{"id":689,"date":"2025-06-20T17:03:54","date_gmt":"2025-06-20T17:03:54","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus2\/?post_type=chapter&#038;p=689"},"modified":"2025-09-10T13:59:55","modified_gmt":"2025-09-10T13:59:55","slug":"integration-by-parts-learn-it-2","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus2\/chapter\/integration-by-parts-learn-it-2\/","title":{"raw":"Integration by Parts: Learn It 2","rendered":"Integration by Parts: Learn It 2"},"content":{"raw":"<h2>How to Choose [latex]u[\/latex] and[latex] dv[\/latex]<\/h2>\r\nThe natural question you're probably asking is: <em>How do I know which part should be [latex]u[\/latex] and which should be [latex]dv[\/latex]?<\/em> Sometimes it takes some trial and error, but there's a helpful strategy that can guide your choices.\r\n\r\n<section class=\"textbox proTip\" aria-label=\"Pro Tip\">\r\n<p class=\"whitespace-normal break-words\"><strong>The LIATE Method<\/strong><\/p>\r\n<p class=\"whitespace-normal break-words\">The acronym <strong>LIATE<\/strong> can help take the guesswork out of choosing [latex]u[\/latex] and [latex]dv[\/latex]:<\/p>\r\n\r\n<ul class=\"[&amp;:not(:last-child)_ul]:pb-1 [&amp;:not(:last-child)_ol]:pb-1 list-disc space-y-1.5 pl-7\">\r\n \t<li class=\"whitespace-normal break-words\"><strong>L<\/strong>ogarithmic Functions<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>I<\/strong>nverse Trigonometric Functions<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>A<\/strong>lgebraic Functions<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>T<\/strong>rigonometric Functions<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>E<\/strong>xponential Functions<\/li>\r\n<\/ul>\r\n<p class=\"whitespace-normal break-words\"><strong>Rule:<\/strong> Choose [latex]u[\/latex] to be the function type that appears <strong>first<\/strong> in this list.<\/p>\r\n\r\n<\/section>For example, if your integral contains both a logarithmic function and an algebraic function, choose [latex]u[\/latex] to be the logarithmic function since <strong>L<\/strong> comes before <strong>A<\/strong> in LIATE.\r\n<h3 class=\"text-xl font-bold text-text-100 mt-1 -mb-0.5\">Why Does LIATE Work?<\/h3>\r\n<p class=\"whitespace-normal break-words\">This mnemonic works because of integration practicality:<\/p>\r\n\r\n<ul class=\"[&amp;:not(:last-child)_ul]:pb-1 [&amp;:not(:last-child)_ol]:pb-1 list-disc space-y-1.5 pl-7\">\r\n \t<li class=\"whitespace-normal break-words\"><strong>Logarithmic and inverse trig functions<\/strong> are at the front because we don't have simple integration formulas for them\u2014so they make poor choices for [latex]dv[\/latex]<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>Exponential and trig functions<\/strong> are at the end because they're easy to integrate and make excellent choices for [latex]dv[\/latex]<\/li>\r\n \t<li class=\"whitespace-normal break-words\"><strong>Algebraic functions<\/strong> are in the middle because they're generally manageable both to integrate and differentiate<\/li>\r\n<\/ul>\r\n<section class=\"textbox recall\" aria-label=\"Recall\">To use the by-parts technique successfully, it is helpful to first review the derivative rules of several familiar transcendental functions.\r\n<ol id=\"fs-id1170572169684\" style=\"list-style-type: decimal;\">\r\n \t<li>[latex] \\frac{d}{dx} (\\sin x) = \\cos x [\/latex]<\/li>\r\n \t<li>[latex] \\frac{d}{dx} (\\cos x) = -\\sin x [\/latex]<\/li>\r\n \t<li>[latex] \\frac{d}{dx} (\\ln x) = \\frac{1}{x} [\/latex]<\/li>\r\n \t<li>[latex] \\frac{d}{dx} (\\arcsin x) = \\frac{1}{\\sqrt{1-x^2}} [\/latex]<\/li>\r\n \t<li>[latex] \\frac{d}{dx} (\\arctan x) = \\frac{1}{1+x^2} [\/latex]<\/li>\r\n<\/ol>\r\n<\/section>Now let's see how this method works in practice.\r\n\r\n<section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042231844\" data-type=\"problem\">\r\n<p id=\"fs-id1165042231849\">Evaluate [latex]\\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx[\/latex].<\/p>\r\n\r\n<\/div>\r\n[reveal-answer q=\"44558896\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558896\"]\r\n<div id=\"fs-id1165042042007\" data-type=\"solution\">\r\n<p id=\"fs-id1165042042010\">Begin by rewriting the integral:<\/p>\r\n\r\n<div id=\"fs-id1165042008468\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx={\\displaystyle\\int }^{\\text{ }}{x}^{-3}\\text{ln}xdx[\/latex].<\/div>\r\n<p id=\"fs-id1165042127807\">Since this integral contains the algebraic function [latex]{x}^{-3}[\/latex] and the logarithmic function [latex]\\text{ln}x[\/latex], choose [latex]u=\\text{ln}x[\/latex], since L comes before A in LIATE. After we have chosen [latex]u=\\text{ln}x[\/latex], we must choose [latex]dv={x}^{-3}dx[\/latex].<\/p>\r\n<p id=\"fs-id1165042127784\">Next, since [latex]u=\\text{ln}x[\/latex], we have [latex]du=\\frac{1}{x}dx[\/latex]. Also, [latex]v={\\displaystyle\\int }^{\\text{ }}{x}^{-3}dx=-\\frac{1}{2}{x}^{-2}[\/latex]. Summarizing,<\/p>\r\n\r\n<div id=\"fs-id1165042109999\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u&amp; =\\hfill &amp; \\text{ln}x\\hfill &amp; &amp; \\hfill dv&amp; =\\hfill &amp; {x}^{-3}dx\\hfill \\\\ \\hfill du&amp; =\\hfill &amp; \\frac{1}{x}dx\\hfill &amp; &amp; \\hfill v&amp; =\\hfill &amp; {\\displaystyle\\int }^{\\text{ }}{x}^{-3}dx=-\\frac{1}{2}{x}^{-2}.\\end{array}[\/latex]<\/div>\r\n<p id=\"fs-id1165042128802\">Substituting into the integration-by-parts formula gives<\/p>\r\n\r\n<div id=\"fs-id1165042128805\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccc}\\hfill \\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx&amp; ={\\displaystyle\\int }^{\\text{ }}{x}^{-3}\\text{ln}xdx=\\left(\\text{ln}x\\right)\\left(\\text{-}\\frac{1}{2}{x}^{-2}\\right)-{\\displaystyle\\int }^{\\text{ }}\\left(\\text{-}\\frac{1}{2}{x}^{-2}\\right)\\left(\\frac{1}{x}dx\\right)\\hfill &amp; &amp; &amp; \\\\ &amp; =-\\frac{1}{2}{x}^{-2}\\text{ln}x+{\\displaystyle\\int }^{\\text{ }}\\frac{1}{2}{x}^{-3}dx\\hfill &amp; &amp; &amp; \\text{Simplify}.\\hfill \\\\ &amp; =-\\frac{1}{2}{x}^{-2}\\text{ln}x-\\frac{1}{4}{x}^{-2}+C\\hfill &amp; &amp; &amp; \\text{Integrate}.\\hfill \\\\ &amp; =-\\frac{1}{2{x}^{2}}\\text{ln}x-\\frac{1}{4{x}^{2}}+C.\\hfill &amp; &amp; &amp; \\text{Rewrite with positive integers.}\\end{array}[\/latex]<\/div>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/section>In some cases it may be necessary to apply integration by parts more than once.\r\n\r\n<section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042015541\" data-type=\"problem\">\r\n<p id=\"fs-id1165042015546\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{x}^{2}{e}^{3x}dx[\/latex].<\/p>\r\n\r\n<\/div>\r\n[reveal-answer q=\"44558893\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558893\"]\r\n<div id=\"fs-id1165040637308\" data-type=\"solution\">\r\n<p id=\"fs-id1165040637310\">Using LIATE, choose [latex]u={x}^{2}[\/latex] and [latex]dv={e}^{3x}dx[\/latex]. Thus, [latex]du=2xdx[\/latex] and [latex]v=\\displaystyle\\int {e}^{3x}dx=\\left(\\frac{1}{3}\\right){e}^{3x}[\/latex]. Therefore,<\/p>\r\n\r\n<div id=\"fs-id1165040740033\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u&amp; =\\hfill &amp; {x}^{2}\\hfill &amp; &amp; \\hfill dv&amp; =\\hfill &amp; {e}^{3x}dx\\hfill \\\\ \\hfill du&amp; =\\hfill &amp; 2xdx\\hfill &amp; &amp; \\hfill v&amp; =\\hfill &amp; \\displaystyle\\int {e}^{3x}dx=\\frac{1}{3}{e}^{3x}.\\end{array}[\/latex]<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042240114\">Substituting into the integration-by-parts formula\u00a0produces<\/p>\r\n\r\n<div id=\"fs-id1165042240117\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int {x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\displaystyle\\int \\frac{2}{3}x{e}^{3x}dx[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165040756177\">We still cannot integrate [latex]\\displaystyle\\int \\frac{2}{3}x{e}^{3x}dx[\/latex] directly, but the integral now has a lower power on [latex]x[\/latex]. We can evaluate this new integral by using integration by parts again. To do this, choose [latex]u=x[\/latex] and [latex]dv=\\frac{2}{3}{e}^{3x}dx[\/latex]. Thus, [latex]du=dx[\/latex] and [latex]v=\\displaystyle\\int \\left(\\frac{2}{3}\\right){e}^{3x}dx=\\left(\\frac{2}{9}\\right){e}^{3x}[\/latex]. Now we have<\/p>\r\n\r\n<div id=\"fs-id1165042002748\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u&amp; =\\hfill &amp; x\\hfill &amp; &amp; \\hfill dv&amp; =\\hfill &amp; \\frac{2}{3}{e}^{3x}dx\\hfill \\\\ \\hfill du&amp; =\\hfill &amp; dx\\hfill &amp; &amp; \\hfill v&amp; =\\hfill &amp; \\displaystyle\\int \\frac{2}{3}{e}^{3x}dx=\\frac{2}{9}{e}^{3x}.\\end{array}[\/latex]<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165040757531\">Substituting back into the previous equation yields<\/p>\r\n\r\n<div id=\"fs-id1165040757534\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}{x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\left(\\frac{2}{9}x{e}^{3x}-{\\displaystyle\\int }^{\\text{ }}\\frac{2}{9}{e}^{3x}dx\\right)[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042110524\">After evaluating the last integral and simplifying, we obtain<\/p>\r\n\r\n<div id=\"fs-id1165042110527\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int {x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\frac{2}{9}x{e}^{3x}+\\frac{2}{27}{e}^{3x}+C[\/latex].<\/div>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/section><section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042035450\" data-type=\"problem\">\r\n<p id=\"fs-id1165042035456\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex].<\/p>\r\n\r\n<\/div>\r\n[reveal-answer q=\"44558891\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558891\"]\r\n\r\nThis integral appears to have only one function\u2014namely, [latex]\\sin\\left(\\text{ln}x\\right)[\/latex] \u2014however, we can always use the constant function 1 as the other function. In this example, let\u2019s choose [latex]u=\\sin\\left(\\text{ln}x\\right)[\/latex] and [latex]dv=1dx[\/latex]. (The decision to use [latex]u=\\sin\\left(\\text{ln}x\\right)[\/latex] is easy. We can\u2019t choose [latex]dv=\\sin\\left(\\text{ln}x\\right)dx[\/latex] because if we could integrate it, we wouldn\u2019t be using integration by parts in the first place!) Consequently, [latex]du=\\frac{1}{x}\\cos\\left(\\text{ln}x\\right)dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}1dx=x[\/latex]. After applying integration by parts to the integral and simplifying, we have\r\n<div id=\"fs-id1165042035489\" data-type=\"solution\">\r\n<div id=\"fs-id1165042257200\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}\\cos\\left(\\text{ln}x\\right)dx[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042110018\">Unfortunately, this process leaves us with a new integral that is very similar to the original. However, let\u2019s see what happens when we apply integration by parts again. This time let\u2019s choose [latex]u=\\cos\\left(\\text{ln}x\\right)[\/latex] and [latex]dv=1dx[\/latex], making [latex]du=\\text{-}\\frac{1}{x}\\sin\\left(\\text{ln}x\\right)dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}1dx=x[\/latex]. Substituting, we have<\/p>\r\n\r\n<div id=\"fs-id1165042110131\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-\\left(x\\cos\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}-\\sin\\left(\\text{ln}x\\right)dx\\right)[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165040741882\">After simplifying, we obtain<\/p>\r\n\r\n<div id=\"fs-id1165040741886\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165040741980\">The last integral is now the same as the original. It may seem that we have simply gone in a circle, but now we can actually evaluate the integral. To see how to do this more clearly, substitute [latex]I={\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex]. Thus, the equation becomes<\/p>\r\n\r\n<div id=\"fs-id1165040742019\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]I=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)-I[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165040742068\">First, add [latex]I[\/latex] to both sides of the equation to obtain<\/p>\r\n\r\n<div id=\"fs-id1165040742075\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]2I=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042266548\">Next, divide by 2:<\/p>\r\n\r\n<div id=\"fs-id1165042266551\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]I=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042266606\">Substituting [latex]I={\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex] again, we have<\/p>\r\n\r\n<div id=\"fs-id1165042266641\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042266721\">From this we see that [latex]\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex] is an antiderivative of [latex]\\sin\\left(\\text{ln}x\\right)dx[\/latex]. For the most general antiderivative, add [latex]+C\\text{:}[\/latex]<\/p>\r\n\r\n<div id=\"fs-id1165042001966\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)+C[\/latex].<\/div>\r\n&nbsp;\r\n\r\n<\/div>\r\n<div id=\"fs-id1165042002057\" data-type=\"commentary\">\r\n<div data-type=\"title\"><strong>Analysis<\/strong><\/div>\r\n<p id=\"fs-id1165042002062\">If this method feels a little strange at first, we can check the answer by differentiation:<\/p>\r\n\r\n<div id=\"fs-id1165042002066\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{c}\\frac{d}{dx}\\left(\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)\\right)\\hfill \\\\ \\\\ =\\frac{1}{2}\\left(\\sin\\left(\\text{ln}x\\right)\\right)+\\cos\\left(\\text{ln}x\\right)\\cdot \\frac{1}{x}\\cdot \\frac{1}{2}x-\\left(\\frac{1}{2}\\cos\\left(\\text{ln}x\\right)-\\sin\\left(\\text{ln}x\\right)\\cdot \\frac{1}{x}\\cdot \\frac{1}{2}x\\right)\\hfill \\\\ =\\sin\\left(\\text{ln}x\\right).\\hfill \\end{array}[\/latex]<\/div>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/section><section class=\"textbox proTip\" aria-label=\"Pro Tip\"><img class=\"wp-image-2132 alignleft\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images-archive-read-only\/wp-content\/uploads\/sites\/1468\/2016\/03\/22011815\/traffic-sign-160659-300x265.png\" alt=\"Caution\" width=\"62\" height=\"55\" \/>Caution! LIATE is a guide, not a rigid rule. If your first choice leads to an integral you can't evaluate, try a different approach.<\/section><section class=\"textbox example\" aria-label=\"Example\">\r\n<div id=\"fs-id1165042132631\" data-type=\"problem\">\r\n<p id=\"fs-id1165042132636\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{t}^{3}{e}^{{t}^{2}}dt[\/latex].<\/p>\r\n\r\n<\/div>\r\n[reveal-answer q=\"44558892\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"44558892\"]\r\n<div id=\"fs-id1165042132671\" data-type=\"solution\">\r\n<p id=\"fs-id1165042132674\">If we use a strict interpretation of the mnemonic LIATE to make our choice of [latex]u[\/latex], we end up with [latex]u={t}^{3}[\/latex] and [latex]dv={e}^{{t}^{2}}dt[\/latex]. Unfortunately, this choice won\u2019t work because we are unable to evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{e}^{{t}^{2}}dt[\/latex]. However, since we can evaluate [latex]{\\displaystyle\\int }^{\\text{ }}t{e}^{{t}^{2}}dx[\/latex], we can try choosing [latex]u={t}^{2}[\/latex] and [latex]dv=t{e}^{{t}^{2}}dt[\/latex]. With these choices we have<\/p>\r\n\r\n<div id=\"fs-id1165040715819\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u&amp; =\\hfill &amp; {t}^{2}\\hfill &amp; &amp; \\hfill dv&amp; =\\hfill &amp; t{e}^{{t}^{2}}dt\\hfill \\\\ \\hfill du&amp; =\\hfill &amp; 2tdt\\hfill &amp; &amp; \\hfill v&amp; =\\hfill &amp; {\\displaystyle\\int }^{\\text{ }}t{e}^{{t}^{2}}dt=\\frac{1}{2}{e}^{{t}^{2}}.\\hfill \\end{array}[\/latex]<\/div>\r\n&nbsp;\r\n<p id=\"fs-id1165042013342\">Thus, we obtain<\/p>\r\n\r\n<div id=\"fs-id1165042013345\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{cc}{\\displaystyle\\int {t}^{3}{e}^{{t}^{2}}dt}\\hfill &amp; =\\frac{1}{2}{t}^{2}{e}^{{t}^{2}}-{\\displaystyle\\int \\frac{1}{2}{e}^{{t}^{2}}2tdt}\\hfill \\\\ \\hfill &amp; =\\frac{1}{2}{t}^{2}{e}^{{t}^{2}}-\\frac{1}{2}{e}^{{t}^{2}}+C.\\end{array}[\/latex]<\/div>\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]311291[\/ohm_question]<\/section>","rendered":"<h2>How to Choose [latex]u[\/latex] and[latex]dv[\/latex]<\/h2>\n<p>The natural question you&#8217;re probably asking is: <em>How do I know which part should be [latex]u[\/latex] and which should be [latex]dv[\/latex]?<\/em> Sometimes it takes some trial and error, but there&#8217;s a helpful strategy that can guide your choices.<\/p>\n<section class=\"textbox proTip\" aria-label=\"Pro Tip\">\n<p class=\"whitespace-normal break-words\"><strong>The LIATE Method<\/strong><\/p>\n<p class=\"whitespace-normal break-words\">The acronym <strong>LIATE<\/strong> can help take the guesswork out of choosing [latex]u[\/latex] and [latex]dv[\/latex]:<\/p>\n<ul class=\"[&amp;:not(:last-child)_ul]:pb-1 [&amp;:not(:last-child)_ol]:pb-1 list-disc space-y-1.5 pl-7\">\n<li class=\"whitespace-normal break-words\"><strong>L<\/strong>ogarithmic Functions<\/li>\n<li class=\"whitespace-normal break-words\"><strong>I<\/strong>nverse Trigonometric Functions<\/li>\n<li class=\"whitespace-normal break-words\"><strong>A<\/strong>lgebraic Functions<\/li>\n<li class=\"whitespace-normal break-words\"><strong>T<\/strong>rigonometric Functions<\/li>\n<li class=\"whitespace-normal break-words\"><strong>E<\/strong>xponential Functions<\/li>\n<\/ul>\n<p class=\"whitespace-normal break-words\"><strong>Rule:<\/strong> Choose [latex]u[\/latex] to be the function type that appears <strong>first<\/strong> in this list.<\/p>\n<\/section>\n<p>For example, if your integral contains both a logarithmic function and an algebraic function, choose [latex]u[\/latex] to be the logarithmic function since <strong>L<\/strong> comes before <strong>A<\/strong> in LIATE.<\/p>\n<h3 class=\"text-xl font-bold text-text-100 mt-1 -mb-0.5\">Why Does LIATE Work?<\/h3>\n<p class=\"whitespace-normal break-words\">This mnemonic works because of integration practicality:<\/p>\n<ul class=\"[&amp;:not(:last-child)_ul]:pb-1 [&amp;:not(:last-child)_ol]:pb-1 list-disc space-y-1.5 pl-7\">\n<li class=\"whitespace-normal break-words\"><strong>Logarithmic and inverse trig functions<\/strong> are at the front because we don&#8217;t have simple integration formulas for them\u2014so they make poor choices for [latex]dv[\/latex]<\/li>\n<li class=\"whitespace-normal break-words\"><strong>Exponential and trig functions<\/strong> are at the end because they&#8217;re easy to integrate and make excellent choices for [latex]dv[\/latex]<\/li>\n<li class=\"whitespace-normal break-words\"><strong>Algebraic functions<\/strong> are in the middle because they&#8217;re generally manageable both to integrate and differentiate<\/li>\n<\/ul>\n<section class=\"textbox recall\" aria-label=\"Recall\">To use the by-parts technique successfully, it is helpful to first review the derivative rules of several familiar transcendental functions.<\/p>\n<ol id=\"fs-id1170572169684\" style=\"list-style-type: decimal;\">\n<li>[latex]\\frac{d}{dx} (\\sin x) = \\cos x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx} (\\cos x) = -\\sin x[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx} (\\ln x) = \\frac{1}{x}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx} (\\arcsin x) = \\frac{1}{\\sqrt{1-x^2}}[\/latex]<\/li>\n<li>[latex]\\frac{d}{dx} (\\arctan x) = \\frac{1}{1+x^2}[\/latex]<\/li>\n<\/ol>\n<\/section>\n<p>Now let&#8217;s see how this method works in practice.<\/p>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div id=\"fs-id1165042231844\" data-type=\"problem\">\n<p id=\"fs-id1165042231849\">Evaluate [latex]\\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx[\/latex].<\/p>\n<\/div>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558896\">Show Solution<\/button><\/p>\n<div id=\"q44558896\" class=\"hidden-answer\" style=\"display: none\">\n<div id=\"fs-id1165042042007\" data-type=\"solution\">\n<p id=\"fs-id1165042042010\">Begin by rewriting the integral:<\/p>\n<div id=\"fs-id1165042008468\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx={\\displaystyle\\int }^{\\text{ }}{x}^{-3}\\text{ln}xdx[\/latex].<\/div>\n<p id=\"fs-id1165042127807\">Since this integral contains the algebraic function [latex]{x}^{-3}[\/latex] and the logarithmic function [latex]\\text{ln}x[\/latex], choose [latex]u=\\text{ln}x[\/latex], since L comes before A in LIATE. After we have chosen [latex]u=\\text{ln}x[\/latex], we must choose [latex]dv={x}^{-3}dx[\/latex].<\/p>\n<p id=\"fs-id1165042127784\">Next, since [latex]u=\\text{ln}x[\/latex], we have [latex]du=\\frac{1}{x}dx[\/latex]. Also, [latex]v={\\displaystyle\\int }^{\\text{ }}{x}^{-3}dx=-\\frac{1}{2}{x}^{-2}[\/latex]. Summarizing,<\/p>\n<div id=\"fs-id1165042109999\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u& =\\hfill & \\text{ln}x\\hfill & & \\hfill dv& =\\hfill & {x}^{-3}dx\\hfill \\\\ \\hfill du& =\\hfill & \\frac{1}{x}dx\\hfill & & \\hfill v& =\\hfill & {\\displaystyle\\int }^{\\text{ }}{x}^{-3}dx=-\\frac{1}{2}{x}^{-2}.\\end{array}[\/latex]<\/div>\n<p id=\"fs-id1165042128802\">Substituting into the integration-by-parts formula gives<\/p>\n<div id=\"fs-id1165042128805\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccc}\\hfill \\displaystyle\\int \\frac{\\text{ln}x}{{x}^{3}}dx& ={\\displaystyle\\int }^{\\text{ }}{x}^{-3}\\text{ln}xdx=\\left(\\text{ln}x\\right)\\left(\\text{-}\\frac{1}{2}{x}^{-2}\\right)-{\\displaystyle\\int }^{\\text{ }}\\left(\\text{-}\\frac{1}{2}{x}^{-2}\\right)\\left(\\frac{1}{x}dx\\right)\\hfill & & & \\\\ & =-\\frac{1}{2}{x}^{-2}\\text{ln}x+{\\displaystyle\\int }^{\\text{ }}\\frac{1}{2}{x}^{-3}dx\\hfill & & & \\text{Simplify}.\\hfill \\\\ & =-\\frac{1}{2}{x}^{-2}\\text{ln}x-\\frac{1}{4}{x}^{-2}+C\\hfill & & & \\text{Integrate}.\\hfill \\\\ & =-\\frac{1}{2{x}^{2}}\\text{ln}x-\\frac{1}{4{x}^{2}}+C.\\hfill & & & \\text{Rewrite with positive integers.}\\end{array}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<p>In some cases it may be necessary to apply integration by parts more than once.<\/p>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div id=\"fs-id1165042015541\" data-type=\"problem\">\n<p id=\"fs-id1165042015546\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{x}^{2}{e}^{3x}dx[\/latex].<\/p>\n<\/div>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558893\">Show Solution<\/button><\/p>\n<div id=\"q44558893\" class=\"hidden-answer\" style=\"display: none\">\n<div id=\"fs-id1165040637308\" data-type=\"solution\">\n<p id=\"fs-id1165040637310\">Using LIATE, choose [latex]u={x}^{2}[\/latex] and [latex]dv={e}^{3x}dx[\/latex]. Thus, [latex]du=2xdx[\/latex] and [latex]v=\\displaystyle\\int {e}^{3x}dx=\\left(\\frac{1}{3}\\right){e}^{3x}[\/latex]. Therefore,<\/p>\n<div id=\"fs-id1165040740033\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u& =\\hfill & {x}^{2}\\hfill & & \\hfill dv& =\\hfill & {e}^{3x}dx\\hfill \\\\ \\hfill du& =\\hfill & 2xdx\\hfill & & \\hfill v& =\\hfill & \\displaystyle\\int {e}^{3x}dx=\\frac{1}{3}{e}^{3x}.\\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042240114\">Substituting into the integration-by-parts formula\u00a0produces<\/p>\n<div id=\"fs-id1165042240117\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int {x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\displaystyle\\int \\frac{2}{3}x{e}^{3x}dx[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165040756177\">We still cannot integrate [latex]\\displaystyle\\int \\frac{2}{3}x{e}^{3x}dx[\/latex] directly, but the integral now has a lower power on [latex]x[\/latex]. We can evaluate this new integral by using integration by parts again. To do this, choose [latex]u=x[\/latex] and [latex]dv=\\frac{2}{3}{e}^{3x}dx[\/latex]. Thus, [latex]du=dx[\/latex] and [latex]v=\\displaystyle\\int \\left(\\frac{2}{3}\\right){e}^{3x}dx=\\left(\\frac{2}{9}\\right){e}^{3x}[\/latex]. Now we have<\/p>\n<div id=\"fs-id1165042002748\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u& =\\hfill & x\\hfill & & \\hfill dv& =\\hfill & \\frac{2}{3}{e}^{3x}dx\\hfill \\\\ \\hfill du& =\\hfill & dx\\hfill & & \\hfill v& =\\hfill & \\displaystyle\\int \\frac{2}{3}{e}^{3x}dx=\\frac{2}{9}{e}^{3x}.\\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165040757531\">Substituting back into the previous equation yields<\/p>\n<div id=\"fs-id1165040757534\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}{x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\left(\\frac{2}{9}x{e}^{3x}-{\\displaystyle\\int }^{\\text{ }}\\frac{2}{9}{e}^{3x}dx\\right)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042110524\">After evaluating the last integral and simplifying, we obtain<\/p>\n<div id=\"fs-id1165042110527\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\displaystyle\\int {x}^{2}{e}^{3x}dx=\\frac{1}{3}{x}^{2}{e}^{3x}-\\frac{2}{9}x{e}^{3x}+\\frac{2}{27}{e}^{3x}+C[\/latex].<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div id=\"fs-id1165042035450\" data-type=\"problem\">\n<p id=\"fs-id1165042035456\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex].<\/p>\n<\/div>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558891\">Show Solution<\/button><\/p>\n<div id=\"q44558891\" class=\"hidden-answer\" style=\"display: none\">\n<p>This integral appears to have only one function\u2014namely, [latex]\\sin\\left(\\text{ln}x\\right)[\/latex] \u2014however, we can always use the constant function 1 as the other function. In this example, let\u2019s choose [latex]u=\\sin\\left(\\text{ln}x\\right)[\/latex] and [latex]dv=1dx[\/latex]. (The decision to use [latex]u=\\sin\\left(\\text{ln}x\\right)[\/latex] is easy. We can\u2019t choose [latex]dv=\\sin\\left(\\text{ln}x\\right)dx[\/latex] because if we could integrate it, we wouldn\u2019t be using integration by parts in the first place!) Consequently, [latex]du=\\frac{1}{x}\\cos\\left(\\text{ln}x\\right)dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}1dx=x[\/latex]. After applying integration by parts to the integral and simplifying, we have<\/p>\n<div id=\"fs-id1165042035489\" data-type=\"solution\">\n<div id=\"fs-id1165042257200\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}\\cos\\left(\\text{ln}x\\right)dx[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042110018\">Unfortunately, this process leaves us with a new integral that is very similar to the original. However, let\u2019s see what happens when we apply integration by parts again. This time let\u2019s choose [latex]u=\\cos\\left(\\text{ln}x\\right)[\/latex] and [latex]dv=1dx[\/latex], making [latex]du=\\text{-}\\frac{1}{x}\\sin\\left(\\text{ln}x\\right)dx[\/latex] and [latex]v={\\displaystyle\\int }^{\\text{ }}1dx=x[\/latex]. Substituting, we have<\/p>\n<div id=\"fs-id1165042110131\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-\\left(x\\cos\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}-\\sin\\left(\\text{ln}x\\right)dx\\right)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165040741882\">After simplifying, we obtain<\/p>\n<div id=\"fs-id1165040741886\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)-{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165040741980\">The last integral is now the same as the original. It may seem that we have simply gone in a circle, but now we can actually evaluate the integral. To see how to do this more clearly, substitute [latex]I={\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex]. Thus, the equation becomes<\/p>\n<div id=\"fs-id1165040742019\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]I=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)-I[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165040742068\">First, add [latex]I[\/latex] to both sides of the equation to obtain<\/p>\n<div id=\"fs-id1165040742075\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]2I=x\\sin\\left(\\text{ln}x\\right)-x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042266548\">Next, divide by 2:<\/p>\n<div id=\"fs-id1165042266551\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]I=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042266606\">Substituting [latex]I={\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx[\/latex] again, we have<\/p>\n<div id=\"fs-id1165042266641\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042266721\">From this we see that [latex]\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)[\/latex] is an antiderivative of [latex]\\sin\\left(\\text{ln}x\\right)dx[\/latex]. For the most general antiderivative, add [latex]+C\\text{:}[\/latex]<\/p>\n<div id=\"fs-id1165042001966\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]{\\displaystyle\\int }^{\\text{ }}\\sin\\left(\\text{ln}x\\right)dx=\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)+C[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<\/div>\n<div id=\"fs-id1165042002057\" data-type=\"commentary\">\n<div data-type=\"title\"><strong>Analysis<\/strong><\/div>\n<p id=\"fs-id1165042002062\">If this method feels a little strange at first, we can check the answer by differentiation:<\/p>\n<div id=\"fs-id1165042002066\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{c}\\frac{d}{dx}\\left(\\frac{1}{2}x\\sin\\left(\\text{ln}x\\right)-\\frac{1}{2}x\\cos\\left(\\text{ln}x\\right)\\right)\\hfill \\\\ \\\\ =\\frac{1}{2}\\left(\\sin\\left(\\text{ln}x\\right)\\right)+\\cos\\left(\\text{ln}x\\right)\\cdot \\frac{1}{x}\\cdot \\frac{1}{2}x-\\left(\\frac{1}{2}\\cos\\left(\\text{ln}x\\right)-\\sin\\left(\\text{ln}x\\right)\\cdot \\frac{1}{x}\\cdot \\frac{1}{2}x\\right)\\hfill \\\\ =\\sin\\left(\\text{ln}x\\right).\\hfill \\end{array}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox proTip\" aria-label=\"Pro Tip\"><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-2132 alignleft\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images-archive-read-only\/wp-content\/uploads\/sites\/1468\/2016\/03\/22011815\/traffic-sign-160659-300x265.png\" alt=\"Caution\" width=\"62\" height=\"55\" \/>Caution! LIATE is a guide, not a rigid rule. If your first choice leads to an integral you can&#8217;t evaluate, try a different approach.<\/section>\n<section class=\"textbox example\" aria-label=\"Example\">\n<div id=\"fs-id1165042132631\" data-type=\"problem\">\n<p id=\"fs-id1165042132636\">Evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{t}^{3}{e}^{{t}^{2}}dt[\/latex].<\/p>\n<\/div>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q44558892\">Show Solution<\/button><\/p>\n<div id=\"q44558892\" class=\"hidden-answer\" style=\"display: none\">\n<div id=\"fs-id1165042132671\" data-type=\"solution\">\n<p id=\"fs-id1165042132674\">If we use a strict interpretation of the mnemonic LIATE to make our choice of [latex]u[\/latex], we end up with [latex]u={t}^{3}[\/latex] and [latex]dv={e}^{{t}^{2}}dt[\/latex]. Unfortunately, this choice won\u2019t work because we are unable to evaluate [latex]{\\displaystyle\\int }^{\\text{ }}{e}^{{t}^{2}}dt[\/latex]. However, since we can evaluate [latex]{\\displaystyle\\int }^{\\text{ }}t{e}^{{t}^{2}}dx[\/latex], we can try choosing [latex]u={t}^{2}[\/latex] and [latex]dv=t{e}^{{t}^{2}}dt[\/latex]. With these choices we have<\/p>\n<div id=\"fs-id1165040715819\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{ccccccc}\\hfill u& =\\hfill & {t}^{2}\\hfill & & \\hfill dv& =\\hfill & t{e}^{{t}^{2}}dt\\hfill \\\\ \\hfill du& =\\hfill & 2tdt\\hfill & & \\hfill v& =\\hfill & {\\displaystyle\\int }^{\\text{ }}t{e}^{{t}^{2}}dt=\\frac{1}{2}{e}^{{t}^{2}}.\\hfill \\end{array}[\/latex]<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1165042013342\">Thus, we obtain<\/p>\n<div id=\"fs-id1165042013345\" class=\"unnumbered\" style=\"text-align: center;\" data-type=\"equation\" data-label=\"\">[latex]\\begin{array}{cc}{\\displaystyle\\int {t}^{3}{e}^{{t}^{2}}dt}\\hfill & =\\frac{1}{2}{t}^{2}{e}^{{t}^{2}}-{\\displaystyle\\int \\frac{1}{2}{e}^{{t}^{2}}2tdt}\\hfill \\\\ \\hfill & =\\frac{1}{2}{t}^{2}{e}^{{t}^{2}}-\\frac{1}{2}{e}^{{t}^{2}}+C.\\end{array}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox tryIt\" aria-label=\"Try It\"><iframe loading=\"lazy\" id=\"ohm311291\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=311291&theme=lumen&iframe_resize_id=ohm311291&source=tnh\" width=\"100%\" height=\"150\"><\/iframe><\/section>\n","protected":false},"author":15,"menu_order":8,"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\/689"}],"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\/689\/revisions"}],"predecessor-version":[{"id":2282,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapters\/689\/revisions\/2282"}],"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\/689\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/media?parent=689"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/pressbooks\/v2\/chapter-type?post=689"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/contributor?post=689"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus2\/wp-json\/wp\/v2\/license?post=689"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}