.com\/Calculus\/Calculus1+Videos\/5.5Substitution519to664_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of &#8220;5.5 Substitution&#8221; here (opens in new window)<\/a>.<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{1}x{e}^{4{x}^{2}+3}dx.[\/latex]<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1170572587724\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1170572587724\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1170571347206\">Let [latex]u=4{x}^{3}+3.[\/latex] Then, [latex]du=8xdx.[\/latex]<\/p>\n<p>To adjust the limits of integration, we note that when [latex]x=0,u=3,[\/latex] and when [latex]x=1,u=7.[\/latex]<\/p>\n<p>So our substitution gives,<\/p>\n<div id=\"fs-id1170571052992\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{0}^{1}x{e}^{4{x}^{2}+3}dx\\hfill & =\\frac{1}{8}{\\displaystyle\\int }_{3}^{7}{e}^{u}du\\hfill \\\\ \\\\ & =\\frac{1}{8}{e}^{u}{|}_{3}^{7}\\hfill \\\\ & =\\frac{{e}^{7}-{e}^{3}}{8}\\hfill \\\\ & \\approx 134.568.\\hfill \\end{array}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/section>\n<p id=\"fs-id1170571289709\">Substitution may be only one of the techniques needed to evaluate a definite integral. All of the properties and rules of integration apply independently, and trigonometric functions may need to be rewritten using a trigonometric identity before we can apply substitution. Also, we have the option of replacing the original expression for [latex]u[\/latex] after we find the antiderivative, which means that we do not have to change the limits of integration. These two approaches are shown in the following examples.<\/p>\n<section class=\"textbox example\">\n<p>Use substitution to evaluate [latex]{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}{ \\cos }^{2}\\theta d\\theta .[\/latex]<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1170572587725\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1170572587725\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1170571030577\">Let us first use a trigonometric identity to rewrite the integral. The trig identity [latex]{ \\cos }^{2}\\theta =\\frac{1+ \\cos 2\\theta }{2}[\/latex] allows us to rewrite the integral as<\/p>\n<div id=\"fs-id1170571131164\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}{ \\cos }^{2}\\theta d\\theta ={\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\frac{1+ \\cos 2\\theta }{2}d\\theta .[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1170573351678\">Then,<\/p>\n<div id=\"fs-id1170573581363\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{cc}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\left(\\frac{1+ \\cos 2\\theta }{2}\\right)d\\theta \\hfill & ={\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}\\left(\\frac{1}{2}+\\frac{1}{2} \\cos 2\\theta \\right)d\\theta \\hfill \\\\ \\\\ \\\\ & =\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta + \\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2} \\cos 2\\theta d\\theta .\\hfill \\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1170571374921\">We can evaluate the first integral as it is, but we need to make a substitution to evaluate the second integral. Let [latex]u=2\\theta .[\/latex] Then, [latex]du=2d\\theta ,[\/latex] or [latex]\\frac{1}{2}du=d\\theta .[\/latex] Also, when [latex]\\theta =0,u=0,[\/latex] and when [latex]\\theta =\\pi \\text{\/}2,u=\\pi .[\/latex] Expressing the second integral in terms of [latex]u[\/latex], we have<\/p>\n<div id=\"fs-id1170571244772\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{}\\\\ \\\\ \\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta +\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2} \\cos 2\\theta d\\theta \\hfill & =\\frac{1}{2}{\\displaystyle\\int }_{0}^{\\pi \\text{\/}2}d\\theta +\\frac{1}{2}(\\frac{1}{2}){\\displaystyle\\int }_{0}^{\\pi } \\cos udu\\hfill \\\\ & =\\frac{\\theta }{2}{|}_{\\theta =0}^{\\theta =\\pi \\text{\/}2}+\\frac{1}{4} \\sin u{|}_{u=0}^{u=\\theta }\\hfill \\\\ & =(\\frac{\\pi }{4}-0)+(0-0)=\\frac{\\pi }{4}.\\hfill \\end{array}[\/latex]<\/div>\n<p>Watch the following video to see the worked solution to this example.<\/p>\n<div style=\"text-align: center;\"><iframe loading=\"lazy\" title=\"YouTube video player\" src=\"https:\/\/www.youtube.com\/embed\/Ak_y3lsBNfE?controls=0&amp;start=774&amp;end=978&amp;autoplay=0\" width=\"750\" height=\"450\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-mce-fragment=\"1\"><\/iframe><\/div>\n<p>For closed captioning, open the video on its original page by clicking the Youtube logo in the lower right-hand corner of the video display. In YouTube, the video will begin at the same starting point as this clip, but will continue playing until the very end.<\/p>\n<p>You can view the <a href=\"https:\/\/oerfiles.s3.us-west-2.amazonaws.com\/Calculus\/Calculus1+Videos\/5.5Substitution774to978_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of &#8220;5.5 Substitution&#8221; here (opens in new window)<\/a>.<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox tryIt\">\n<iframe loading=\"lazy\" id=\"ohm211747\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=211747&theme=lumen&iframe_resize_id=ohm211747&source=tnh\" width=\"100%\" height=\"150\"><\/iframe><br \/>\n<\/section>\n","protected":false},"author":6,"menu_order":6,"template":"","meta":{"_candela_citation":"[{\"type\":\"cc\",\"description\":\"Calculus Volume 1\",\"author\":\"Gilbert Strang, Edwin (Jed) Herman\",\"organization\":\"OpenStax\",\"url\":\"https:\/\/openstax.org\/details\/books\/calculus-volume-1\",\"project\":\"\",\"license\":\"cc-by-nc-sa\",\"license_terms\":\"Access for free at https:\/\/openstax.org\/books\/calculus-volume-1\/pages\/1-introduction\"},{\"type\":\"original\",\"description\":\"5.5 Substitution\",\"author\":\"Ryan Melton\",\"organization\":\"\",\"url\":\"\",\"project\":\"\",\"license\":\"cc-by\",\"license_terms\":\"\"}]","pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"part":399,"module-header":"","content_attributions":[{"type":"cc","description":"Calculus Volume 1","author":"Gilbert Strang, Edwin (Jed) Herman","organization":"OpenStax","url":"https:\/\/openstax.org\/details\/books\/calculus-volume-1","project":"","license":"cc-by-nc-sa","license_terms":"Access for free at https:\/\/openstax.org\/books\/calculus-volume-1\/pages\/1-introduction"},{"type":"original","description":"5.5 Substitution","author":"Ryan Melton","organization":"","url":"","project":"","license":"cc-by","license_terms":""}],"internal_book_links":[],"video_content":null,"cc_video_embed_content":{"cc_scripts":"","media_targets":[]},"try_it_collection":null,"_links":{"self":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/405"}],"collection":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/users\/6"}],"version-history":[{"count":0,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/405\/revisions"}],"part":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/parts\/399"}],"metadata":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/405\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/media?parent=405"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapter-type?post=405"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/contributor?post=405"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/license?post=405"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}