{"id":691,"date":"2025-06-20T17:03:58","date_gmt":"2025-06-20T17:03:58","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus2\/?post_type=chapter&#038;p=691"},"modified":"2025-09-10T14:03:30","modified_gmt":"2025-09-10T14:03:30","slug":"integration-by-parts-learn-it-3","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus2\/chapter\/integration-by-parts-learn-it-3\/","title":{"raw":"Integration by Parts: Learn It 3","rendered":"Integration by Parts: Learn It 3"},"content":{"raw":"<h2 data-type=\"title\">Integration by Parts for Definite Integrals<\/h2>\r\nNow that we have used integration by parts successfully to evaluate <span class=\"no-emphasis\" data-type=\"term\">indefinite integrals<\/span>, we turn our attention to definite integrals. The integration technique is really the same, only we add a step to evaluate the integral at the upper and lower limits of integration.\r\n\r\n<section class=\"textbox keyTakeaway\" aria-label=\"Key Takeaway\">\r\n<div>\r\n<h3>integration by parts for definite integrals<\/h3>\r\n<p id=\"fs-id1165042231049\">Let [latex]u=f\\left(x\\right)[\/latex] and [latex]v=g\\left(x\\right)[\/latex] be functions with continuous derivatives on [latex]\\left[a,b\\right][\/latex]. Then<\/p>\r\n\r\n<center>[latex]{\\displaystyle\\int }_{a}^{b}udv={uv|}_{a}^{b}-{\\displaystyle\\int }_{a}^{b}vdu[\/latex].<\/center><\/div>\r\n<\/section><section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042058875\" data-type=\"problem\">\u00a0Find the area of the region bounded above by the graph of [latex]y={\\tan}^{-1}x[\/latex] and below by the [latex]x[\/latex] -axis over the interval [latex]\\left[0,1\\right][\/latex].<\/div>\r\n<div id=\"fs-id1165042071427\" data-type=\"commentary\">\r\n\r\n[reveal-answer q=\"44558879\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558879\"]\r\n<div id=\"fs-id1165042237897\" data-type=\"solution\">\r\n<p id=\"fs-id1165042237899\">This region is shown in Figure 1. To find the area, we must evaluate [latex]\\underset{0}{\\overset{1}{\\displaystyle\\int }}{\\tan}^{-1}xdx[\/latex].<\/p>\r\n\r\n<figure id=\"CNX_Calc_Figure_07_01_001\"><figcaption><\/figcaption>\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"562\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/4175\/2019\/04\/11233750\/CNX_Calc_Figure_07_01_001.jpg\" alt=\"This figure is the graph of the inverse tangent function. It is an increasing function that passes through the origin. In the first quadrant there is a shaded region under the graph, above the x-axis. The shaded area is bounded to the right at x = 1.\" width=\"562\" height=\"570\" data-media-type=\"image\/jpeg\" \/> Figure 1. To find the area of the shaded region, we have to use integration by parts.[\/caption]<\/figure>\r\n<p id=\"fs-id1165042237957\">For this integral, let\u2019s choose [latex]u={\\tan}^{-1}x[\/latex] and [latex]dv=dx[\/latex], thereby making [latex]du=\\frac{1}{{x}^{2}+1}dx[\/latex] and [latex]v=x[\/latex]. After applying the integration-by-parts formula we obtain<\/p>\r\n\r\n<div id=\"fs-id1165042238034\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\text{Area}=x{\\tan}^{-1}{x|}_{0}^{1}-\\underset{0}{\\overset{1}{\\displaystyle\\int }}\\frac{x}{{x}^{2}+1}dx[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042304278\">Use <em data-effect=\"italics\">u<\/em>-substitution to obtain<\/p>\r\n\r\n<div id=\"fs-id1165042304286\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\underset{0}{\\overset{1}{\\displaystyle\\int }}\\frac{x}{{x}^{2}+1}dx=\\frac{1}{2}\\text{ln}|{x}^{2}+1{|}_{0}^{1}[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042304368\">Thus,<\/p>\r\n\r\n<div id=\"fs-id1165042304371\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\text{Area}=x{\\tan }^{-1}x{|}_{0}^{1}-\\frac{1}{2}\\mathrm{ln}|{x}^{2}+1|{|}_{0}^{1}=\\frac{\\pi }{4}-\\frac{1}{2}\\mathrm{ln}2[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042304463\">At this point it might not be a bad idea to do a \"reality check\" on the reasonableness of our solution. Since [latex]\\frac{\\pi }{4}-\\frac{1}{2}\\text{ln}2\\approx 0.4388[\/latex], and from Figure 1 we expect our area to be slightly less than 0.5, this solution appears to be reasonable.<\/p>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/div>\r\n<\/section><section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042058875\" data-type=\"problem\">\r\n<p id=\"fs-id1165042058881\">Find the volume of the solid obtained by revolving the region bounded by the graph of [latex]f\\left(x\\right)={e}^{\\text{-}x}[\/latex], the <em data-effect=\"italics\">x<\/em>-axis, the <em data-effect=\"italics\">y<\/em>-axis, and the line [latex]x=1[\/latex] about the <em data-effect=\"italics\">y<\/em>-axis.<\/p>\r\n\r\n<\/div>\r\n[reveal-answer q=\"44558869\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558869\"]\r\n<div id=\"fs-id1165042058936\" data-type=\"solution\">\r\n<p id=\"fs-id1165042058938\">The best option to solving this problem is to use the shell method. Begin by sketching the region to be revolved, along with a typical rectangle (see the following graph).<\/p>\r\n\r\n<figure id=\"CNX_Calc_Figure_07_01_002\"><figcaption><\/figcaption>\r\n\r\n[caption id=\"\" align=\"alignnone\" width=\"731\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/4175\/2019\/04\/11233752\/CNX_Calc_Figure_07_01_002.jpg\" alt=\"This figure is the graph of the function e^-x. It is an increasing function on the left side of the y-axis and decreasing on the right side of the y-axis. The curve also comes to a point on the y-axis at y=1. Under the curve there is a shaded rectangle in the first quadrant. There is also a cylinder under the graph, formed by revolving the rectangle around the y-axis.\" width=\"731\" height=\"272\" data-media-type=\"image\/jpeg\" \/> Figure 2. We can use the shell method to find a volume of revolution.[\/caption]<\/figure>\r\n<p id=\"fs-id1165042058966\">To find the volume using shells, we must evaluate [latex]2\\pi {\\displaystyle\\int }_{0}^{1}x{e}^{\\text{-}x}dx[\/latex]. To do this, let [latex]u=x[\/latex] and [latex]dv={e}^{\\text{-}x}[\/latex]. These choices lead to [latex]du=dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}{e}^{\\text{-}x}=\\text{-}{e}^{\\text{-}x}[\/latex]. Substituting into the integration-by-parts for definite integrals formula, we obtain<\/p>\r\n\r\n<div id=\"fs-id1165042281368\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{cccc}\\hfill \\text{Volume}&amp; =2\\pi \\underset{0}{\\overset{1}{\\displaystyle\\int }}x{e}^{\\text{-}x}dx=2\\pi \\left(\\text{-}x{e}^{\\text{-}x}{|}_{0}^{1}+\\underset{0}{\\overset{1}{\\displaystyle\\int }}{e}^{\\text{-}x}dx\\right)\\hfill &amp; &amp; \\text{Use integration by parts}.\\hfill \\\\ &amp; =-2\\pi x{e}^{\\text{-}x}{|}_{0}^{1}-2\\pi {e}^{\\text{-}x}{|}_{0}^{1}\\hfill &amp; &amp; \\text{Evaluate}\\underset{0}{\\overset{1}{\\displaystyle\\int }}{e}^{\\text{-}x}dx=\\text{-}{e}^{\\text{-}x}{|}_{0}^{1}.\\hfill \\\\ &amp; =2\\pi -\\frac{4\\pi }{e}.\\hfill &amp; &amp; \\text{Evaluate and simplify}.\\hfill \\end{array}[\/latex]<\/div>\r\n&nbsp;\r\n\r\n<\/div>\r\n<div id=\"fs-id1165042071427\" data-type=\"commentary\">\r\n<div data-type=\"title\"><strong>Analysis<\/strong><\/div>\r\n<p id=\"fs-id1165042071432\">Again, it is a good idea to check the reasonableness of our solution. We observe that the solid has a volume slightly less than that of a cylinder of radius [latex]1[\/latex] and height of [latex]\\frac{1}{e}[\/latex] added to the volume of a cone of base radius [latex]1[\/latex] and height of [latex]1-\\frac{1}{3}[\/latex]. Consequently, the solid should have a volume a bit less than<\/p>\r\n\r\n<div id=\"fs-id1165042071470\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\pi {\\left(1\\right)}^{2}\\frac{1}{e}+\\left(\\frac{\\pi }{3}\\right){\\left(1\\right)}^{2}\\left(1-\\frac{1}{e}\\right)=\\frac{2\\pi }{3e}-\\frac{\\pi }{3}\\approx 1.8177[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042071569\">Since [latex]2\\pi -\\frac{4\\pi }{e}\\approx 1.6603[\/latex], we see that our calculated volume is reasonable.<\/p>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/section><section class=\"textbox tryIt\" aria-label=\"Try It\">[ohm_question hide_question_numbers=1]311292[\/ohm_question]<\/section>","rendered":"<h2 data-type=\"title\">Integration by Parts for Definite Integrals<\/h2>\n<p>Now that we have used integration by parts successfully to evaluate <span class=\"no-emphasis\" data-type=\"term\">indefinite integrals<\/span>, we turn our attention to definite integrals. The integration technique is really the same, only we add a step to evaluate the integral at the upper and lower limits of integration.<\/p>\n<section class=\"textbox keyTakeaway\" aria-label=\"Key Takeaway\">\n<div>\n<h3>integration by parts for definite integrals<\/h3>\n<p id=\"fs-id1165042231049\">Let [latex]u=f\\left(x\\right)[\/latex] and [latex]v=g\\left(x\\right)[\/latex] be functions with continuous derivatives on [latex]\\left[a,b\\right][\/latex]. Then<\/p>\n<div style=\"text-align: center;\">[latex]{\\displaystyle\\int }_{a}^{b}udv={uv|}_{a}^{b}-{\\displaystyle\\int }_{a}^{b}vdu[\/latex].<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div id=\"fs-id1165042058875\" data-type=\"problem\">\u00a0Find the area of the region bounded above by the graph of [latex]y={\\tan}^{-1}x[\/latex] and below by the [latex]x[\/latex] -axis over the interval [latex]\\left[0,1\\right][\/latex].<\/div>\n<div id=\"fs-id1165042071427\" data-type=\"commentary\">\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558879\">Show Solution<\/button><\/p>\n<div id=\"q44558879\" class=\"hidden-answer\" style=\"display: none\">\n<div id=\"fs-id1165042237897\" data-type=\"solution\">\n<p id=\"fs-id1165042237899\">This region is shown in Figure 1. To find the area, we must evaluate [latex]\\underset{0}{\\overset{1}{\\displaystyle\\int }}{\\tan}^{-1}xdx[\/latex].<\/p>\n<figure id=\"CNX_Calc_Figure_07_01_001\"><figcaption><\/figcaption><figure style=\"width: 562px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/4175\/2019\/04\/11233750\/CNX_Calc_Figure_07_01_001.jpg\" alt=\"This figure is the graph of the inverse tangent function. It is an increasing function that passes through the origin. In the first quadrant there is a shaded region under the graph, above the x-axis. The shaded area is bounded to the right at x = 1.\" width=\"562\" height=\"570\" data-media-type=\"image\/jpeg\" \/><figcaption class=\"wp-caption-text\">Figure 1. To find the area of the shaded region, we have to use integration by parts.<\/figcaption><\/figure>\n<\/figure>\n<p id=\"fs-id1165042237957\">For this integral, let\u2019s choose [latex]u={\\tan}^{-1}x[\/latex] and [latex]dv=dx[\/latex], thereby making [latex]du=\\frac{1}{{x}^{2}+1}dx[\/latex] and [latex]v=x[\/latex]. After applying the integration-by-parts formula we obtain<\/p>\n<div id=\"fs-id1165042238034\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\text{Area}=x{\\tan}^{-1}{x|}_{0}^{1}-\\underset{0}{\\overset{1}{\\displaystyle\\int }}\\frac{x}{{x}^{2}+1}dx[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042304278\">Use <em data-effect=\"italics\">u<\/em>-substitution to obtain<\/p>\n<div id=\"fs-id1165042304286\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\underset{0}{\\overset{1}{\\displaystyle\\int }}\\frac{x}{{x}^{2}+1}dx=\\frac{1}{2}\\text{ln}|{x}^{2}+1{|}_{0}^{1}[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042304368\">Thus,<\/p>\n<div id=\"fs-id1165042304371\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\text{Area}=x{\\tan }^{-1}x{|}_{0}^{1}-\\frac{1}{2}\\mathrm{ln}|{x}^{2}+1|{|}_{0}^{1}=\\frac{\\pi }{4}-\\frac{1}{2}\\mathrm{ln}2[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042304463\">At this point it might not be a bad idea to do a &#8220;reality check&#8221; on the reasonableness of our solution. Since [latex]\\frac{\\pi }{4}-\\frac{1}{2}\\text{ln}2\\approx 0.4388[\/latex], and from Figure 1 we expect our area to be slightly less than 0.5, this solution appears to be reasonable.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div data-type=\"problem\">\n<p id=\"fs-id1165042058881\">Find the volume of the solid obtained by revolving the region bounded by the graph of [latex]f\\left(x\\right)={e}^{\\text{-}x}[\/latex], the <em data-effect=\"italics\">x<\/em>-axis, the <em data-effect=\"italics\">y<\/em>-axis, and the line [latex]x=1[\/latex] about the <em data-effect=\"italics\">y<\/em>-axis.<\/p>\n<\/div>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558869\">Show Solution<\/button><\/p>\n<div id=\"q44558869\" class=\"hidden-answer\" style=\"display: none\">\n<div id=\"fs-id1165042058936\" data-type=\"solution\">\n<p id=\"fs-id1165042058938\">The best option to solving this problem is to use the shell method. Begin by sketching the region to be revolved, along with a typical rectangle (see the following graph).<\/p>\n<figure id=\"CNX_Calc_Figure_07_01_002\"><figcaption><\/figcaption><figure style=\"width: 731px\" class=\"wp-caption alignnone\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/4175\/2019\/04\/11233752\/CNX_Calc_Figure_07_01_002.jpg\" alt=\"This figure is the graph of the function e^-x. It is an increasing function on the left side of the y-axis and decreasing on the right side of the y-axis. The curve also comes to a point on the y-axis at y=1. Under the curve there is a shaded rectangle in the first quadrant. There is also a cylinder under the graph, formed by revolving the rectangle around the y-axis.\" width=\"731\" height=\"272\" data-media-type=\"image\/jpeg\" \/><figcaption class=\"wp-caption-text\">Figure 2. We can use the shell method to find a volume of revolution.<\/figcaption><\/figure>\n<\/figure>\n<p id=\"fs-id1165042058966\">To find the volume using shells, we must evaluate [latex]2\\pi {\\displaystyle\\int }_{0}^{1}x{e}^{\\text{-}x}dx[\/latex]. To do this, let [latex]u=x[\/latex] and [latex]dv={e}^{\\text{-}x}[\/latex]. These choices lead to [latex]du=dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}{e}^{\\text{-}x}=\\text{-}{e}^{\\text{-}x}[\/latex]. Substituting into the integration-by-parts for definite integrals formula, we obtain<\/p>\n<div id=\"fs-id1165042281368\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{cccc}\\hfill \\text{Volume}& =2\\pi \\underset{0}{\\overset{1}{\\displaystyle\\int }}x{e}^{\\text{-}x}dx=2\\pi \\left(\\text{-}x{e}^{\\text{-}x}{|}_{0}^{1}+\\underset{0}{\\overset{1}{\\displaystyle\\int }}{e}^{\\text{-}x}dx\\right)\\hfill & & \\text{Use integration by parts}.\\hfill \\\\ & =-2\\pi x{e}^{\\text{-}x}{|}_{0}^{1}-2\\pi {e}^{\\text{-}x}{|}_{0}^{1}\\hfill & & \\text{Evaluate}\\underset{0}{\\overset{1}{\\displaystyle\\int }}{e}^{\\text{-}x}dx=\\text{-}{e}^{\\text{-}x}{|}_{0}^{1}.\\hfill \\\\ & =2\\pi -\\frac{4\\pi }{e}.\\hfill & & \\text{Evaluate and simplify}.\\hfill \\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<\/div>\n<div data-type=\"commentary\">\n<div data-type=\"title\"><strong>Analysis<\/strong><\/div>\n<p id=\"fs-id1165042071432\">Again, it is a good idea to check the reasonableness of our solution. We observe that the solid has a volume slightly less than that of a cylinder of radius [latex]1[\/latex] and height of [latex]\\frac{1}{e}[\/latex] added to the volume of a cone of base radius [latex]1[\/latex] and height of [latex]1-\\frac{1}{3}[\/latex]. Consequently, the solid should have a volume a bit less than<\/p>\n<div id=\"fs-id1165042071470\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\pi {\\left(1\\right)}^{2}\\frac{1}{e}+\\left(\\frac{\\pi }{3}\\right){\\left(1\\right)}^{2}\\left(1-\\frac{1}{e}\\right)=\\frac{2\\pi }{3e}-\\frac{\\pi }{3}\\approx 1.8177[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042071569\">Since [latex]2\\pi -\\frac{4\\pi }{e}\\approx 1.6603[\/latex], we see that our calculated volume is reasonable.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox tryIt\" aria-label=\"Try It\"><iframe loading=\"lazy\" id=\"ohm311292\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=311292&theme=lumen&iframe_resize_id=ohm311292&source=tnh\" width=\"100%\" height=\"150\"><\/iframe><\/section>\n","protected":false},"author":15,"menu_order":9,"template":"","meta":{"_candela_citation":"[]","pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"part":541,"module-header":"- Select Header -","content_attributions":[],"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\/691"}],"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\/15"}],"version-history":[{"count":5,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/691\/revisions"}],"predecessor-version":[{"id":2283,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/691\/revisions\/2283"}],"part":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/parts\/541"}],"metadata":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/691\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/media?parent=691"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapter-type?post=691"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/contributor?post=691"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/license?post=691"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}