{"id":1232,"date":"2025-10-15T15:42:10","date_gmt":"2025-10-15T15:42:10","guid":{"rendered":"https:\/\/content.one.lumenlearning.com\/calculus3\/?post_type=chapter&#038;p=1232"},"modified":"2025-10-29T16:21:38","modified_gmt":"2025-10-29T16:21:38","slug":"double-integrals-in-polar-coordinates-learn-it-2","status":"publish","type":"chapter","link":"https:\/\/content.one.lumenlearning.com\/calculus3\/chapter\/double-integrals-in-polar-coordinates-learn-it-2\/","title":{"raw":"Double Integrals in Polar Coordinates: Learn It 2","rendered":"Double Integrals in Polar Coordinates: Learn It 2"},"content":{"raw":"<h2 data-type=\"title\">General Polar Regions of Integration<\/h2>\r\nTo evaluate the double integral of a continuous function by iterated integrals over general polar regions, we consider regions analogous to Type I and Type II as discussed earlier for rectangular coordinates. It is more common to write polar equations as [latex]r = f(\\theta)[\/latex] than [latex]\\theta = f(r)[\/latex], so we describe a general polar region as [latex]R = {(r,\\theta)\\mid \\alpha \\leq \\theta \\leq \\beta, h_1(\\theta) \\leq r \\leq h_2(\\theta) }[\/latex] (see the following figure).\r\n\r\n[caption id=\"attachment_1362\" align=\"aligncenter\" width=\"354\"]<img class=\"size-full wp-image-1362\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/25143121\/5-3-5.jpeg\" alt=\"A region D is shown in polar coordinates with edges given by theta = alpha, theta = beta, r = h2(theta), and r = h1(theta).\" width=\"354\" height=\"333\" \/> Figure 5.\u00a0A general polar region between [latex]\\alpha &lt; 0&lt;\\beta[\/latex] and\u00a0[latex]h_{1}(\\theta) &lt; r&lt;h_{2}(\\theta)[\/latex].[\/caption]<section class=\"textbox keyTakeaway\" aria-label=\"Key Takeaway\">\r\n<h3>double integrals over a general polar regions<\/h3>\r\nIf [latex]{f}{(r,{\\theta})}[\/latex] is continuous on a general polar region [latex]D[\/latex] as described above, then:\r\n<p style=\"text-align: center;\">[latex]\\underset{R}{\\displaystyle\\iint}f(r,\\theta)r \\ dr \\ d\\theta=\\displaystyle\\int_{\\theta=\\alpha}^{\\theta=\\beta}\\displaystyle\\int_{r=h_1(\\theta)}^{r=h_2(\\theta)}f(r,\\theta)r \\ dr \\ d\\theta[\/latex]<\/p>\r\n\r\n<\/section><section class=\"textbox example\" aria-label=\"Example\">Evaluate the integral [latex]\\underset{D}{\\displaystyle\\iint}{r^2}{\\sin\\theta}{r} \\ {dr} \\ {d{\\theta}}[\/latex] where [latex]D[\/latex] is the region bounded by the polar axis and the upper half of the cardioid [latex]{r} = {1} + {\\cos\\theta}[\/latex].[reveal-answer q=\"425517802\"]Show Solution[\/reveal-answer]\r\n[hidden-answer a=\"425517802\"]We can describe the region [latex]D[\/latex] as [latex]\\{(r,\\theta)\\mid0\\leq\\theta\\leq\\pi,0\\leq{r}\\leq1+\\cos\\theta\\}[\/latex] as shown in the following figure.[caption id=\"attachment_1363\" align=\"aligncenter\" width=\"425\"]<img class=\"size-full wp-image-1363\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/25143147\/5-3-6.jpeg\" alt=\"A region D is given as the top half of a cardioid with equation r = 1 + cos theta.\" width=\"425\" height=\"360\" \/> Figure 6.\u00a0The region [latex]D[\/latex] is the top half of a cardioid.[\/caption]Hence, we have<center>\r\n[latex]\r\n\\begin{array}{ccc}\r\n\\underset{D}{\\displaystyle\\iint}r^2\\sin\\theta{r}dr \\ d\\theta \\hfill &amp;= \\hfill \\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}\\displaystyle\\int_{r=0}^{r=1+\\cos\\theta}(r^2\\sin\\theta)r dr d\\theta \\\\\r\n\\hfill &amp;= \\hfill \\frac{1}{4}\\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}[r^4]_{r=0}^{r=1+\\cos\\theta}\\sin\\theta d\\theta \\\\\r\n\\hfill &amp;= \\hfill \\frac{1}{4}\\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}(1+\\cos\\theta)^4\\sin\\theta d\\theta \\\\\r\n\\hfill &amp;= \\hfill -\\frac{1}{4}[\\frac{(1+\\cos\\theta)^5}{5}]_0^{\\pi}=\\frac{8}{5}.\r\n\\end{array}\r\n[\/latex]<\/center>[\/hidden-answer]<\/section>","rendered":"<h2 data-type=\"title\">General Polar Regions of Integration<\/h2>\n<p>To evaluate the double integral of a continuous function by iterated integrals over general polar regions, we consider regions analogous to Type I and Type II as discussed earlier for rectangular coordinates. It is more common to write polar equations as [latex]r = f(\\theta)[\/latex] than [latex]\\theta = f(r)[\/latex], so we describe a general polar region as [latex]R = {(r,\\theta)\\mid \\alpha \\leq \\theta \\leq \\beta, h_1(\\theta) \\leq r \\leq h_2(\\theta) }[\/latex] (see the following figure).<\/p>\n<figure id=\"attachment_1362\" aria-describedby=\"caption-attachment-1362\" style=\"width: 354px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1362\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/25143121\/5-3-5.jpeg\" alt=\"A region D is shown in polar coordinates with edges given by theta = alpha, theta = beta, r = h2(theta), and r = h1(theta).\" width=\"354\" height=\"333\" \/><figcaption id=\"caption-attachment-1362\" class=\"wp-caption-text\">Figure 5.\u00a0A general polar region between [latex]\\alpha &lt; 0&lt;\\beta[\/latex] and\u00a0[latex]h_{1}(\\theta) &lt; r&lt;h_{2}(\\theta)[\/latex].<\/figcaption><\/figure>\n<section class=\"textbox keyTakeaway\" aria-label=\"Key Takeaway\">\n<h3>double integrals over a general polar regions<\/h3>\n<p>If [latex]{f}{(r,{\\theta})}[\/latex] is continuous on a general polar region [latex]D[\/latex] as described above, then:<\/p>\n<p style=\"text-align: center;\">[latex]\\underset{R}{\\displaystyle\\iint}f(r,\\theta)r \\ dr \\ d\\theta=\\displaystyle\\int_{\\theta=\\alpha}^{\\theta=\\beta}\\displaystyle\\int_{r=h_1(\\theta)}^{r=h_2(\\theta)}f(r,\\theta)r \\ dr \\ d\\theta[\/latex]<\/p>\n<\/section>\n<section class=\"textbox example\" aria-label=\"Example\">Evaluate the integral [latex]\\underset{D}{\\displaystyle\\iint}{r^2}{\\sin\\theta}{r} \\ {dr} \\ {d{\\theta}}[\/latex] where [latex]D[\/latex] is the region bounded by the polar axis and the upper half of the cardioid [latex]{r} = {1} + {\\cos\\theta}[\/latex].<\/p>\n<div class=\"qa-wrapper\" style=\"display: block\"><button class=\"show-answer show-answer-button collapsed\" data-target=\"q425517802\">Show Solution<\/button><\/p>\n<div id=\"q425517802\" class=\"hidden-answer\" style=\"display: none\">We can describe the region [latex]D[\/latex] as [latex]\\{(r,\\theta)\\mid0\\leq\\theta\\leq\\pi,0\\leq{r}\\leq1+\\cos\\theta\\}[\/latex] as shown in the following figure.<\/p>\n<figure id=\"attachment_1363\" aria-describedby=\"caption-attachment-1363\" style=\"width: 425px\" class=\"wp-caption aligncenter\"><img loading=\"lazy\" decoding=\"async\" class=\"size-full wp-image-1363\" src=\"https:\/\/s3-us-west-2.amazonaws.com\/courses-images\/wp-content\/uploads\/sites\/5667\/2021\/11\/25143147\/5-3-6.jpeg\" alt=\"A region D is given as the top half of a cardioid with equation r = 1 + cos theta.\" width=\"425\" height=\"360\" \/><figcaption id=\"caption-attachment-1363\" class=\"wp-caption-text\">Figure 6.\u00a0The region [latex]D[\/latex] is the top half of a cardioid.<\/figcaption><\/figure>\n<p>Hence, we have<\/p>\n<div style=\"text-align: center;\">\n[latex]\\begin{array}{ccc}  \\underset{D}{\\displaystyle\\iint}r^2\\sin\\theta{r}dr \\ d\\theta \\hfill &= \\hfill \\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}\\displaystyle\\int_{r=0}^{r=1+\\cos\\theta}(r^2\\sin\\theta)r dr d\\theta \\\\  \\hfill &= \\hfill \\frac{1}{4}\\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}[r^4]_{r=0}^{r=1+\\cos\\theta}\\sin\\theta d\\theta \\\\  \\hfill &= \\hfill \\frac{1}{4}\\displaystyle\\int_{\\theta=0}^{\\theta=\\pi}(1+\\cos\\theta)^4\\sin\\theta d\\theta \\\\  \\hfill &= \\hfill -\\frac{1}{4}[\\frac{(1+\\cos\\theta)^5}{5}]_0^{\\pi}=\\frac{8}{5}.  \\end{array}[\/latex]<\/div>\n<\/div>\n<\/div>\n<\/section>\n","protected":false},"author":15,"menu_order":20,"template":"","meta":{"_candela_citation":"[]","pb_show_title":"on","pb_short_title":"","pb_subtitle":"","pb_authors":[],"pb_section_license":""},"chapter-type":[],"contributor":[],"license":[],"class_list":["post-1232","chapter","type-chapter","status-publish","hentry"],"part":432,"module-header":"- Select Header 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