{"id":245,"date":"2023-09-20T22:48:32","date_gmt":"2023-09-20T22:48:32","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/rate-of-change-applications\/"},"modified":"2024-08-05T12:43:24","modified_gmt":"2024-08-05T12:43:24","slug":"derivatives-as-rates-of-change-learn-it-2","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/derivatives-as-rates-of-change-learn-it-2\/","title":{"raw":"Derivatives as Rates of Change: Learn It 2","rendered":"Derivatives as Rates of Change: Learn It 2"},"content":{"raw":"<h2>Rate of Change Applications<\/h2>\r\n<h3>Motion Along a Line<\/h3>\r\n<p id=\"fs-id1169738881072\">Another use for the derivative is to analyze motion along a line.<\/p>\r\n<p>Velocity is the rate of change of position. By taking the derivative of velocity, we can find acceleration, which is the rate of change of velocity. Additionally, it's important to introduce the concept of speed, which is the magnitude of velocity. Thus, we can state the following mathematical definitions:<\/p>\r\n<section class=\"textbox keyTakeaway\">\r\n<h3>velocity, speed and acceleration<\/h3>\r\n<p id=\"fs-id1169738947283\">Let [latex]s(t)[\/latex] be a function giving the position of an object at time [latex]t[\/latex].<\/p>\r\n<ul>\r\n\t<li id=\"fs-id1169739195686\">The <strong>velocity<\/strong> of the object at time [latex]t[\/latex] is given by [latex]v(t)=s^{\\prime}(t)[\/latex].<\/li>\r\n\t<li>The <strong>speed<\/strong> of the object at time [latex]t[\/latex] is given by [latex]|v(t)|[\/latex].<\/li>\r\n\t<li>The <strong>acceleration<\/strong> of the object at [latex]t[\/latex] is given by [latex]a(t)=v^{\\prime}(t)=s''(t)[\/latex].<\/li>\r\n<\/ul>\r\n<\/section>\r\n<section class=\"textbox proTip\">\r\n<p>Many of the problems involving position, velocity and acceleration will require finding zeros of quadratic and higher order polynomial functions. To find these zeros, recall that factoring and setting each factor equal to zero will be the easiest way to solve these functions. If it doesn't factor and it is a quadratic, the quadratic equation will always work.<\/p>\r\n<\/section>\r\n<div id=\"fs-id1169738906211\" class=\"textbook exercises\">\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169738942237\">A ball is dropped from a height of [latex]64[\/latex] feet. Its height above ground (in feet) [latex]t[\/latex] seconds later is given by [latex]s(t)=-16t^2+64[\/latex].<\/p>\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"386\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205359\/CNX_Calc_Figure_03_04_002.jpg\" alt=\"On the Cartesian coordinate plane, the function s(t) = \u221216t2 + 64 is graphed. This function starts at (0, 64) and decreases to (0, 2).\" width=\"386\" height=\"315\" \/> Figure 2. Dropped ball graph, height vs. time.[\/caption]\r\n\r\n<ol id=\"fs-id1169738940918\" style=\"list-style-type: lower-alpha;\">\r\n\t<li>What is the instantaneous velocity of the ball when it hits the ground?<\/li>\r\n\t<li>What is the average velocity during its fall?<\/li>\r\n<\/ol>\r\n<p>[reveal-answer q=\"fs-id1169739233455\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739233455\"]<\/p>\r\n<p id=\"fs-id1169739233455\">The first thing to do is determine how long it takes the ball to reach the ground. To do this, set [latex]s(t)=0[\/latex]. Solving [latex]-16t^2+64=0[\/latex], we get [latex]t=2[\/latex], so it takes [latex]2[\/latex] seconds for the ball to reach the ground.<\/p>\r\n<ol id=\"fs-id1169739220828\" style=\"list-style-type: lower-alpha;\">\r\n\t<li>The instantaneous velocity of the ball as it strikes the ground is [latex]v(2)[\/latex]. Since [latex]v(t)=s^{\\prime}(t)=-32t[\/latex] m we obtain [latex]v(t)=-64[\/latex] ft\/s.<\/li>\r\n\t<li>The average velocity of the ball during its fall is<br \/>\r\n<div id=\"fs-id1169739018761\" class=\"equation unnumbered\">[latex]v_{avg}=\\frac{s(2)-s(0)}{2-0}=\\frac{0-64}{2}=-32[\/latex] ft\/s.<\/div>\r\n<\/li>\r\n<\/ol>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739231121\">The position of a particle moving along a coordinate axis is given by [latex]s(t)=t^3-9t^2+24t+4, \\, t\\ge 0[\/latex].<\/p>\r\n<ol id=\"fs-id1169738912848\" style=\"list-style-type: lower-alpha;\">\r\n\t<li>Find [latex]v(t)[\/latex].<\/li>\r\n\t<li>At what time(s) is the particle at rest?<\/li>\r\n\t<li>On what time intervals is the particle moving from left to right? From right to left?<\/li>\r\n\t<li>Use the information obtained to sketch the path of the particle along a coordinate axis.<\/li>\r\n<\/ol>\r\n<p>[reveal-answer q=\"fs-id1169739340338\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739340338\"]<\/p>\r\n<ol id=\"fs-id1169739340338\" style=\"list-style-type: lower-alpha;\">\r\n\t<li>The velocity is the derivative of the position function:<br \/>\r\n<div id=\"fs-id1169739198570\" class=\"equation unnumbered\">[latex]v(t)=s^{\\prime}(t)=3t^2-18t+24[\/latex].<\/div>\r\n<\/li>\r\n\t<li>The particle is at rest when [latex]v(t)=0[\/latex], so set [latex]3t^2-18t+24=0[\/latex]. Factoring the left-hand side of the equation produces [latex]3(t-2)(t-4)=0[\/latex]. Solving, we find that the particle is at rest at [latex]t=2[\/latex] and [latex]t=4[\/latex].<\/li>\r\n\t<li>The particle is moving from left to right when [latex]v(t)&gt;0[\/latex] and from right to left when [latex]v(t)&lt;0[\/latex]. The graph below gives the analysis of the sign of [latex]v(t)[\/latex] for [latex]t\\ge 0[\/latex], but it does not represent the axis along which the particle is moving.\r\n[caption id=\"\" align=\"aligncenter\" width=\"487\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205402\/CNX_Calc_Figure_03_04_003.jpg\" alt=\"A number line marked with 0, 2, and 4. Between 0 and 2, there is a plus sign. Above 2, there is a 0. Between 2 and 4 there is a negative sign. Above 4 there is a 0. After 4 there is a plus sign and v(t).\" width=\"487\" height=\"67\" \/> Figure 3. The sign of v(t) determines the direction of the particle.[\/caption]\r\n\r\n<div class=\"wp-caption-text\" style=\"text-align: center;\">\u00a0<\/div>\r\n<p style=\"text-align: left;\">Since [latex]3t^2-18t+24&gt;0[\/latex] on [latex][0,2)\\cup (2,+\\infty)[\/latex], the particle is moving from left to right on these intervals.<br \/>\r\nSince [latex]3t^2-18t+24&lt;0[\/latex] on [latex](2,4)[\/latex], the particle is moving from right to left on this interval.<\/p>\r\n<\/li>\r\n\t<li>Before we can sketch the graph of the particle, we need to know its position at the time it starts moving [latex](t=0)[\/latex] and at the times that it changes direction [latex](t=2,4)[\/latex]. We have [latex]s(0)=4, \\, s(2)=24[\/latex], and [latex]s(4)=20[\/latex]. This means that the particle begins on the coordinate axis at 4 and changes direction at 0 and 20 on the coordinate axis. The path of the particle is shown on a coordinate axis in the graph below.\r\n[caption id=\"\" align=\"aligncenter\" width=\"484\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205404\/CNX_Calc_Figure_03_04_005.jpg\" alt=\"A number line is given and above it a line snakes, starting at t = 0 above 4 on the number line. Then the line at t = 2 is above 24 on the number line. Then the line decreases at t = 4 to be above 20 on the number line, at which point the line reverses direction again and increases indefinitely.\" width=\"484\" height=\"109\" \/> Figure 4. The path of the particle can be determined by analyzing [latex]v(t)[\/latex].[\/caption]\r\n<\/li>\r\n<\/ol>\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\/XOgb95xhWF0?controls=0&amp;start=527&amp;end=950&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\/3.4DerivativesAsRatesOfChange527to950_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of \"3.4 Derivatives as Rates of Change\" here (opens in new window)<\/a>.<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<\/div>\r\n<div id=\"fs-id1169736660682\" class=\"textbook key-takeaways\">\r\n<section class=\"textbox tryIt\">\r\n<p>[ohm_question hide_question_numbers=1]205568[\/ohm_question]<\/p>\r\n<\/section>\r\n<\/div>","rendered":"<h2>Rate of Change Applications<\/h2>\n<h3>Motion Along a Line<\/h3>\n<p id=\"fs-id1169738881072\">Another use for the derivative is to analyze motion along a line.<\/p>\n<p>Velocity is the rate of change of position. By taking the derivative of velocity, we can find acceleration, which is the rate of change of velocity. Additionally, it&#8217;s important to introduce the concept of speed, which is the magnitude of velocity. Thus, we can state the following mathematical definitions:<\/p>\n<section class=\"textbox keyTakeaway\">\n<h3>velocity, speed and acceleration<\/h3>\n<p id=\"fs-id1169738947283\">Let [latex]s(t)[\/latex] be a function giving the position of an object at time [latex]t[\/latex].<\/p>\n<ul>\n<li id=\"fs-id1169739195686\">The <strong>velocity<\/strong> of the object at time [latex]t[\/latex] is given by [latex]v(t)=s^{\\prime}(t)[\/latex].<\/li>\n<li>The <strong>speed<\/strong> of the object at time [latex]t[\/latex] is given by [latex]|v(t)|[\/latex].<\/li>\n<li>The <strong>acceleration<\/strong> of the object at [latex]t[\/latex] is given by [latex]a(t)=v^{\\prime}(t)=s''(t)[\/latex].<\/li>\n<\/ul>\n<\/section>\n<section class=\"textbox proTip\">\n<p>Many of the problems involving position, velocity and acceleration will require finding zeros of quadratic and higher order polynomial functions. To find these zeros, recall that factoring and setting each factor equal to zero will be the easiest way to solve these functions. If it doesn&#8217;t factor and it is a quadratic, the quadratic equation will always work.<\/p>\n<\/section>\n<div id=\"fs-id1169738906211\" class=\"textbook exercises\">\n<section class=\"textbox example\">\n<p id=\"fs-id1169738942237\">A ball is dropped from a height of [latex]64[\/latex] feet. Its height above ground (in feet) [latex]t[\/latex] seconds later is given by [latex]s(t)=-16t^2+64[\/latex].<\/p>\n<figure style=\"width: 386px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205359\/CNX_Calc_Figure_03_04_002.jpg\" alt=\"On the Cartesian coordinate plane, the function s(t) = \u221216t2 + 64 is graphed. This function starts at (0, 64) and decreases to (0, 2).\" width=\"386\" height=\"315\" \/><figcaption class=\"wp-caption-text\">Figure 2. Dropped ball graph, height vs. time.<\/figcaption><\/figure>\n<ol id=\"fs-id1169738940918\" style=\"list-style-type: lower-alpha;\">\n<li>What is the instantaneous velocity of the ball when it hits the ground?<\/li>\n<li>What is the average velocity during its fall?<\/li>\n<\/ol>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739233455\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739233455\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169739233455\">The first thing to do is determine how long it takes the ball to reach the ground. To do this, set [latex]s(t)=0[\/latex]. Solving [latex]-16t^2+64=0[\/latex], we get [latex]t=2[\/latex], so it takes [latex]2[\/latex] seconds for the ball to reach the ground.<\/p>\n<ol id=\"fs-id1169739220828\" style=\"list-style-type: lower-alpha;\">\n<li>The instantaneous velocity of the ball as it strikes the ground is [latex]v(2)[\/latex]. Since [latex]v(t)=s^{\\prime}(t)=-32t[\/latex] m we obtain [latex]v(t)=-64[\/latex] ft\/s.<\/li>\n<li>The average velocity of the ball during its fall is\n<div id=\"fs-id1169739018761\" class=\"equation unnumbered\">[latex]v_{avg}=\\frac{s(2)-s(0)}{2-0}=\\frac{0-64}{2}=-32[\/latex] ft\/s.<\/div>\n<\/li>\n<\/ol>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739231121\">The position of a particle moving along a coordinate axis is given by [latex]s(t)=t^3-9t^2+24t+4, \\, t\\ge 0[\/latex].<\/p>\n<ol id=\"fs-id1169738912848\" style=\"list-style-type: lower-alpha;\">\n<li>Find [latex]v(t)[\/latex].<\/li>\n<li>At what time(s) is the particle at rest?<\/li>\n<li>On what time intervals is the particle moving from left to right? From right to left?<\/li>\n<li>Use the information obtained to sketch the path of the particle along a coordinate axis.<\/li>\n<\/ol>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739340338\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739340338\" class=\"hidden-answer\" style=\"display: none\">\n<ol id=\"fs-id1169739340338\" style=\"list-style-type: lower-alpha;\">\n<li>The velocity is the derivative of the position function:\n<div id=\"fs-id1169739198570\" class=\"equation unnumbered\">[latex]v(t)=s^{\\prime}(t)=3t^2-18t+24[\/latex].<\/div>\n<\/li>\n<li>The particle is at rest when [latex]v(t)=0[\/latex], so set [latex]3t^2-18t+24=0[\/latex]. Factoring the left-hand side of the equation produces [latex]3(t-2)(t-4)=0[\/latex]. Solving, we find that the particle is at rest at [latex]t=2[\/latex] and [latex]t=4[\/latex].<\/li>\n<li>The particle is moving from left to right when [latex]v(t)>0[\/latex] and from right to left when [latex]v(t)<0[\/latex]. The graph below gives the analysis of the sign of [latex]v(t)[\/latex] for [latex]t\\ge 0[\/latex], but it does not represent the axis along which the particle is moving.\n\n\n<figure style=\"width: 487px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205402\/CNX_Calc_Figure_03_04_003.jpg\" alt=\"A number line marked with 0, 2, and 4. Between 0 and 2, there is a plus sign. Above 2, there is a 0. Between 2 and 4 there is a negative sign. Above 4 there is a 0. After 4 there is a plus sign and v(t).\" width=\"487\" height=\"67\" \/><figcaption class=\"wp-caption-text\">Figure 3. The sign of v(t) determines the direction of the particle.<\/figcaption><\/figure>\n<div class=\"wp-caption-text\" style=\"text-align: center;\">\u00a0<\/div>\n<p style=\"text-align: left;\">Since [latex]3t^2-18t+24>0[\/latex] on [latex][0,2)\\cup (2,+\\infty)[\/latex], the particle is moving from left to right on these intervals.<br \/>\nSince [latex]3t^2-18t+24<0[\/latex] on [latex](2,4)[\/latex], the particle is moving from right to left on this interval.<\/p>\n<\/li>\n<li>Before we can sketch the graph of the particle, we need to know its position at the time it starts moving [latex](t=0)[\/latex] and at the times that it changes direction [latex](t=2,4)[\/latex]. We have [latex]s(0)=4, \\, s(2)=24[\/latex], and [latex]s(4)=20[\/latex]. This means that the particle begins on the coordinate axis at 4 and changes direction at 0 and 20 on the coordinate axis. The path of the particle is shown on a coordinate axis in the graph below.<br \/>\n<figure style=\"width: 484px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205404\/CNX_Calc_Figure_03_04_005.jpg\" alt=\"A number line is given and above it a line snakes, starting at t = 0 above 4 on the number line. Then the line at t = 2 is above 24 on the number line. Then the line decreases at t = 4 to be above 20 on the number line, at which point the line reverses direction again and increases indefinitely.\" width=\"484\" height=\"109\" \/><figcaption class=\"wp-caption-text\">Figure 4. The path of the particle can be determined by analyzing [latex]v(t)[\/latex].<\/figcaption><\/figure>\n<\/li>\n<\/ol>\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\/XOgb95xhWF0?controls=0&amp;start=527&amp;end=950&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\/3.4DerivativesAsRatesOfChange527to950_transcript.txt\" target=\"_blank\" rel=\"noopener\">transcript for this segmented clip of &#8220;3.4 Derivatives as Rates of Change&#8221; here (opens in new window)<\/a>.<\/p>\n<\/div>\n<\/div>\n<\/section>\n<\/div>\n<div id=\"fs-id1169736660682\" class=\"textbook key-takeaways\">\n<section class=\"textbox tryIt\">\n<iframe loading=\"lazy\" id=\"ohm205568\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=205568&theme=lumen&iframe_resize_id=ohm205568&source=tnh\" width=\"100%\" height=\"150\"><\/iframe><br \/>\n<\/section>\n<\/div>\n","protected":false},"author":6,"menu_order":24,"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\":\"3.4 Derivatives as Rates of Change\",\"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":503,"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":"3.4 Derivatives as Rates of Change","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\/245"}],"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":8,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/245\/revisions"}],"predecessor-version":[{"id":4508,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/245\/revisions\/4508"}],"part":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/parts\/503"}],"metadata":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/245\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/media?parent=245"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapter-type?post=245"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/contributor?post=245"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/license?post=245"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}