{"id":1125,"date":"2021-11-09T23:42:35","date_gmt":"2021-11-09T23:42:35","guid":{"rendered":"https:\/\/courses.lumenlearning.com\/calculus3\/?post_type=chapter&#038;p=1125"},"modified":"2022-11-01T05:27:08","modified_gmt":"2022-11-01T05:27:08","slug":"using-divergence-and-curl","status":"publish","type":"chapter","link":"https:\/\/courses.lumenlearning.com\/calculus3\/chapter\/using-divergence-and-curl\/","title":{"raw":"Using Divergence and Curl","rendered":"Using Divergence and Curl"},"content":{"raw":"<div data-type=\"note\">\r\n<div class=\"textbox learning-objectives\">\r\n<h3>Learning Objectives<\/h3>\r\n<ul class=\"os-abstract\">\r\n \t<li><span class=\"os-abstract-content\">Use the properties of curl and divergence to determine whether a vector field is conservative.<\/span><\/li>\r\n<\/ul>\r\n<\/div>\r\n<p id=\"fs-id1167794054131\">Now that we understand the basic concepts of divergence and curl, we can discuss their properties and establish relationships between them and conservative vector fields.<\/p>\r\n\r\n<\/div>\r\n<div data-type=\"note\">If\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a vector field in [latex]\\mathbb{R}^3[\/latex], then the curl of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is also a vector field in [latex]\\mathbb{R}^3[\/latex]. Therefore, we can take the divergence of a curl. The next theorem says that the result is always zero. This result is useful because it gives us a way to show that some vector fields are not the curl of any other field. To give this result a physical interpretation, recall that divergence of a velocity field\u00a0[latex]{\\bf{v}}[\/latex]\u00a0at point [latex]P[\/latex] measures the tendency of the corresponding fluid to flow out of [latex]P[\/latex]. Since [latex]\\text{div curl }({\\bf{v}})=0[\/latex], the net rate of flow in vector field curl([latex]{\\bf{v}}[\/latex]) at any point is zero. Taking the curl of vector field\u00a0[latex]{\\bf{F}}[\/latex]\u00a0eliminates whatever divergence was present in\u00a0[latex]{\\bf{F}}[\/latex].<\/div>\r\n<div data-type=\"note\"><\/div>\r\n<div data-type=\"note\">\r\n<div class=\"textbox shaded\">\r\n<h3 style=\"text-align: center;\">Theorem: divergence of the curl<\/h3>\r\n\r\n<hr \/>\r\n\r\nLet [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] be a vector field in [latex]\\mathbb{R}^3[\/latex] such that the component functions all have continuous second-order partial derivatives. Then, [latex]\\text{div curl }({\\bf{F}})=\\nabla\\cdot(\\nabla\\times{\\bf{F}})=0[\/latex].\r\n\r\n<\/div>\r\n<h3 data-type=\"title\">Proof<\/h3>\r\n<p id=\"fs-id1167793355188\">By the definitions of divergence and curl, and by Clairaut\u2019s theorem,<\/p>\r\n<p style=\"text-align: center;\">[latex]\\large{\\begin{aligned}\r\n\\text{div curl }({\\bf{F}})&amp;=\\text{div }[(R_y-Q_z){\\bf{i}}+(P_z-R_x){\\bf{j}}+(Q_x-P_y){\\bf{k}}] \\\\&amp;=R_{yx}-Q_{xz}+P_{yz}-R_{yx}+Q_{zx}-P_{zy} \\\\\r\n&amp;=0\r\n\\end{aligned}}[\/latex].<\/p>\r\n[latex]_\\blacksquare[\/latex]\r\n\r\n<\/div>\r\n<div data-type=\"note\">\r\n<div class=\"textbox exercises\">\r\n<h3>Example: showing that a vector field is not the curl of another<\/h3>\r\nShow that [latex]{\\bf{F}}(x,y,z)=e^x{\\bf{i}}+yz{\\bf{j}}+xz^2{\\bf{k}}[\/latex] is not the curl of another vector field. That is, show that there is no other vector\u00a0[latex]{\\bf{G}}[\/latex]\u00a0with curl [latex]{\\bf{G}}={\\bf{F}}[\/latex].\r\n\r\n[reveal-answer q=\"748329916\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"748329916\"]\r\n<p id=\"fs-id1167793553752\">Notice that the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is all of [latex]\\mathbb{R}^3[\/latex] and the second-order partials of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0are all continuous. Therefore, we can apply the previous theorem to\u00a0[latex]{\\bf{F}}[\/latex].<\/p>\r\n<p id=\"fs-id1167793918481\">The divergence of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is [latex]e^x+z+2xz[\/latex]. If\u00a0[latex]{\\bf{F}}[\/latex]\u00a0were the curl of vector field\u00a0[latex]\\bf{G}[\/latex], then [latex]\\text{div }{\\bf{F}}=\\text{div curl }{\\bf{G}}=0[\/latex]. But, the divergence of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is not zero, and therefore\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is not the curl of any other vector field.<\/p>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<div class=\"textbox key-takeaways\">\r\n<h3>try it<\/h3>\r\nIs it possible for [latex]{\\bf{G}}(x,y,z)=\\langle\\sin{x},\\cos{y},\\sin{(x,y,z)}\\rangle[\/latex] to be the curl of a vector field?\r\n\r\n[reveal-answer q=\"679340216\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"679340216\"]\r\n\r\nNo.\r\n\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<\/div>\r\n\r\n[caption]Watch the following video to see the worked solution to the above Try It[\/caption]\r\n\r\n<center><iframe src=\"\/\/plugin.3playmedia.com\/show?mf=8250325&amp;p3sdk_version=1.10.1&amp;p=20361&amp;pt=375&amp;video_id=3Lpc9ylxjtw&amp;video_target=tpm-plugin-zu9cpf88-3Lpc9ylxjtw\" width=\"800px\" height=\"450px\" frameborder=\"0\" marginwidth=\"0px\" marginheight=\"0px\"><\/iframe><\/center><center>You can view the <a href=\"https:\/\/course-building.s3.us-west-2.amazonaws.com\/Calculus+3\/Calc+3+transcripts\/CP6.45_transcript.html\">transcript for \u201cCP 6.45\u201d here (opens in new window).<\/a><\/center>\r\n<p id=\"fs-id1167793977413\">With the next two theorems, we show that if\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a conservative vector field then its curl is zero, and if the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is simply connected then the converse is also true. This gives us another way to test whether a vector field is conservative.<\/p>\r\n\r\n<div class=\"textbox shaded\">\r\n<h3 style=\"text-align: center;\">theorem: curl of a conservative vector field<\/h3>\r\n\r\n<hr \/>\r\n\r\nIf [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] is conservative, then [latex] \\text{curl } \\bf{F}=\\bf{0} [\/latex]<span class=\"os-math-in-para\"><span id=\"MathJax-Element-116-Frame\" class=\"MathJax\" style=\"box-sizing: border-box; overflow: initial; display: inline-table; font-style: normal; font-weight: normal; line-height: normal; font-size: 16px; text-indent: 0px; text-align: left; text-transform: none; letter-spacing: normal; word-spacing: normal; overflow-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; padding: 0px; margin: 0px; position: relative;\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; display=&quot;inline&quot;&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mtext&gt;curl&lt;\/mtext&gt;&lt;mspace width=&quot;0.2em&quot; \/&gt;&lt;mstyle mathvariant=&quot;bold&quot; mathsize=&quot;normal&quot;&gt;&lt;mtext&gt;F&lt;\/mtext&gt;&lt;\/mstyle&gt;&lt;mo&gt;=&lt;\/mo&gt;&lt;mn&gt;0&lt;\/mn&gt;&lt;mo&gt;.&lt;\/mo&gt;&lt;\/mrow&gt;&lt;\/mrow&gt;&lt;annotation-xml encoding=&quot;MathML-Content&quot;&gt;&lt;mrow&gt;&lt;mtext&gt;curl&lt;\/mtext&gt;&lt;mspace width=&quot;0.2em&quot;&gt;&lt;\/mspace&gt;&lt;mstyle mathvariant=&quot;bold&quot; mathsize=&quot;normal&quot;&gt;&lt;mtext&gt;F&lt;\/mtext&gt;&lt;\/mstyle&gt;&lt;mo&gt;=&lt;\/mo&gt;&lt;mn&gt;0&lt;\/mn&gt;&lt;mo&gt;.&lt;\/mo&gt;&lt;\/mrow&gt;&lt;\/annotation-xml&gt;&lt;\/semantics&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-3195\" class=\"math\"><span id=\"MathJax-Span-3196\" class=\"mrow\"><span id=\"MathJax-Span-3197\" class=\"semantics\"><span id=\"MathJax-Span-3198\" class=\"mrow\"><span id=\"MathJax-Span-3199\" class=\"mrow\"><span id=\"MathJax-Span-3200\" class=\"mtext\">.\u00a0<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span>\r\n\r\n<\/div>\r\n<h3 data-type=\"title\">Proof<\/h3>\r\n<p id=\"fs-id1167793445753\">Since conservative vector fields satisfy the cross-partials property, all the cross-partials of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0are equal. Therefore,<\/p>\r\n<p style=\"text-align: center;\">[latex]\\large{\\begin{aligned}\r\n\\text{curl }{\\bf{F}}&amp;=(R_y-Q_z){\\bf{i}}+(P_z-R_x){\\bf{j}}+(Q_x-P_y){\\bf{k}} \\\\\r\n&amp;=0\r\n\\end{aligned}}[\/latex].<\/p>\r\n[latex]_\\blacksquare[\/latex]\r\n\r\nThe same theorem is true for vector fields in a plane.\r\n<div id=\"fs-id1167793524959\" class=\"unnumbered\" data-type=\"equation\" data-label=\"\"><\/div>\r\n<p id=\"fs-id1167794121468\">Since a conservative vector field is the gradient of a scalar function, the previous theorem says that [latex]\\text{curl }(\\nabla{f})=0[\/latex] for any scalar function [latex]f[\/latex]. In terms of our curl notation, [latex]\\nabla\\times\\nabla{(f)}=0[\/latex]. This equation makes sense because the cross product of a vector with itself is always the zero vector. Sometimes equation [latex]\\nabla\\times\\nabla{(f)}=0[\/latex] is simplified as [latex]\\nabla\\times\\nabla=0[\/latex].<\/p>\r\n\r\n<div id=\"fs-id1167793495816\" class=\"theorem ui-has-child-title\" data-type=\"note\">\r\n<div class=\"textbox shaded\">\r\n<h3 style=\"text-align: center;\">theorem: curl test for a conservative field<\/h3>\r\n\r\n<hr \/>\r\n\r\nLet [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] be a vector field in space on a simply connected domain. If [latex]\\text{curl }{\\bf{F}}=0[\/latex], then\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.\r\n\r\n<\/div>\r\n<h3 data-type=\"title\">Proof<\/h3>\r\n<p id=\"fs-id1167793355840\">Since [latex]\\text{curl }{\\bf{F}}=0[\/latex], we have that [latex]R_y=Q_z[\/latex],\u00a0[latex]P_z=R_x[\/latex], and\u00a0[latex]Q_x=P_y[\/latex]. Therefore,\u00a0[latex]{\\bf{F}}[\/latex]\u00a0satisfies the cross-partials property on a simply connected domain, and\u00a0Cross-Partial Property of Conservative Fields Theorem\u00a0implies that\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.<\/p>\r\n[latex]_\\blacksquare[\/latex]\r\n<p id=\"fs-id1167793498800\">The same theorem is also true in a plane. Therefore, if\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a vector field in a plane or in space and the domain is simply connected, then\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative if and only if [latex]\\text{curl }{\\bf{F}}=0[\/latex].<\/p>\r\n\r\n<\/div>\r\n<div data-type=\"note\">\r\n<div class=\"textbox exercises\">\r\n<h3>Example: testing whether a vector field is conservative<\/h3>\r\nUse the curl to determine whether [latex]{\\bf{F}}(x,y,z)=\\langle{y}z,xz,xy\\rangle[\/latex] is conservative.\r\n\r\n[reveal-answer q=\"478259405\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"478259405\"]\r\n\r\nNote that the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is all of [latex]\\mathbb{R}^3[\/latex], which is simply connected (Figure 1). Therefore, we can test whether\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative by calculating its curl.\r\n\r\n[caption id=\"attachment_5333\" align=\"aligncenter\" width=\"382\"]<img class=\"size-full wp-image-5333\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/31234154\/6.56.jpg\" alt=\"&lt;img src=&quot;\/apps\/archive\/20220422.171947\/resources\/7749bed210536f0229f8267b69c34794d0305459&quot; data-media-type=&quot;image\/jpeg&quot; alt=&quot;A diagram showing the curl of a vector field in two dimensions. The curl is zero. The arrows seem to be pointing up and over into the yz plane.&quot; id=&quot;30&quot;&gt;\" width=\"382\" height=\"398\" \/> Figure 1. The curl of vector field [latex]{\\bf{F}}(x,y,z)=\\langle{y}z,xz,xy\\rangle[\/latex] is zero.[\/caption]\r\n<p id=\"fs-id1167794023727\">The curl of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is<\/p>\r\n<p style=\"text-align: center;\">[latex]\\left(\\frac{\\partial}{\\partial{y}}xy-\\frac{\\partial}{\\partial{z}}xz\\right){\\bf{i}}+\\left(\\frac{\\partial}{\\partial{y}}yz-\\frac{\\partial}{\\partial{z}}xy\\right){\\bf{j}}+\\left(\\frac{\\partial}{\\partial{y}}xz-\\frac{\\partial}{\\partial{z}}yz\\right){\\bf{k}}=(x-x){\\bf{i}}+(y-y){\\bf{j}}+(z-z){\\bf{k}}=0[\/latex].<\/p>\r\n<p id=\"fs-id1167794054301\">Thus,\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.<\/p>\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<p id=\"fs-id1167793562322\">We have seen that the curl of a gradient is zero. What is the divergence of a gradient? If [latex]f[\/latex] is a function of two variables, then [latex]\\text{div }(\\nabla{f})=\\nabla\\cdot(\\nabla{f})=f_{xx}+f_{yy}[\/latex]. We abbreviate this \u201cdouble dot product\u201d as [latex]\\nabla^2[\/latex]. This operator is called the\u00a0<span id=\"6f668e5d-300d-4e6c-aec3-70b59f71fe69_term268\" class=\"no-emphasis\" data-type=\"term\"><em data-effect=\"italics\">Laplace operator<\/em><\/span><em data-effect=\"italics\">,<\/em>\u00a0and in this notation Laplace\u2019s equation becomes [latex]\\nabla^2f=0[\/latex]. Therefore, a harmonic function is a function that becomes zero after taking the divergence of a gradient.<\/p>\r\n<p id=\"fs-id1167794018031\">Similarly, if [latex]f[\/latex] is a function of three variables then<\/p>\r\n<p style=\"text-align: center;\">[latex]\\large{\\text{div }(\\nabla{f})=\\nabla\\cdot(\\nabla{f})=f_{xx}+f_{yy}+f_{zz}}[\/latex].<\/p>\r\n<p id=\"fs-id1167793619900\">Using this notation we get Laplace\u2019s equation for harmonic functions of three variables:<\/p>\r\n<p style=\"text-align: center;\">[latex]\\large{\\nabla^2f=0}[\/latex].<\/p>\r\n<p id=\"fs-id1167793829624\">Harmonic functions arise in many applications. For example, the potential function of an electrostatic field in a region of space that has no static charge is harmonic.<\/p>\r\n\r\n<\/div>\r\n<div class=\"textbox exercises\">\r\n<h3>Example: analyzing a function<\/h3>\r\nIs it possible for [latex]f(x, y)=x^{2}+x-y[\/latex] to be the potential function of an electrostatic field that is located in a region of [latex]\\mathbb{R}^2[\/latex] free of static charge?\r\n\r\n[reveal-answer q=\"783691260\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"783691260\"]\r\n\r\nIf [latex]f[\/latex] were such a potential function, then [latex]f[\/latex] would be harmonic. Note that [latex]f_{xx}=2[\/latex], and [latex]f_{yy}=0[\/latex], so [latex]f_{xx}+f_{yy}\\ne0[\/latex]. Therefore, [latex]f[\/latex] is not harmonic and [latex]f[\/latex] cannot represent an electrostatic potential.\r\n\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<div class=\"textbox key-takeaways\">\r\n<h3>try it<\/h3>\r\nIs it possible for function [latex]f(x, y)=x^{2}-y^{2}+x[\/latex] to be the potential function of an electrostatic field located in a region of [latex]\\mathbb{R}^2[\/latex] free of static charge?\r\n\r\n[reveal-answer q=\"746189149\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"746189149\"]\r\n\r\nYes.\r\n\r\n[\/hidden-answer]\r\n\r\n<\/div>\r\n<div data-type=\"note\"><\/div>","rendered":"<div data-type=\"note\">\n<div class=\"textbox learning-objectives\">\n<h3>Learning Objectives<\/h3>\n<ul class=\"os-abstract\">\n<li><span class=\"os-abstract-content\">Use the properties of curl and divergence to determine whether a vector field is conservative.<\/span><\/li>\n<\/ul>\n<\/div>\n<p id=\"fs-id1167794054131\">Now that we understand the basic concepts of divergence and curl, we can discuss their properties and establish relationships between them and conservative vector fields.<\/p>\n<\/div>\n<div data-type=\"note\">If\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a vector field in [latex]\\mathbb{R}^3[\/latex], then the curl of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is also a vector field in [latex]\\mathbb{R}^3[\/latex]. Therefore, we can take the divergence of a curl. The next theorem says that the result is always zero. This result is useful because it gives us a way to show that some vector fields are not the curl of any other field. To give this result a physical interpretation, recall that divergence of a velocity field\u00a0[latex]{\\bf{v}}[\/latex]\u00a0at point [latex]P[\/latex] measures the tendency of the corresponding fluid to flow out of [latex]P[\/latex]. Since [latex]\\text{div curl }({\\bf{v}})=0[\/latex], the net rate of flow in vector field curl([latex]{\\bf{v}}[\/latex]) at any point is zero. Taking the curl of vector field\u00a0[latex]{\\bf{F}}[\/latex]\u00a0eliminates whatever divergence was present in\u00a0[latex]{\\bf{F}}[\/latex].<\/div>\n<div data-type=\"note\"><\/div>\n<div data-type=\"note\">\n<div class=\"textbox shaded\">\n<h3 style=\"text-align: center;\">Theorem: divergence of the curl<\/h3>\n<hr \/>\n<p>Let [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] be a vector field in [latex]\\mathbb{R}^3[\/latex] such that the component functions all have continuous second-order partial derivatives. Then, [latex]\\text{div curl }({\\bf{F}})=\\nabla\\cdot(\\nabla\\times{\\bf{F}})=0[\/latex].<\/p>\n<\/div>\n<h3 data-type=\"title\">Proof<\/h3>\n<p id=\"fs-id1167793355188\">By the definitions of divergence and curl, and by Clairaut\u2019s theorem,<\/p>\n<p style=\"text-align: center;\">[latex]\\large{\\begin{aligned}  \\text{div curl }({\\bf{F}})&=\\text{div }[(R_y-Q_z){\\bf{i}}+(P_z-R_x){\\bf{j}}+(Q_x-P_y){\\bf{k}}] \\\\&=R_{yx}-Q_{xz}+P_{yz}-R_{yx}+Q_{zx}-P_{zy} \\\\  &=0  \\end{aligned}}[\/latex].<\/p>\n<p>[latex]_\\blacksquare[\/latex]<\/p>\n<\/div>\n<div data-type=\"note\">\n<div class=\"textbox exercises\">\n<h3>Example: showing that a vector field is not the curl of another<\/h3>\n<p>Show that [latex]{\\bf{F}}(x,y,z)=e^x{\\bf{i}}+yz{\\bf{j}}+xz^2{\\bf{k}}[\/latex] is not the curl of another vector field. That is, show that there is no other vector\u00a0[latex]{\\bf{G}}[\/latex]\u00a0with curl [latex]{\\bf{G}}={\\bf{F}}[\/latex].<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><span class=\"show-answer collapsed\" style=\"cursor: pointer\" data-target=\"q748329916\">Show Solution<\/span><\/p>\n<div id=\"q748329916\" class=\"hidden-answer\" style=\"display: none\">\n<p id=\"fs-id1167793553752\">Notice that the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is all of [latex]\\mathbb{R}^3[\/latex] and the second-order partials of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0are all continuous. Therefore, we can apply the previous theorem to\u00a0[latex]{\\bf{F}}[\/latex].<\/p>\n<p id=\"fs-id1167793918481\">The divergence of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is [latex]e^x+z+2xz[\/latex]. If\u00a0[latex]{\\bf{F}}[\/latex]\u00a0were the curl of vector field\u00a0[latex]\\bf{G}[\/latex], then [latex]\\text{div }{\\bf{F}}=\\text{div curl }{\\bf{G}}=0[\/latex]. But, the divergence of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is not zero, and therefore\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is not the curl of any other vector field.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<div class=\"textbox key-takeaways\">\n<h3>try it<\/h3>\n<p>Is it possible for [latex]{\\bf{G}}(x,y,z)=\\langle\\sin{x},\\cos{y},\\sin{(x,y,z)}\\rangle[\/latex] to be the curl of a vector field?<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><span class=\"show-answer collapsed\" style=\"cursor: pointer\" data-target=\"q679340216\">Show Solution<\/span><\/p>\n<div id=\"q679340216\" class=\"hidden-answer\" style=\"display: none\">\n<p>No.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>Watch the following video to see the worked solution to the above Try It<\/p>\n<div style=\"text-align: center;\"><iframe loading=\"lazy\" src=\"\/\/plugin.3playmedia.com\/show?mf=8250325&amp;p3sdk_version=1.10.1&amp;p=20361&amp;pt=375&amp;video_id=3Lpc9ylxjtw&amp;video_target=tpm-plugin-zu9cpf88-3Lpc9ylxjtw\" width=\"800px\" height=\"450px\" frameborder=\"0\" marginwidth=\"0px\" marginheight=\"0px\"><\/iframe><\/div>\n<div style=\"text-align: center;\">You can view the <a href=\"https:\/\/course-building.s3.us-west-2.amazonaws.com\/Calculus+3\/Calc+3+transcripts\/CP6.45_transcript.html\">transcript for \u201cCP 6.45\u201d here (opens in new window).<\/a><\/div>\n<p id=\"fs-id1167793977413\">With the next two theorems, we show that if\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a conservative vector field then its curl is zero, and if the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is simply connected then the converse is also true. This gives us another way to test whether a vector field is conservative.<\/p>\n<div class=\"textbox shaded\">\n<h3 style=\"text-align: center;\">theorem: curl of a conservative vector field<\/h3>\n<hr \/>\n<p>If [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] is conservative, then [latex]\\text{curl } \\bf{F}=\\bf{0}[\/latex]<span class=\"os-math-in-para\"><span id=\"MathJax-Element-116-Frame\" class=\"MathJax\" style=\"box-sizing: border-box; overflow: initial; display: inline-table; font-style: normal; font-weight: normal; line-height: normal; font-size: 16px; text-indent: 0px; text-align: left; text-transform: none; letter-spacing: normal; word-spacing: normal; overflow-wrap: normal; white-space: nowrap; float: none; direction: ltr; max-width: none; max-height: none; min-width: 0px; min-height: 0px; border: 0px; padding: 0px; margin: 0px; position: relative;\" tabindex=\"0\" role=\"presentation\" data-mathml=\"&lt;math xmlns=&quot;http:\/\/www.w3.org\/1998\/Math\/MathML&quot; display=&quot;inline&quot;&gt;&lt;semantics&gt;&lt;mrow&gt;&lt;mrow&gt;&lt;mtext&gt;curl&lt;\/mtext&gt;&lt;mspace width=&quot;0.2em&quot; \/&gt;&lt;mstyle mathvariant=&quot;bold&quot; mathsize=&quot;normal&quot;&gt;&lt;mtext&gt;F&lt;\/mtext&gt;&lt;\/mstyle&gt;&lt;mo&gt;=&lt;\/mo&gt;&lt;mn&gt;0&lt;\/mn&gt;&lt;mo&gt;.&lt;\/mo&gt;&lt;\/mrow&gt;&lt;\/mrow&gt;&lt;annotation-xml encoding=&quot;MathML-Content&quot;&gt;&lt;mrow&gt;&lt;mtext&gt;curl&lt;\/mtext&gt;&lt;mspace width=&quot;0.2em&quot;&gt;&lt;\/mspace&gt;&lt;mstyle mathvariant=&quot;bold&quot; mathsize=&quot;normal&quot;&gt;&lt;mtext&gt;F&lt;\/mtext&gt;&lt;\/mstyle&gt;&lt;mo&gt;=&lt;\/mo&gt;&lt;mn&gt;0&lt;\/mn&gt;&lt;mo&gt;.&lt;\/mo&gt;&lt;\/mrow&gt;&lt;\/annotation-xml&gt;&lt;\/semantics&gt;&lt;\/math&gt;\"><span id=\"MathJax-Span-3195\" class=\"math\"><span id=\"MathJax-Span-3196\" class=\"mrow\"><span id=\"MathJax-Span-3197\" class=\"semantics\"><span id=\"MathJax-Span-3198\" class=\"mrow\"><span id=\"MathJax-Span-3199\" class=\"mrow\"><span id=\"MathJax-Span-3200\" class=\"mtext\">.\u00a0<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/p>\n<\/div>\n<h3 data-type=\"title\">Proof<\/h3>\n<p id=\"fs-id1167793445753\">Since conservative vector fields satisfy the cross-partials property, all the cross-partials of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0are equal. Therefore,<\/p>\n<p style=\"text-align: center;\">[latex]\\large{\\begin{aligned}  \\text{curl }{\\bf{F}}&=(R_y-Q_z){\\bf{i}}+(P_z-R_x){\\bf{j}}+(Q_x-P_y){\\bf{k}} \\\\  &=0  \\end{aligned}}[\/latex].<\/p>\n<p>[latex]_\\blacksquare[\/latex]<\/p>\n<p>The same theorem is true for vector fields in a plane.<\/p>\n<div id=\"fs-id1167793524959\" class=\"unnumbered\" data-type=\"equation\" data-label=\"\"><\/div>\n<p id=\"fs-id1167794121468\">Since a conservative vector field is the gradient of a scalar function, the previous theorem says that [latex]\\text{curl }(\\nabla{f})=0[\/latex] for any scalar function [latex]f[\/latex]. In terms of our curl notation, [latex]\\nabla\\times\\nabla{(f)}=0[\/latex]. This equation makes sense because the cross product of a vector with itself is always the zero vector. Sometimes equation [latex]\\nabla\\times\\nabla{(f)}=0[\/latex] is simplified as [latex]\\nabla\\times\\nabla=0[\/latex].<\/p>\n<div id=\"fs-id1167793495816\" class=\"theorem ui-has-child-title\" data-type=\"note\">\n<div class=\"textbox shaded\">\n<h3 style=\"text-align: center;\">theorem: curl test for a conservative field<\/h3>\n<hr \/>\n<p>Let [latex]{\\bf{F}}=\\langle{P},Q,R\\rangle[\/latex] be a vector field in space on a simply connected domain. If [latex]\\text{curl }{\\bf{F}}=0[\/latex], then\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.<\/p>\n<\/div>\n<h3 data-type=\"title\">Proof<\/h3>\n<p id=\"fs-id1167793355840\">Since [latex]\\text{curl }{\\bf{F}}=0[\/latex], we have that [latex]R_y=Q_z[\/latex],\u00a0[latex]P_z=R_x[\/latex], and\u00a0[latex]Q_x=P_y[\/latex]. Therefore,\u00a0[latex]{\\bf{F}}[\/latex]\u00a0satisfies the cross-partials property on a simply connected domain, and\u00a0Cross-Partial Property of Conservative Fields Theorem\u00a0implies that\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.<\/p>\n<p>[latex]_\\blacksquare[\/latex]<\/p>\n<p id=\"fs-id1167793498800\">The same theorem is also true in a plane. Therefore, if\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is a vector field in a plane or in space and the domain is simply connected, then\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative if and only if [latex]\\text{curl }{\\bf{F}}=0[\/latex].<\/p>\n<\/div>\n<div data-type=\"note\">\n<div class=\"textbox exercises\">\n<h3>Example: testing whether a vector field is conservative<\/h3>\n<p>Use the curl to determine whether [latex]{\\bf{F}}(x,y,z)=\\langle{y}z,xz,xy\\rangle[\/latex] is conservative.<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><span class=\"show-answer collapsed\" style=\"cursor: pointer\" data-target=\"q478259405\">Show Solution<\/span><\/p>\n<div id=\"q478259405\" class=\"hidden-answer\" style=\"display: none\">\n<p>Note that the domain of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is all of [latex]\\mathbb{R}^3[\/latex], which is simply connected (Figure 1). Therefore, we can test whether\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative by calculating its curl.<\/p>\n<div id=\"attachment_5333\" style=\"width: 392px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" aria-describedby=\"caption-attachment-5333\" class=\"size-full wp-image-5333\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/31234154\/6.56.jpg\" alt=\"&lt;img src=&quot;\/apps\/archive\/20220422.171947\/resources\/7749bed210536f0229f8267b69c34794d0305459&quot; data-media-type=&quot;image\/jpeg&quot; alt=&quot;A diagram showing the curl of a vector field in two dimensions. The curl is zero. The arrows seem to be pointing up and over into the yz plane.&quot; id=&quot;30&quot;&gt;\" width=\"382\" height=\"398\" \/><\/p>\n<p id=\"caption-attachment-5333\" class=\"wp-caption-text\">Figure 1. The curl of vector field [latex]{\\bf{F}}(x,y,z)=\\langle{y}z,xz,xy\\rangle[\/latex] is zero.<\/p>\n<\/div>\n<p id=\"fs-id1167794023727\">The curl of\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is<\/p>\n<p style=\"text-align: center;\">[latex]\\left(\\frac{\\partial}{\\partial{y}}xy-\\frac{\\partial}{\\partial{z}}xz\\right){\\bf{i}}+\\left(\\frac{\\partial}{\\partial{y}}yz-\\frac{\\partial}{\\partial{z}}xy\\right){\\bf{j}}+\\left(\\frac{\\partial}{\\partial{y}}xz-\\frac{\\partial}{\\partial{z}}yz\\right){\\bf{k}}=(x-x){\\bf{i}}+(y-y){\\bf{j}}+(z-z){\\bf{k}}=0[\/latex].<\/p>\n<p id=\"fs-id1167794054301\">Thus,\u00a0[latex]{\\bf{F}}[\/latex]\u00a0is conservative.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<p id=\"fs-id1167793562322\">We have seen that the curl of a gradient is zero. What is the divergence of a gradient? If [latex]f[\/latex] is a function of two variables, then [latex]\\text{div }(\\nabla{f})=\\nabla\\cdot(\\nabla{f})=f_{xx}+f_{yy}[\/latex]. We abbreviate this \u201cdouble dot product\u201d as [latex]\\nabla^2[\/latex]. This operator is called the\u00a0<span id=\"6f668e5d-300d-4e6c-aec3-70b59f71fe69_term268\" class=\"no-emphasis\" data-type=\"term\"><em data-effect=\"italics\">Laplace operator<\/em><\/span><em data-effect=\"italics\">,<\/em>\u00a0and in this notation Laplace\u2019s equation becomes [latex]\\nabla^2f=0[\/latex]. Therefore, a harmonic function is a function that becomes zero after taking the divergence of a gradient.<\/p>\n<p id=\"fs-id1167794018031\">Similarly, if [latex]f[\/latex] is a function of three variables then<\/p>\n<p style=\"text-align: center;\">[latex]\\large{\\text{div }(\\nabla{f})=\\nabla\\cdot(\\nabla{f})=f_{xx}+f_{yy}+f_{zz}}[\/latex].<\/p>\n<p id=\"fs-id1167793619900\">Using this notation we get Laplace\u2019s equation for harmonic functions of three variables:<\/p>\n<p style=\"text-align: center;\">[latex]\\large{\\nabla^2f=0}[\/latex].<\/p>\n<p id=\"fs-id1167793829624\">Harmonic functions arise in many applications. For example, the potential function of an electrostatic field in a region of space that has no static charge is harmonic.<\/p>\n<\/div>\n<div class=\"textbox exercises\">\n<h3>Example: analyzing a function<\/h3>\n<p>Is it possible for [latex]f(x, y)=x^{2}+x-y[\/latex] to be the potential function of an electrostatic field that is located in a region of [latex]\\mathbb{R}^2[\/latex] free of static charge?<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><span class=\"show-answer collapsed\" style=\"cursor: pointer\" data-target=\"q783691260\">Show Solution<\/span><\/p>\n<div id=\"q783691260\" class=\"hidden-answer\" style=\"display: none\">\n<p>If [latex]f[\/latex] were such a potential function, then [latex]f[\/latex] would be harmonic. Note that [latex]f_{xx}=2[\/latex], and [latex]f_{yy}=0[\/latex], so [latex]f_{xx}+f_{yy}\\ne0[\/latex]. Therefore, [latex]f[\/latex] is not harmonic and [latex]f[\/latex] cannot represent an electrostatic potential.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<div class=\"textbox key-takeaways\">\n<h3>try it<\/h3>\n<p>Is it possible for function [latex]f(x, y)=x^{2}-y^{2}+x[\/latex] to be the potential function of an electrostatic field located in a region of [latex]\\mathbb{R}^2[\/latex] free of static charge?<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><span class=\"show-answer collapsed\" style=\"cursor: pointer\" data-target=\"q746189149\">Show Solution<\/span><\/p>\n<div id=\"q746189149\" class=\"hidden-answer\" style=\"display: none\">\n<p>Yes.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<div data-type=\"note\"><\/div>\n\n\t\t\t <section class=\"citations-section\" role=\"contentinfo\">\n\t\t\t <h3>Candela Citations<\/h3>\n\t\t\t\t\t <div>\n\t\t\t\t\t\t <div id=\"citation-list-1125\">\n\t\t\t\t\t\t\t <div class=\"licensing\"><div class=\"license-attribution-dropdown-subheading\">CC licensed content, Original<\/div><ul class=\"citation-list\"><li>CP 6.45. <strong>Authored by<\/strong>: Ryan Melton. <strong>License<\/strong>: <em><a target=\"_blank\" rel=\"license\" href=\"https:\/\/creativecommons.org\/licenses\/by\/4.0\/\">CC BY: Attribution<\/a><\/em><\/li><\/ul><div class=\"license-attribution-dropdown-subheading\">CC licensed content, Shared previously<\/div><ul class=\"citation-list\"><li>Calculus Volume 3. <strong>Authored by<\/strong>: Gilbert Strang, Edwin (Jed) Herman. <strong>Provided by<\/strong>: OpenStax. <strong>Located at<\/strong>: <a target=\"_blank\" href=\"https:\/\/openstax.org\/books\/calculus-volume-3\/pages\/1-introduction\">https:\/\/openstax.org\/books\/calculus-volume-3\/pages\/1-introduction<\/a>. <strong>License<\/strong>: <em><a target=\"_blank\" rel=\"license\" href=\"https:\/\/creativecommons.org\/licenses\/by-nc-sa\/4.0\/\">CC BY-NC-SA: Attribution-NonCommercial-ShareAlike<\/a><\/em>. <strong>License Terms<\/strong>: Access for free at https:\/\/openstax.org\/books\/calculus-volume-3\/pages\/1-introduction<\/li><\/ul><\/div>\n\t\t\t\t\t\t <\/div>\n\t\t\t\t\t <\/div>\n\t\t\t <\/section>","protected":false},"author":428269,"menu_order":23,"template":"","meta":{"_candela_citation":"[{\"type\":\"cc\",\"description\":\"Calculus Volume 3\",\"author\":\"Gilbert Strang, Edwin (Jed) Herman\",\"organization\":\"OpenStax\",\"url\":\"https:\/\/openstax.org\/books\/calculus-volume-3\/pages\/1-introduction\",\"project\":\"\",\"license\":\"cc-by-nc-sa\",\"license_terms\":\"Access for free at https:\/\/openstax.org\/books\/calculus-volume-3\/pages\/1-introduction\"},{\"type\":\"original\",\"description\":\"CP 6.45\",\"author\":\"Ryan Melton\",\"organization\":\"\",\"url\":\"\",\"project\":\"\",\"license\":\"cc-by\",\"license_terms\":\"\"}]","CANDELA_OUTCOMES_GUID":"","pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-1125","chapter","type-chapter","status-publish","hentry"],"part":24,"_links":{"self":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapters\/1125","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapters"}],"about":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/wp\/v2\/types\/chapter"}],"author":[{"embeddable":true,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/wp\/v2\/users\/428269"}],"version-history":[{"count":71,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapters\/1125\/revisions"}],"predecessor-version":[{"id":6118,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapters\/1125\/revisions\/6118"}],"part":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/parts\/24"}],"metadata":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapters\/1125\/metadata\/"}],"wp:attachment":[{"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/wp\/v2\/media?parent=1125"}],"wp:term":[{"taxonomy":"chapter-type","embeddable":true,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/pressbooks\/v2\/chapter-type?post=1125"},{"taxonomy":"contributor","embeddable":true,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/wp\/v2\/contributor?post=1125"},{"taxonomy":"license","embeddable":true,"href":"https:\/\/courses.lumenlearning.com\/calculus3\/wp-json\/wp\/v2\/license?post=1125"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}