{"id":5,"date":"2021-12-11T11:32:52","date_gmt":"2021-12-11T16:32:52","guid":{"rendered":"https:\/\/pressbooks.library.ryerson.ca\/multivariatecalculus\/?p=5"},"modified":"2022-03-06T01:48:38","modified_gmt":"2022-03-06T06:48:38","slug":"chapter-1","status":"publish","type":"chapter","link":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/chapter\/chapter-1\/","title":{"raw":"Unit 1: Partial Derivatives","rendered":"Unit 1: Partial Derivatives"},"content":{"raw":"<h2>The Concept<\/h2>\r\nWhen studying derivatives of functions of one variable [latex]y=f(x)[\/latex], we found that one interpretation of the derivative is an instantaneous rate of change of [latex]y[\/latex] as a function of [latex]x[\/latex]. Leibniz notation for the derivative is [latex]\\frac{dy}{dx}[\/latex], which implies that [latex]y[\/latex] is the dependent variable and [latex]x[\/latex] is the independent variable. [latex]\\frac{dy}{dx}[\/latex] also represents the slope of the tangent line at a certain point of this function.\r\n\r\nFor a function [latex]z=f(x,y)[\/latex] of two variables, [latex]x[\/latex] and [latex]y[\/latex] are the independent variables (input to function [latex]f[\/latex]) and [latex]z[\/latex] is the dependent variable (output of function [latex]z[\/latex], the value of [latex]z[\/latex] is depend on the values of [latex]x[\/latex] and [latex]y[\/latex] ). We will have two partial derivatives and their Leibniz notations are [latex]\\frac{\\partial z}{\\partial x}[\/latex], and [latex]\\frac{\\partial z}{\\partial y}[\/latex]. They are analogous to ordinary derivatives:\r\n<p style=\"padding-left: 40px\">[latex]\\frac{\\partial z}{\\partial x}(x_0, y_0)=\\frac{\\text{change in } z}{\\text{change in }x}(\\text{holding }y \\text{ as a constant } y_0)[\/latex]<\/p>\r\n<p style=\"padding-left: 40px\">[latex]\\frac{\\partial z}{\\partial y}(x_0, y_0)=\\frac{\\text{change in } z}{\\text{change in }y}(\\text{holding }x \\text{ as a constant } x_0)[\/latex]<\/p>\r\nBesides the Leibniz notations above, you can also write the derivatives as [latex]\\frac{\\partial z}{\\partial x}=f_x[\/latex] and [latex]\\frac{\\partial z}{\\partial y}=f_y[\/latex]. Similar to the geometric meaning of [latex]\\frac{dy}{dx}[\/latex] in two-dimensional (2D), [latex]\\frac{\\partial z}{\\partial x}[\/latex] and [latex]\\frac{\\partial z}{\\partial y}[\/latex] in three-dimensional (3D) represent the slopes of tangent lines as well.\r\n<h2>The Plot<\/h2>\r\nNow, you should engage with the 3D plot below for partial derivatives[footnote]Made with GeoGebra, licensed Creative Commons CC BY-NC-SA 4.0.[\/footnote]. Follow the steps below to apply changes to the plot and observe the effects:\r\n<ol>\r\n \t<li>Input a function of two variables, then set [latex]y[\/latex] as a constant, e.g., [latex]-1[\/latex]. A cross-section plane [latex]y=-1[\/latex] is plotted. Recall that the function [latex]y = y_0[\/latex] (or [latex]x=x_0[\/latex]) in 3D represents the planes that are perpendicular to the <em>[latex]xy[\/latex]<\/em>-plane.<\/li>\r\n \t<li>A tangent line passing through the point ([latex]x_0[\/latex], [latex]y_0[\/latex]) and also on the cross-section plane [latex]y=y_0[\/latex] is plotted. Change the [latex]y[\/latex]-values using the slider, and you will see the cross-section and the tangent line changes. You can also rotate the graph to get a better view. Since the particle derivative is the slope of the tangent line, the partial derivative [latex]\\frac{\\partial z}{\\partial x}[\/latex] changes as well.<\/li>\r\n \t<li>Repeat the same steps in (1) and (2) for [latex]\\frac{\\partial z}{\\partial y}[\/latex].<\/li>\r\n<\/ol>\r\n<span>[h5p id=\"2\"]<\/span>\r\n<div class=\"textbox textbox--exercises\"><header class=\"textbox__header\">\r\n<h2 class=\"textbox__title\">Self-Checking Questions<\/h2>\r\n<\/header>\r\n<div class=\"textbox__content\">\r\n\r\nCheck your understanding by solving the following questions<span>[footnote]Gilbert Strang, Edwin \u201cJed\u201d Herman,\u00a0 OpenStax,\u00a0Calculus Volume 3,\u00a0 Calculus Volumes 1, 2, and 3 are licensed under an Attribution-NonCommercial-Sharealike 4.0 International License (CC BY-NC-SA).[\/footnote]<\/span>:\r\n<ol>\r\n \t<li>Let [latex]f(x,y)=\\frac{xy}{x-y}[\/latex]. Find [latex]f_x(2,-2)[\/latex] and [latex]f_y(2,-2)[\/latex].<\/li>\r\n \t<li>The apparent temperature index, [latex]A[\/latex], is a measure of how the temperature feels,<\/li>\r\n<\/ol>\r\n<p style=\"text-align: center\">[latex]A=0.885x -22.4 y +1.2 xy -0.544[\/latex]<\/p>\r\n<p style=\"padding-left: 40px\">where [latex]x[\/latex] is relative humidity and [latex]y[\/latex] is the air temperature. Find [latex]\\frac{\\partial A}{\\partial x}[\/latex] and [latex]\\frac{\\partial A}{\\partial y}[\/latex] when [latex]x=20\u00b0F[\/latex] and [latex]y=1[\/latex].<\/p>\r\n<span>[h5p id=\"7\"]<\/span><span style=\"color: #000000\"><\/span>\r\n\r\n<\/div>\r\n<\/div>\r\n&nbsp;","rendered":"<h2>The Concept<\/h2>\n<p>When studying derivatives of functions of one variable [latex]y=f(x)[\/latex], we found that one interpretation of the derivative is an instantaneous rate of change of [latex]y[\/latex] as a function of [latex]x[\/latex]. Leibniz notation for the derivative is [latex]\\frac{dy}{dx}[\/latex], which implies that [latex]y[\/latex] is the dependent variable and [latex]x[\/latex] is the independent variable. [latex]\\frac{dy}{dx}[\/latex] also represents the slope of the tangent line at a certain point of this function.<\/p>\n<p>For a function [latex]z=f(x,y)[\/latex] of two variables, [latex]x[\/latex] and [latex]y[\/latex] are the independent variables (input to function [latex]f[\/latex]) and [latex]z[\/latex] is the dependent variable (output of function [latex]z[\/latex], the value of [latex]z[\/latex] is depend on the values of [latex]x[\/latex] and [latex]y[\/latex] ). We will have two partial derivatives and their Leibniz notations are [latex]\\frac{\\partial z}{\\partial x}[\/latex], and [latex]\\frac{\\partial z}{\\partial y}[\/latex]. They are analogous to ordinary derivatives:<\/p>\n<p style=\"padding-left: 40px\">[latex]\\frac{\\partial z}{\\partial x}(x_0, y_0)=\\frac{\\text{change in } z}{\\text{change in }x}(\\text{holding }y \\text{ as a constant } y_0)[\/latex]<\/p>\n<p style=\"padding-left: 40px\">[latex]\\frac{\\partial z}{\\partial y}(x_0, y_0)=\\frac{\\text{change in } z}{\\text{change in }y}(\\text{holding }x \\text{ as a constant } x_0)[\/latex]<\/p>\n<p>Besides the Leibniz notations above, you can also write the derivatives as [latex]\\frac{\\partial z}{\\partial x}=f_x[\/latex] and [latex]\\frac{\\partial z}{\\partial y}=f_y[\/latex]. Similar to the geometric meaning of [latex]\\frac{dy}{dx}[\/latex] in two-dimensional (2D), [latex]\\frac{\\partial z}{\\partial x}[\/latex] and [latex]\\frac{\\partial z}{\\partial y}[\/latex] in three-dimensional (3D) represent the slopes of tangent lines as well.<\/p>\n<h2>The Plot<\/h2>\n<p>Now, you should engage with the 3D plot below for partial derivatives<a class=\"footnote\" title=\"Made with GeoGebra, licensed Creative Commons CC BY-NC-SA 4.0.\" id=\"return-footnote-5-1\" href=\"#footnote-5-1\" aria-label=\"Footnote 1\"><sup class=\"footnote\">[1]<\/sup><\/a>. Follow the steps below to apply changes to the plot and observe the effects:<\/p>\n<ol>\n<li>Input a function of two variables, then set [latex]y[\/latex] as a constant, e.g., [latex]-1[\/latex]. A cross-section plane [latex]y=-1[\/latex] is plotted. Recall that the function [latex]y = y_0[\/latex] (or [latex]x=x_0[\/latex]) in 3D represents the planes that are perpendicular to the <em>[latex]xy[\/latex]<\/em>-plane.<\/li>\n<li>A tangent line passing through the point ([latex]x_0[\/latex], [latex]y_0[\/latex]) and also on the cross-section plane [latex]y=y_0[\/latex] is plotted. Change the [latex]y[\/latex]-values using the slider, and you will see the cross-section and the tangent line changes. You can also rotate the graph to get a better view. Since the particle derivative is the slope of the tangent line, the partial derivative [latex]\\frac{\\partial z}{\\partial x}[\/latex] changes as well.<\/li>\n<li>Repeat the same steps in (1) and (2) for [latex]\\frac{\\partial z}{\\partial y}[\/latex].<\/li>\n<\/ol>\n<p><span><\/p>\n<div id=\"h5p-2\">\n<div class=\"h5p-content\" data-content-id=\"2\"><\/div>\n<\/div>\n<p><\/span><\/p>\n<div class=\"textbox textbox--exercises\">\n<header class=\"textbox__header\">\n<h2 class=\"textbox__title\">Self-Checking Questions<\/h2>\n<\/header>\n<div class=\"textbox__content\">\n<p>Check your understanding by solving the following questions<span><a class=\"footnote\" title=\"Gilbert Strang, Edwin \u201cJed\u201d Herman,\u00a0 OpenStax,\u00a0Calculus Volume 3,\u00a0 Calculus Volumes 1, 2, and 3 are licensed under an Attribution-NonCommercial-Sharealike 4.0 International License (CC BY-NC-SA).\" id=\"return-footnote-5-2\" href=\"#footnote-5-2\" aria-label=\"Footnote 2\"><sup class=\"footnote\">[2]<\/sup><\/a><\/span>:<\/p>\n<ol>\n<li>Let [latex]f(x,y)=\\frac{xy}{x-y}[\/latex]. Find [latex]f_x(2,-2)[\/latex] and [latex]f_y(2,-2)[\/latex].<\/li>\n<li>The apparent temperature index, [latex]A[\/latex], is a measure of how the temperature feels,<\/li>\n<\/ol>\n<p style=\"text-align: center\">[latex]A=0.885x -22.4 y +1.2 xy -0.544[\/latex]<\/p>\n<p style=\"padding-left: 40px\">where [latex]x[\/latex] is relative humidity and [latex]y[\/latex] is the air temperature. Find [latex]\\frac{\\partial A}{\\partial x}[\/latex] and [latex]\\frac{\\partial A}{\\partial y}[\/latex] when [latex]x=20\u00b0F[\/latex] and [latex]y=1[\/latex].<\/p>\n<p><span><\/p>\n<div id=\"h5p-7\">\n<div class=\"h5p-iframe-wrapper\"><iframe id=\"h5p-iframe-7\" class=\"h5p-iframe\" data-content-id=\"7\" style=\"height:1px\" src=\"about:blank\" frameBorder=\"0\" scrolling=\"no\" title=\"Unit 1. Self-Checking Questions\"><\/iframe><\/div>\n<\/div>\n<p><\/span><span style=\"color: #000000\"><\/span><\/p>\n<\/div>\n<\/div>\n<p>&nbsp;<\/p>\n<hr class=\"before-footnotes clear\" \/><div class=\"footnotes\"><ol><li id=\"footnote-5-1\">Made with GeoGebra, licensed Creative Commons CC BY-NC-SA 4.0. <a href=\"#return-footnote-5-1\" class=\"return-footnote\" aria-label=\"Return to footnote 1\">&crarr;<\/a><\/li><li id=\"footnote-5-2\">Gilbert Strang, Edwin \u201cJed\u201d Herman,\u00a0 OpenStax,\u00a0Calculus Volume 3,\u00a0 Calculus Volumes 1, 2, and 3 are licensed under an Attribution-NonCommercial-Sharealike 4.0 International License (CC BY-NC-SA). <a href=\"#return-footnote-5-2\" class=\"return-footnote\" aria-label=\"Return to footnote 2\">&crarr;<\/a><\/li><\/ol><\/div>","protected":false},"author":178,"menu_order":1,"template":"","meta":{"pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[48],"contributor":[],"license":[],"class_list":["post-5","chapter","type-chapter","status-publish","hentry","chapter-type-standard"],"part":3,"_links":{"self":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapters\/5","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/wp\/v2\/users\/178"}],"version-history":[{"count":66,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapters\/5\/revisions"}],"predecessor-version":[{"id":561,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapters\/5\/revisions\/561"}],"part":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/parts\/3"}],"metadata":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapters\/5\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/wp\/v2\/media?parent=5"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/pressbooks\/v2\/chapter-type?post=5"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/wp\/v2\/contributor?post=5"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/pressbooks.library.torontomu.ca\/multivariatecalculus\/wp-json\/wp\/v2\/license?post=5"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}