{"id":258,"date":"2023-09-20T22:48:37","date_gmt":"2023-09-20T22:48:37","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/derivatives-of-inverse-trigonometric-functions\/"},"modified":"2024-08-05T12:53:40","modified_gmt":"2024-08-05T12:53:40","slug":"derivatives-of-inverse-functions-learn-it-2","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/derivatives-of-inverse-functions-learn-it-2\/","title":{"raw":"Derivatives of Inverse Functions: Learn It 2","rendered":"Derivatives of Inverse Functions: Learn It 2"},"content":{"raw":"<h2>Derivatives of Inverse Trigonometric Functions<\/h2>\r\n<p id=\"fs-id1169739029363\">We now shift our focus to the derivatives of inverse trigonometric functions, which play a crucial role in the study of integration later in this course. Intriguingly, unlike their trigonometric counterparts, the derivatives of inverse trigonometric functions are algebraic. This is a notable deviation from previous patterns observed, where derivatives of algebraic functions typically remained algebraic, and derivatives of trigonometric functions were also trigonometric. This departure underscores an important mathematical insight: the derivative of a function does not necessarily share the same type as the original function.<\/p>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739188589\">Use the inverse function theorem to find the derivative of [latex]g(x)=\\sin^{-1} x[\/latex].<\/p>\r\n<p>[reveal-answer q=\"fs-id1169739269789\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739269789\"]<\/p>\r\n<p id=\"fs-id1169739269789\">Since for [latex]x[\/latex] in the interval [latex][-\\frac{\\pi}{2},\\frac{\\pi}{2}], \\, f(x)= \\sin x[\/latex] is the inverse of [latex]g(x)= \\sin^{-1} x[\/latex], begin by finding [latex]f^{\\prime}(x)[\/latex].<\/p>\r\n<p>Since:<\/p>\r\n<div id=\"fs-id1169736611678\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)= \\cos x[\/latex] and [latex]f^{\\prime}(g(x))= \\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex],<\/div>\r\n<p id=\"fs-id1169739347090\">we see that:<\/p>\r\n<div id=\"fs-id1169739369239\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]g^{\\prime}(x)=\\frac{d}{dx}(\\sin^{-1} x)=\\frac{1}{f^{\\prime}(g(x))}=\\frac{1}{\\sqrt{1-x^2}}[\/latex]<\/div>\r\n<p><strong>Analysis<\/strong><\/p>\r\n<p id=\"fs-id1169739111057\">To see that [latex]\\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex], consider the following argument. Set [latex]\\sin^{-1} x=\\theta[\/latex]. In this case, [latex]\\sin \\theta =x[\/latex] where [latex]-\\frac{\\pi}{2}\\le \\theta \\le \\frac{\\pi}{2}[\/latex]. We begin by considering the case where [latex]0&lt;\\theta &lt;\\frac{\\pi}{2}[\/latex]. Since [latex]\\theta[\/latex] is an acute angle, we may construct a right triangle having acute angle [latex]\\theta[\/latex], a hypotenuse of length 1, and the side opposite angle [latex]\\theta [\/latex] having length [latex]x[\/latex]. From the Pythagorean theorem, the side adjacent to angle [latex]\\theta[\/latex] has length [latex]\\sqrt{1-x^2}[\/latex]. This triangle is shown in Figure 2. Using the triangle, we see that [latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex].<\/p>\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"426\"]<img class=\"\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205436\/CNX_Calc_Figure_03_07_002.jpg\" alt=\"A right triangle with angle \u03b8, opposite side x, hypotenuse 1, and adjacent side equal to the square root of the quantity (1 \u2013 x2).\" width=\"426\" height=\"205\" \/> Figure 2. Using a right triangle having acute angle [latex]\\theta[\/latex], a hypotenuse of length 1, and the side opposite angle [latex]\\theta[\/latex] having length [latex]x[\/latex], we can see that [latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex].[\/caption]\r\n\r\n<div id=\"fs-id1169739303300\" class=\"equation unnumbered\">In the case where [latex]-\\frac{\\pi}{2}&lt;\\theta &lt;0[\/latex], we make the observation that [latex]0&lt;-\\theta&lt;\\frac{\\pi}{2}[\/latex] and hence [latex]\\cos (\\sin^{-1} x)= \\cos \\theta = \\cos (\u2212\\theta )=\\sqrt{1-x^2}[\/latex].<\/div>\r\n<p id=\"fs-id1169736611289\">Now if [latex]\\theta =\\frac{\\pi}{2}[\/latex] or [latex]\\theta =-\\frac{\\pi}{2}, \\, x=1[\/latex] or [latex]x=-1[\/latex], and since in either case [latex]\\cos \\theta =0[\/latex] and [latex]\\sqrt{1-x^2}=0[\/latex], we have<\/p>\r\n<div id=\"fs-id1169739340290\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex]<\/div>\r\n<p id=\"fs-id1169739190632\">Consequently, in all cases, [latex]\\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex].<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739190553\">Apply the chain rule to find the derivative of [latex]h(x)=\\sin^{-1} (g(x))[\/latex] and use this result to find the derivative of [latex]h(x)=\\sin^{-1}(2x^3)[\/latex].<\/p>\r\n<p>[reveal-answer q=\"fs-id1169739189899\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739189899\"]<\/p>\r\n<p id=\"fs-id1169739189899\">Applying the chain rule to [latex]h(x)=\\sin^{-1} (g(x))[\/latex], we have<\/p>\r\n<div id=\"fs-id1169736596017\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]h^{\\prime}(x)=\\dfrac{1}{\\sqrt{1-(g(x))^2}}g^{\\prime}(x)[\/latex].<\/div>\r\n<p>&nbsp;<\/p>\r\n<p id=\"fs-id1169739269950\">Now let [latex]g(x)=2x^3[\/latex], so [latex]g^{\\prime}(x)=6x^{2}[\/latex]. Substituting into the previous result, we obtain<\/p>\r\n<div id=\"fs-id1169739336080\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{ll} h^{\\prime}(x) &amp; =\\dfrac{1}{\\sqrt{1-4x^6}} \\cdot 6x^{2} \\\\ &amp; =\\dfrac{6x^{2}}{\\sqrt{1-4x^6}} \\end{array}[\/latex]<\/div>\r\n<p>Watch the following video to see the worked solution to this example.<\/p>\r\n<center><iframe title=\"YouTube video player\" src=\"https:\/\/www.youtube.com\/embed\/0dlA5QJZYsw?controls=0&amp;start=628&amp;end=723&amp;autoplay=0\" width=\"750\" height=\"450\" frameborder=\"0\" allowfullscreen=\"allowfullscreen\" data-mce-fragment=\"1\"><\/iframe><\/center>\r\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>\r\n<p>You can view the <a href=\"https:\/\/oerfiles.s3.us-west-2.amazonaws.com\/Calculus\/Calculus1+Videos\/3.7DerivativesOfInverseFunctions628to723_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of \"3.7 Derivatives of Inverse Functions (edited)\" here (opens in new window)<\/a>.<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<p id=\"fs-id1169739282743\">The derivatives of the remaining inverse trigonometric functions may also be found by using the inverse function theorem. These formulas are provided in the following theorem.<\/p>\r\n<section class=\"textbox keyTakeaway\">\r\n<h3 style=\"text-align: left;\">derivatives of inverse trigonometric functions<\/h3>\r\n<p style=\"text-align: center;\">[latex]\\begin{array}{lllll}\\frac{d}{dx}(\\sin^{-1} x)=\\large \\frac{1}{\\sqrt{1-x^2}} &amp; &amp; &amp; &amp; \\frac{d}{dx}(\\cos^{-1} x)=\\large \\frac{-1}{\\sqrt{1-x^2}} \\\\ \\frac{d}{dx}(\\tan^{-1} x)=\\large \\frac{1}{1+x^2} &amp; &amp; &amp; &amp; \\frac{d}{dx}(\\cot^{-1} x)=\\large \\frac{-1}{1+x^2} \\\\ \\frac{d}{dx}(\\sec^{-1} x)=\\large \\frac{1}{|x|\\sqrt{x^2-1}} &amp; &amp; &amp; &amp; \\frac{d}{dx}(\\csc^{-1} x)=\\large \\frac{-1}{|x|\\sqrt{x^2-1}} \\end{array}[\/latex]<\/p>\r\n<\/section>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169736654830\">Find the derivative of [latex]f(x)=\\tan^{-1} (x^2)[\/latex]<\/p>\r\n<p>[reveal-answer q=\"fs-id1169739270394\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739270394\"]<\/p>\r\n<p id=\"fs-id1169739270394\">Let [latex]g(x)=x^2[\/latex], so [latex]g^{\\prime}(x)=2x[\/latex]. Substituting into [latex]\\frac{d}{dx}(\\tan^{-1} x)=\\large \\frac{1}{1+x^2}[\/latex], we obtain<\/p>\r\n<div id=\"fs-id1169736661176\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)=\\frac{1}{1+(x^2)^2} \\cdot (2x)[\/latex]<\/div>\r\n<p id=\"fs-id1169736595973\">Simplifying, we have<\/p>\r\n<div id=\"fs-id1169736595976\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)=\\frac{2x}{1+x^4}[\/latex]<\/div>\r\n\r\n[\/hidden-answer]<\/section>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739208500\">The position of a particle at time [latex]t[\/latex] is given by [latex]s(t)= \\tan^{-1}\\left(\\dfrac{1}{t}\\right)[\/latex] for [latex]t\\ge \\frac{1}{2}[\/latex]. Find the velocity of the particle at time [latex]t=1[\/latex].<\/p>\r\n<p>[reveal-answer q=\"fs-id1169736656603\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169736656603\"]<\/p>\r\n<p id=\"fs-id1169736656603\">Begin by differentiating [latex]s(t)[\/latex] in order to find [latex]v(t)[\/latex]. Thus,<\/p>\r\n<div id=\"fs-id1169739242485\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]v(t)=s^{\\prime}(t)=\\dfrac{1}{1+(\\frac{1}{t})^2} \\cdot \\dfrac{-1}{t^2}[\/latex]<\/div>\r\n<p id=\"fs-id1169739282656\">Simplifying, we have<\/p>\r\n<div id=\"fs-id1169736615257\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]v(t)=-\\dfrac{1}{t^2+1}[\/latex]<\/div>\r\n<p id=\"fs-id1169736594230\" style=\"text-align: center;\">Thus, [latex]v(1)=-\\dfrac{1}{2}[\/latex]<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<section class=\"textbox tryIt\">\r\n<p>[ohm_question hide_question_numbers=1]206679[\/ohm_question]<\/p>\r\n<\/section>","rendered":"<h2>Derivatives of Inverse Trigonometric Functions<\/h2>\n<p id=\"fs-id1169739029363\">We now shift our focus to the derivatives of inverse trigonometric functions, which play a crucial role in the study of integration later in this course. Intriguingly, unlike their trigonometric counterparts, the derivatives of inverse trigonometric functions are algebraic. This is a notable deviation from previous patterns observed, where derivatives of algebraic functions typically remained algebraic, and derivatives of trigonometric functions were also trigonometric. This departure underscores an important mathematical insight: the derivative of a function does not necessarily share the same type as the original function.<\/p>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739188589\">Use the inverse function theorem to find the derivative of [latex]g(x)=\\sin^{-1} x[\/latex].<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739269789\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739269789\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169739269789\">Since for [latex]x[\/latex] in the interval [latex][-\\frac{\\pi}{2},\\frac{\\pi}{2}], \\, f(x)= \\sin x[\/latex] is the inverse of [latex]g(x)= \\sin^{-1} x[\/latex], begin by finding [latex]f^{\\prime}(x)[\/latex].<\/p>\n<p>Since:<\/p>\n<div id=\"fs-id1169736611678\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)= \\cos x[\/latex] and [latex]f^{\\prime}(g(x))= \\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex],<\/div>\n<p id=\"fs-id1169739347090\">we see that:<\/p>\n<div id=\"fs-id1169739369239\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]g^{\\prime}(x)=\\frac{d}{dx}(\\sin^{-1} x)=\\frac{1}{f^{\\prime}(g(x))}=\\frac{1}{\\sqrt{1-x^2}}[\/latex]<\/div>\n<p><strong>Analysis<\/strong><\/p>\n<p id=\"fs-id1169739111057\">To see that [latex]\\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex], consider the following argument. Set [latex]\\sin^{-1} x=\\theta[\/latex]. In this case, [latex]\\sin \\theta =x[\/latex] where [latex]-\\frac{\\pi}{2}\\le \\theta \\le \\frac{\\pi}{2}[\/latex]. We begin by considering the case where [latex]0<\\theta <\\frac{\\pi}{2}[\/latex]. Since [latex]\\theta[\/latex] is an acute angle, we may construct a right triangle having acute angle [latex]\\theta[\/latex], a hypotenuse of length 1, and the side opposite angle [latex]\\theta[\/latex] having length [latex]x[\/latex]. From the Pythagorean theorem, the side adjacent to angle [latex]\\theta[\/latex] has length [latex]\\sqrt{1-x^2}[\/latex]. This triangle is shown in Figure 2. Using the triangle, we see that [latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex].<\/p>\n<figure style=\"width: 426px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205436\/CNX_Calc_Figure_03_07_002.jpg\" alt=\"A right triangle with angle \u03b8, opposite side x, hypotenuse 1, and adjacent side equal to the square root of the quantity (1 \u2013 x2).\" width=\"426\" height=\"205\" \/><figcaption class=\"wp-caption-text\">Figure 2. Using a right triangle having acute angle [latex]\\theta[\/latex], a hypotenuse of length 1, and the side opposite angle [latex]\\theta[\/latex] having length [latex]x[\/latex], we can see that [latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex].<\/figcaption><\/figure>\n<div id=\"fs-id1169739303300\" class=\"equation unnumbered\">In the case where [latex]-\\frac{\\pi}{2}<\\theta <0[\/latex], we make the observation that [latex]0<-\\theta<\\frac{\\pi}{2}[\/latex] and hence [latex]\\cos (\\sin^{-1} x)= \\cos \\theta = \\cos (\u2212\\theta )=\\sqrt{1-x^2}[\/latex].<\/div>\n<p id=\"fs-id1169736611289\">Now if [latex]\\theta =\\frac{\\pi}{2}[\/latex] or [latex]\\theta =-\\frac{\\pi}{2}, \\, x=1[\/latex] or [latex]x=-1[\/latex], and since in either case [latex]\\cos \\theta =0[\/latex] and [latex]\\sqrt{1-x^2}=0[\/latex], we have<\/p>\n<div id=\"fs-id1169739340290\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\cos (\\sin^{-1} x)= \\cos \\theta =\\sqrt{1-x^2}[\/latex]<\/div>\n<p id=\"fs-id1169739190632\">Consequently, in all cases, [latex]\\cos (\\sin^{-1} x)=\\sqrt{1-x^2}[\/latex].<\/p>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739190553\">Apply the chain rule to find the derivative of [latex]h(x)=\\sin^{-1} (g(x))[\/latex] and use this result to find the derivative of [latex]h(x)=\\sin^{-1}(2x^3)[\/latex].<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739189899\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739189899\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169739189899\">Applying the chain rule to [latex]h(x)=\\sin^{-1} (g(x))[\/latex], we have<\/p>\n<div id=\"fs-id1169736596017\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]h^{\\prime}(x)=\\dfrac{1}{\\sqrt{1-(g(x))^2}}g^{\\prime}(x)[\/latex].<\/div>\n<p>&nbsp;<\/p>\n<p id=\"fs-id1169739269950\">Now let [latex]g(x)=2x^3[\/latex], so [latex]g^{\\prime}(x)=6x^{2}[\/latex]. Substituting into the previous result, we obtain<\/p>\n<div id=\"fs-id1169739336080\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]\\begin{array}{ll} h^{\\prime}(x) & =\\dfrac{1}{\\sqrt{1-4x^6}} \\cdot 6x^{2} \\\\ & =\\dfrac{6x^{2}}{\\sqrt{1-4x^6}} \\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\/0dlA5QJZYsw?controls=0&amp;start=628&amp;end=723&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\/3.7DerivativesOfInverseFunctions628to723_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of &#8220;3.7 Derivatives of Inverse Functions (edited)&#8221; here (opens in new window)<\/a>.<\/p>\n<\/div>\n<\/div>\n<\/section>\n<p id=\"fs-id1169739282743\">The derivatives of the remaining inverse trigonometric functions may also be found by using the inverse function theorem. These formulas are provided in the following theorem.<\/p>\n<section class=\"textbox keyTakeaway\">\n<h3 style=\"text-align: left;\">derivatives of inverse trigonometric functions<\/h3>\n<p style=\"text-align: center;\">[latex]\\begin{array}{lllll}\\frac{d}{dx}(\\sin^{-1} x)=\\large \\frac{1}{\\sqrt{1-x^2}} & & & & \\frac{d}{dx}(\\cos^{-1} x)=\\large \\frac{-1}{\\sqrt{1-x^2}} \\\\ \\frac{d}{dx}(\\tan^{-1} x)=\\large \\frac{1}{1+x^2} & & & & \\frac{d}{dx}(\\cot^{-1} x)=\\large \\frac{-1}{1+x^2} \\\\ \\frac{d}{dx}(\\sec^{-1} x)=\\large \\frac{1}{|x|\\sqrt{x^2-1}} & & & & \\frac{d}{dx}(\\csc^{-1} x)=\\large \\frac{-1}{|x|\\sqrt{x^2-1}} \\end{array}[\/latex]<\/p>\n<\/section>\n<section class=\"textbox example\">\n<p id=\"fs-id1169736654830\">Find the derivative of [latex]f(x)=\\tan^{-1} (x^2)[\/latex]<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739270394\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739270394\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169739270394\">Let [latex]g(x)=x^2[\/latex], so [latex]g^{\\prime}(x)=2x[\/latex]. Substituting into [latex]\\frac{d}{dx}(\\tan^{-1} x)=\\large \\frac{1}{1+x^2}[\/latex], we obtain<\/p>\n<div id=\"fs-id1169736661176\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)=\\frac{1}{1+(x^2)^2} \\cdot (2x)[\/latex]<\/div>\n<p id=\"fs-id1169736595973\">Simplifying, we have<\/p>\n<div id=\"fs-id1169736595976\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]f^{\\prime}(x)=\\frac{2x}{1+x^4}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739208500\">The position of a particle at time [latex]t[\/latex] is given by [latex]s(t)= \\tan^{-1}\\left(\\dfrac{1}{t}\\right)[\/latex] for [latex]t\\ge \\frac{1}{2}[\/latex]. Find the velocity of the particle at time [latex]t=1[\/latex].<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169736656603\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169736656603\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169736656603\">Begin by differentiating [latex]s(t)[\/latex] in order to find [latex]v(t)[\/latex]. Thus,<\/p>\n<div id=\"fs-id1169739242485\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]v(t)=s^{\\prime}(t)=\\dfrac{1}{1+(\\frac{1}{t})^2} \\cdot \\dfrac{-1}{t^2}[\/latex]<\/div>\n<p id=\"fs-id1169739282656\">Simplifying, we have<\/p>\n<div id=\"fs-id1169736615257\" class=\"equation unnumbered\" style=\"text-align: center;\">[latex]v(t)=-\\dfrac{1}{t^2+1}[\/latex]<\/div>\n<p id=\"fs-id1169736594230\" style=\"text-align: center;\">Thus, [latex]v(1)=-\\dfrac{1}{2}[\/latex]<\/p>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox tryIt\">\n<iframe loading=\"lazy\" id=\"ohm206679\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=206679&theme=lumen&iframe_resize_id=ohm206679&source=tnh\" width=\"100%\" height=\"150\"><\/iframe><br \/>\n<\/section>\n","protected":false},"author":6,"menu_order":16,"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\":\"3.7 Derivatives of Inverse Functions (edited)\",\"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":560,"module-header":"learn_it","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":"3.7 Derivatives of Inverse Functions (edited)","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\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/258"}],"collection":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/users\/6"}],"version-history":[{"count":9,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/258\/revisions"}],"predecessor-version":[{"id":4528,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/258\/revisions\/4528"}],"part":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/parts\/560"}],"metadata":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/258\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/media?parent=258"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapter-type?post=258"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/contributor?post=258"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/license?post=258"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}