{"id":231,"date":"2023-09-20T22:48:26","date_gmt":"2023-09-20T22:48:26","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/velocities-and-rates-of-change\/"},"modified":"2024-08-05T01:48:23","modified_gmt":"2024-08-05T01:48:23","slug":"defining-the-derivative-learn-it-3","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus1\/chapter\/defining-the-derivative-learn-it-3\/","title":{"raw":"Defining the Derivative: Learn It 3","rendered":"Defining the Derivative: Learn It 3"},"content":{"raw":"<h2>Velocities and Rates of Change<\/h2>\r\n<p id=\"fs-id1169739353680\">Now that we can evaluate a derivative, we can apply it to velocity problems. Recall that if [latex]s(t)[\/latex] is the position of an object moving along a coordinate axis, the <span class=\"no-emphasis\">average velocity<\/span> of the object over a time interval [latex][a,t][\/latex] if [latex]t&gt;a[\/latex] or [latex][t,a][\/latex] if [latex]t&lt;a[\/latex] is:<\/p>\r\n<div id=\"fs-id1169739303202\" class=\"equation\" style=\"text-align: center;\">[latex]v_{\\text{avg}}=\\dfrac{s(t)-s(a)}{t-a}[\/latex]<\/div>\r\n<p id=\"fs-id1169739189992\">As the values of [latex]t[\/latex] approach [latex]a[\/latex], the values of [latex]v_{\\text{avg}}[\/latex] approach the value we call the <span class=\"no-emphasis\">instantaneous velocity<\/span> at [latex]a[\/latex]. That is, instantaneous velocity at [latex]a[\/latex], denoted [latex]v(a)[\/latex], is given by<\/p>\r\n<div id=\"fs-id1169739274700\" class=\"equation\" style=\"text-align: center;\">[latex]v(a)=s^{\\prime}(a)=\\underset{t\\to a}{\\lim}\\dfrac{s(t)-s(a)}{t-a}[\/latex]<\/div>\r\n<p id=\"fs-id1169739064816\">To better understand the relationship between average velocity and instantaneous velocity, see Figure 7. In this figure, the slope of the tangent line (shown in red) is the instantaneous velocity of the object at time [latex]t=a[\/latex]. The slope of the secant line (shown in green) is the average velocity of the object over the time interval [latex][a,t][\/latex].<\/p>\r\n\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\/11205202\/CNX_Calc_Figure_03_01_007.jpg\" alt=\"This figure consists of the Cartesian coordinate plane with 0, a, and t1 marked on the t-axis. The function y = s(t) is graphed in the first quadrant along with two lines marked tangent and secant. The tangent line touches y = s(t) at only one point, (a, s(a)). The secant line touches y = s(t) at two points: (a, s(a)) and (t1, s(t1)).\" width=\"487\" height=\"284\" \/> Figure 7. The slope of the secant line is the average velocity over the interval [latex][a,t][\/latex]. The slope of the tangent line is the instantaneous velocity.[\/caption]\r\n\r\n<p id=\"fs-id1169736619727\">We can use the definitions to calculate the instantaneous velocity, or we can estimate the velocity of a moving object by using a table of values. We can then confirm the estimate by using the difference quotient.<\/p>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739188880\">A lead weight on a spring is oscillating up and down. Its position at time [latex]t[\/latex] with respect to a fixed horizontal line is given by [latex]s(t)= \\sin t[\/latex]. Use a table of values to estimate [latex]v(0)[\/latex]. Check the estimate by using the definition of a derivative.<\/p>\r\n\r\n[caption id=\"\" align=\"aligncenter\" width=\"325\"]<img src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/2332\/2018\/01\/11205205\/CNX_Calc_Figure_03_01_010.jpg\" alt=\"A picture of a spring hanging down with a weight at the end. There is a horizontal dashed line marked 0 a little bit above the weight.\" width=\"325\" height=\"192\" \/> Figure 8. A lead weight suspended from a spring in vertical oscillatory motion.[\/caption]\r\n\r\n<p>[reveal-answer q=\"fs-id1169738960040\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169738960040\"]<\/p>\r\n<p id=\"fs-id1169738960040\">We can estimate the instantaneous velocity at [latex]t=0[\/latex] by computing a table of average velocities using values of [latex]t[\/latex] approaching [latex]0[\/latex], as shown in the table below.<\/p>\r\n<table id=\"fs-id1169739242675\" summary=\"This table has seven rows and two columns. The first row is a header row and it labels each column. The first column header is x and the second column is (sin t - sin 0)\/(t \u2212 0) = (sin t)\/t. Under the first column are the values -0.1, -0.01, -0.001, 0.001, 0.01, and 0.1. Under the second column are the values 0.998334166, 0.9999833333, 0.999999833, 0.999999833, 0.9999833333, and 0.998334166.\">\r\n<caption>Average velocities using values of [latex]t[\/latex] approaching [latex]0[\/latex]<\/caption>\r\n<thead>\r\n<tr valign=\"top\">\r\n<th>[latex]t[\/latex]<\/th>\r\n<th>[latex]\\frac{\\sin t - \\sin 0}{t-0}=\\frac{\\sin t}{t}[\/latex]<\/th>\r\n<\/tr>\r\n<\/thead>\r\n<tbody>\r\n<tr>\r\n<td>[latex]-0.1[\/latex]<\/td>\r\n<td>[latex]0.998334166[\/latex]<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>[latex]-0.01[\/latex]<\/td>\r\n<td>[latex]0.9999833333[\/latex]<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>[latex]-0.001[\/latex]<\/td>\r\n<td>[latex]0.999999833[\/latex]<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>[latex]0.001[\/latex]<\/td>\r\n<td>[latex]0.999999833[\/latex]<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>[latex]0.01[\/latex]<\/td>\r\n<td>[latex]0.9999833333[\/latex]<\/td>\r\n<\/tr>\r\n<tr>\r\n<td>[latex]0.1[\/latex]<\/td>\r\n<td>[latex]0.998334166[\/latex]<\/td>\r\n<\/tr>\r\n<\/tbody>\r\n<\/table>\r\n<p id=\"fs-id1169739188902\">From the table we see that the average velocity over the time interval [latex][-0.1,0][\/latex] is [latex]0.998334166[\/latex], the average velocity over the time interval [latex][-0.01,0][\/latex] is [latex]0.9999833333[\/latex], and so forth. Using this table of values, it appears that a good estimate is [latex]v(0)=1[\/latex].<\/p>\r\n<p id=\"fs-id1169739298311\">By using the definition of a derivative, we can see that<\/p>\r\n<div id=\"fs-id1169739302610\" class=\"equation unnumbered\">[latex]v(0)=s^{\\prime}(0)=\\underset{t\\to 0}{\\lim}\\dfrac{\\sin t- \\sin 0}{t-0}=\\underset{t\\to 0}{\\lim}\\dfrac{\\sin t}{t}=1[\/latex].<\/div>\r\n<p id=\"fs-id1169739111046\">Thus, in fact, [latex]v(0)=1[\/latex].<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<p id=\"fs-id1169739305376\">As we have seen throughout this section, the slope of a tangent line to a function and instantaneous velocity are related concepts. Each is calculated by computing a derivative and each measures the <strong>instantaneous rate of change<\/strong> of a function, or the rate of change of a function at any point along the function.<\/p>\r\n<section class=\"textbox keyTakeaway\">\r\n<h3 style=\"text-align: left;\">instantaneous rate of change<\/h3>\r\n<p>The<strong> instantaneous rate of change<\/strong> of a function [latex]f(x)[\/latex] at a value [latex]a[\/latex] is its derivative [latex]f^{\\prime}(a)[\/latex].<\/p>\r\n<\/section>\r\n<section class=\"textbox example\">\r\n<p id=\"fs-id1169739187352\">A homeowner sets the thermostat so that the temperature in the house begins to drop from [latex]70^{\\circ}\\text{F}[\/latex] at 9 p.m., reaches a low of [latex]60^{\\circ}[\/latex] during the night, and rises back to [latex]70^{\\circ}[\/latex] by 7 a.m. the next morning.<\/p>\r\n<p>Suppose that the temperature in the house is given by [latex]T(t)=0.4t^2-4t+70[\/latex] for [latex]0\\le t\\le 10[\/latex], where [latex]t[\/latex] is the number of hours past 9 p.m. Find the instantaneous rate of change of the temperature at midnight.<\/p>\r\n<p>[reveal-answer q=\"fs-id1169739297924\"]Show Solution[\/reveal-answer]<br \/>\r\n[hidden-answer a=\"fs-id1169739297924\"]<\/p>\r\n<p id=\"fs-id1169739297924\">Since midnight is [latex]3[\/latex] hours past 9 p.m., we want to compute [latex]T^{\\prime }(3)[\/latex]. Refer to the definition of a derivative.<\/p>\r\n<div id=\"fs-id1169739270561\" class=\"equation unnumbered\">[latex]\\begin{array}{lllll}T^{\\prime}(3) &amp; =\\underset{t\\to 3}{\\lim}\\frac{T(t)-T(3)}{t-3} &amp; &amp; &amp; \\text{Apply the definition.} \\\\ &amp; =\\underset{t\\to 3}{\\lim}\\frac{0.4t^2-4t+70-61.6}{t-3} &amp; &amp; &amp; \\begin{array}{l}\\text{Substitute }T(t)=0.4t^2-4t+70 \\, \\text{and} \\\\ T(3)=61.6. \\end{array} \\\\ &amp; =\\underset{t\\to 3}{\\lim}\\frac{0.4t^2-4t+8.4}{t-3} &amp; &amp; &amp; \\text{Simplify.} \\\\ &amp; =\\underset{t\\to 3}{\\lim}\\frac{0.4(t-3)(t-7)}{t-3} &amp; &amp; &amp; =\\underset{t\\to 3}{\\lim}\\frac{0.4(t-3)(t-7)}{t-3} \\\\ &amp; =\\underset{t\\to 3}{\\lim}0.4(t-7) &amp; &amp; &amp; \\text{Cancel.} \\\\ &amp; =-1.6 &amp; &amp; &amp; \\text{Evaluate the limit.} \\end{array}[\/latex]<\/div>\r\n<p id=\"fs-id1169739274032\">The instantaneous rate of change of the temperature at midnight is [latex]-1.6^{\\circ}\\text{F}[\/latex] per hour.<\/p>\r\n<p>[\/hidden-answer]<\/p>\r\n<\/section>\r\n<section class=\"textbox tryIt\">\r\n<p>[ohm_question]162461[\/ohm_question]<\/p>\r\n<\/section>","rendered":"<h2>Velocities and Rates of Change<\/h2>\n<p id=\"fs-id1169739353680\">Now that we can evaluate a derivative, we can apply it to velocity problems. Recall that if [latex]s(t)[\/latex] is the position of an object moving along a coordinate axis, the <span class=\"no-emphasis\">average velocity<\/span> of the object over a time interval [latex][a,t][\/latex] if [latex]t>a[\/latex] or [latex][t,a][\/latex] if [latex]t<a[\/latex] is:<\/p>\n<div id=\"fs-id1169739303202\" class=\"equation\" style=\"text-align: center;\">[latex]v_{\\text{avg}}=\\dfrac{s(t)-s(a)}{t-a}[\/latex]<\/div>\n<p id=\"fs-id1169739189992\">As the values of [latex]t[\/latex] approach [latex]a[\/latex], the values of [latex]v_{\\text{avg}}[\/latex] approach the value we call the <span class=\"no-emphasis\">instantaneous velocity<\/span> at [latex]a[\/latex]. That is, instantaneous velocity at [latex]a[\/latex], denoted [latex]v(a)[\/latex], is given by<\/p>\n<div id=\"fs-id1169739274700\" class=\"equation\" style=\"text-align: center;\">[latex]v(a)=s^{\\prime}(a)=\\underset{t\\to a}{\\lim}\\dfrac{s(t)-s(a)}{t-a}[\/latex]<\/div>\n<p id=\"fs-id1169739064816\">To better understand the relationship between average velocity and instantaneous velocity, see Figure 7. In this figure, the slope of the tangent line (shown in red) is the instantaneous velocity of the object at time [latex]t=a[\/latex]. The slope of the secant line (shown in green) is the average velocity of the object over the time interval [latex][a,t][\/latex].<\/p>\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\/11205202\/CNX_Calc_Figure_03_01_007.jpg\" alt=\"This figure consists of the Cartesian coordinate plane with 0, a, and t1 marked on the t-axis. The function y = s(t) is graphed in the first quadrant along with two lines marked tangent and secant. The tangent line touches y = s(t) at only one point, (a, s(a)). The secant line touches y = s(t) at two points: (a, s(a)) and (t1, s(t1)).\" width=\"487\" height=\"284\" \/><figcaption class=\"wp-caption-text\">Figure 7. The slope of the secant line is the average velocity over the interval [latex][a,t][\/latex]. The slope of the tangent line is the instantaneous velocity.<\/figcaption><\/figure>\n<p id=\"fs-id1169736619727\">We can use the definitions to calculate the instantaneous velocity, or we can estimate the velocity of a moving object by using a table of values. We can then confirm the estimate by using the difference quotient.<\/p>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739188880\">A lead weight on a spring is oscillating up and down. Its position at time [latex]t[\/latex] with respect to a fixed horizontal line is given by [latex]s(t)= \\sin t[\/latex]. Use a table of values to estimate [latex]v(0)[\/latex]. Check the estimate by using the definition of a derivative.<\/p>\n<figure style=\"width: 325px\" 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\/11205205\/CNX_Calc_Figure_03_01_010.jpg\" alt=\"A picture of a spring hanging down with a weight at the end. There is a horizontal dashed line marked 0 a little bit above the weight.\" width=\"325\" height=\"192\" \/><figcaption class=\"wp-caption-text\">Figure 8. A lead weight suspended from a spring in vertical oscillatory motion.<\/figcaption><\/figure>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169738960040\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169738960040\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169738960040\">We can estimate the instantaneous velocity at [latex]t=0[\/latex] by computing a table of average velocities using values of [latex]t[\/latex] approaching [latex]0[\/latex], as shown in the table below.<\/p>\n<table id=\"fs-id1169739242675\" summary=\"This table has seven rows and two columns. The first row is a header row and it labels each column. The first column header is x and the second column is (sin t - sin 0)\/(t \u2212 0) = (sin t)\/t. Under the first column are the values -0.1, -0.01, -0.001, 0.001, 0.01, and 0.1. Under the second column are the values 0.998334166, 0.9999833333, 0.999999833, 0.999999833, 0.9999833333, and 0.998334166.\">\n<caption>Average velocities using values of [latex]t[\/latex] approaching [latex]0[\/latex]<\/caption>\n<thead>\n<tr valign=\"top\">\n<th>[latex]t[\/latex]<\/th>\n<th>[latex]\\frac{\\sin t - \\sin 0}{t-0}=\\frac{\\sin t}{t}[\/latex]<\/th>\n<\/tr>\n<\/thead>\n<tbody>\n<tr>\n<td>[latex]-0.1[\/latex]<\/td>\n<td>[latex]0.998334166[\/latex]<\/td>\n<\/tr>\n<tr>\n<td>[latex]-0.01[\/latex]<\/td>\n<td>[latex]0.9999833333[\/latex]<\/td>\n<\/tr>\n<tr>\n<td>[latex]-0.001[\/latex]<\/td>\n<td>[latex]0.999999833[\/latex]<\/td>\n<\/tr>\n<tr>\n<td>[latex]0.001[\/latex]<\/td>\n<td>[latex]0.999999833[\/latex]<\/td>\n<\/tr>\n<tr>\n<td>[latex]0.01[\/latex]<\/td>\n<td>[latex]0.9999833333[\/latex]<\/td>\n<\/tr>\n<tr>\n<td>[latex]0.1[\/latex]<\/td>\n<td>[latex]0.998334166[\/latex]<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p id=\"fs-id1169739188902\">From the table we see that the average velocity over the time interval [latex][-0.1,0][\/latex] is [latex]0.998334166[\/latex], the average velocity over the time interval [latex][-0.01,0][\/latex] is [latex]0.9999833333[\/latex], and so forth. Using this table of values, it appears that a good estimate is [latex]v(0)=1[\/latex].<\/p>\n<p id=\"fs-id1169739298311\">By using the definition of a derivative, we can see that<\/p>\n<div id=\"fs-id1169739302610\" class=\"equation unnumbered\">[latex]v(0)=s^{\\prime}(0)=\\underset{t\\to 0}{\\lim}\\dfrac{\\sin t- \\sin 0}{t-0}=\\underset{t\\to 0}{\\lim}\\dfrac{\\sin t}{t}=1[\/latex].<\/div>\n<p id=\"fs-id1169739111046\">Thus, in fact, [latex]v(0)=1[\/latex].<\/p>\n<\/div>\n<\/div>\n<\/section>\n<p id=\"fs-id1169739305376\">As we have seen throughout this section, the slope of a tangent line to a function and instantaneous velocity are related concepts. Each is calculated by computing a derivative and each measures the <strong>instantaneous rate of change<\/strong> of a function, or the rate of change of a function at any point along the function.<\/p>\n<section class=\"textbox keyTakeaway\">\n<h3 style=\"text-align: left;\">instantaneous rate of change<\/h3>\n<p>The<strong> instantaneous rate of change<\/strong> of a function [latex]f(x)[\/latex] at a value [latex]a[\/latex] is its derivative [latex]f^{\\prime}(a)[\/latex].<\/p>\n<\/section>\n<section class=\"textbox example\">\n<p id=\"fs-id1169739187352\">A homeowner sets the thermostat so that the temperature in the house begins to drop from [latex]70^{\\circ}\\text{F}[\/latex] at 9 p.m., reaches a low of [latex]60^{\\circ}[\/latex] during the night, and rises back to [latex]70^{\\circ}[\/latex] by 7 a.m. the next morning.<\/p>\n<p>Suppose that the temperature in the house is given by [latex]T(t)=0.4t^2-4t+70[\/latex] for [latex]0\\le t\\le 10[\/latex], where [latex]t[\/latex] is the number of hours past 9 p.m. Find the instantaneous rate of change of the temperature at midnight.<\/p>\n<p><div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"qfs-id1169739297924\">Show Solution<\/button><\/p>\n<div id=\"qfs-id1169739297924\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1169739297924\">Since midnight is [latex]3[\/latex] hours past 9 p.m., we want to compute [latex]T^{\\prime }(3)[\/latex]. Refer to the definition of a derivative.<\/p>\n<div id=\"fs-id1169739270561\" class=\"equation unnumbered\">[latex]\\begin{array}{lllll}T^{\\prime}(3) & =\\underset{t\\to 3}{\\lim}\\frac{T(t)-T(3)}{t-3} & & & \\text{Apply the definition.} \\\\ & =\\underset{t\\to 3}{\\lim}\\frac{0.4t^2-4t+70-61.6}{t-3} & & & \\begin{array}{l}\\text{Substitute }T(t)=0.4t^2-4t+70 \\, \\text{and} \\\\ T(3)=61.6. \\end{array} \\\\ & =\\underset{t\\to 3}{\\lim}\\frac{0.4t^2-4t+8.4}{t-3} & & & \\text{Simplify.} \\\\ & =\\underset{t\\to 3}{\\lim}\\frac{0.4(t-3)(t-7)}{t-3} & & & =\\underset{t\\to 3}{\\lim}\\frac{0.4(t-3)(t-7)}{t-3} \\\\ & =\\underset{t\\to 3}{\\lim}0.4(t-7) & & & \\text{Cancel.} \\\\ & =-1.6 & & & \\text{Evaluate the limit.} \\end{array}[\/latex]<\/div>\n<p id=\"fs-id1169739274032\">The instantaneous rate of change of the temperature at midnight is [latex]-1.6^{\\circ}\\text{F}[\/latex] per hour.<\/p>\n<\/div>\n<\/div>\n<\/section>\n<section class=\"textbox tryIt\">\n<iframe loading=\"lazy\" id=\"ohm162461\" class=\"resizable\" src=\"https:\/\/ohm.lumenlearning.com\/multiembedq.php?id=162461&theme=lumen&iframe_resize_id=ohm162461&source=tnh&show_question_numbers\" width=\"100%\" height=\"150\"><\/iframe><br \/>\n<\/section>\n","protected":false},"author":6,"menu_order":7,"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\":\"3.1 Defining the Derivative\",\"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":"3.1 Defining the Derivative","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\/231"}],"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\/231\/revisions"}],"predecessor-version":[{"id":2839,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapters\/231\/revisions\/2839"}],"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\/231\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/media?parent=231"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/pressbooks\/v2\/chapter-type?post=231"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/contributor?post=231"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/content.one.lumenlearning.com\/calculus1\/wp-json\/wp\/v2\/license?post=231"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}