{"id":8879,"date":"2024-01-23T19:38:17","date_gmt":"2024-01-23T14:08:17","guid":{"rendered":"https:\/\/physicscatalyst.com\/article\/?p=8879"},"modified":"2024-01-23T19:38:22","modified_gmt":"2024-01-23T14:08:22","slug":"integration-of-root-x","status":"publish","type":"post","link":"https:\/\/physicscatalyst.com\/article\/integration-of-root-x\/","title":{"rendered":"integration of root x"},"content":{"rendered":"\n<p>The integral of the root x, can be found using power rule. The integral of $\\sqrt x $ with respect to (x) is:<\/p>\n\n\n\n<p>\\[<br>\\int \\sqrt x \\, dx =\\frac{2}{3} x^{3\/2} + C<br>\\]<\/p>\n\n\n\n<p>Here, (C) represents the constant of integration, which is added because the process of integration determines the antiderivative up to an arbitrary constant.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Proof of integration of root x<\/h2>\n\n\n\n<p>To integrate the square root of $x $ (i.e., $\\sqrt{x}$), we express it as $x^{1\/2} $. The integral is then:<\/p>\n\n\n\n<p>$$ \\int \\sqrt{x} \\, dx = \\int x^{1\/2} \\, dx $$<\/p>\n\n\n\n<p>To integrate this, we use the power rule for integration:<\/p>\n\n\n\n<p>$$ \\int x^n \\, dx = \\frac{x^{n+1}}{n+1} + C $$<\/p>\n\n\n\n<p>where $C $ is the constant of integration. Applying this rule:<\/p>\n\n\n\n<p>$$ \\int x^{1\/2} \\, dx = \\frac{x^{(1\/2) + 1}}{(1\/2) + 1} + C = \\frac{x^{3\/2}}{3\/2} + C $$<\/p>\n\n\n\n<p>Simplifying the fraction:<\/p>\n\n\n\n<p>$$ = \\frac{2}{3} x^{3\/2} + C $$<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p>So, the integral of (\\sqrt{x}$ is:<\/p>\n\n\n\n<p>$$ \\frac{2}{3} x^{3\/2} + C $$<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Integration based on root x<\/h2>\n\n\n\n<p>$$ \\int \\sqrt{ax + b} \\, dx = \\frac{2}{3a} (ax + b)^{3\/2} + C $$<\/p>\n\n\n\n<p><strong>Proof<\/strong><\/p>\n\n\n\n<p>Choose a substitution that simplifies the integrand. Let ( $u = ax + b$ ). Then, ( $du = a \\, dx$ ) or ( $dx = \\frac{du}{a}$ ).<br>Substitute ( u ) and ( dx ) into the integral:<br>$$= \\int \\sqrt{u} \\cdot \\frac{du}{a} $$<br>$$= \\frac{1}{a} \\int u^{1\/2} \\, du $$<br>$$= \\frac{1}{a} \\cdot \\frac{2}{3} u^{3\/2} + C $$<br>Here, ( C ) is the constant of integration.<br>Substitute back for ( u ) to get the final answer:<br>$$\\int \\sqrt{ax + b} \\, dx= \\frac{2}{3a} (ax + b)^{3\/2} + C $$<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Definite Integral of root x<\/h2>\n\n\n\n<p>To evaluate a definite integral of the root x, $\\int_a^b \\sqrt x \\, dx$, where $ a $ and $ b $ are the limits of integration, we follow a similar process as with the indefinite integral and the we&#8217;ll apply the limits at the end.<\/p>\n\n\n\n<p>$$<br>\\int_a^b \\sqrt(x) \\, dx = [ \\frac{2}{3} x^{3\/2}]_a^b<br>$$<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Solved Examples<\/h2>\n\n\n\n<p><strong>Question 1<\/strong><\/p>\n\n\n\n<p>$$ \\int \\sqrt{3x &#8211; 1} \\, dx $$<\/p>\n\n\n\n<p><strong>Solution<\/strong><\/p>\n\n\n\n<p>Choose a substitution that simplifies the integrand. Let $ u = 3x &#8211; 1 $. Then, $ du = 3 \\, dx $ or $ dx = \\frac{du}{3} $.<br>Substitute $ u $ and $ dx $ into the integral:<br>$$ =\\int \\sqrt{u} \\cdot \\frac{du}{3} $$<br>You can simplify this to:<br>$$ =\\frac{1}{3} \\int u^{1\/2} \\, du $$<br>Now integrate with respect to $ u $:<br>$$ =\\frac{1}{3} \\cdot \\frac{2}{3} u^{3\/2} + C $$<br>Here, $ C $ is the constant of integration.<br>Substitute back for $ u $ to get the final answer:<br>$$= \\frac{2}{9} (3x &#8211; 1)^{3\/2} + C $$<\/p>\n\n\n\n<p><strong>Question 2<\/strong><\/p>\n\n\n\n<p>$$ \\int \\sqrt{x} \\cdot \\ln(x) \\, dx $$<\/p>\n\n\n\n<p><strong>Solution<\/strong><\/p>\n\n\n\n<p>Integrating $ \\sqrt{x} \\cdot \\ln(x) $ requires the use of integration by parts.<\/p>\n\n\n\n<p>$$ \\int u \\, dv = uv &#8211; \\int v \\, du $$<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Let $ u = \\ln(x) $ (since the derivative of $ \\ln(x) $ is simpler than its integral).<\/li>\n\n\n\n<li>Then $ dv = \\sqrt{x} \\, dx $ (since we know how to integrate $ \\sqrt{x} $).<\/li>\n<\/ul>\n\n\n\n<p>Then<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>$ du = \\frac{1}{x} \\, dx $.<\/li>\n\n\n\n<li>$ v = \\int \\sqrt{x} \\, dx = \\int x^{1\/2} \\, dx = \\frac{2}{3} x^{3\/2} $ (using the power rule).<\/li>\n<\/ul>\n\n\n\n<p>Therefore<\/p>\n\n\n\n<p>$$ \\int \\sqrt{x} \\cdot \\ln(x) \\, dx = uv &#8211; \\int v \\, du $$<br>$$ = \\ln(x) \\cdot \\frac{2}{3} x^{3\/2} &#8211; \\int \\frac{2}{3} x^{3\/2} \\cdot \\frac{1}{x} \\, dx $$<br>$$ = \\frac{2}{3} x^{3\/2} \\ln(x) &#8211; \\frac{2}{3} \\int x^{1\/2} \\, dx $$<br>$$ = \\frac{2}{3} x^{3\/2} \\ln(x) &#8211; \\frac{2}{3} \\cdot \\frac{2}{3} x^{3\/2} + C $$<br>$$ = \\frac{2}{3} x^{3\/2} \\ln(x) &#8211; \\frac{4}{9} x^{3\/2} + C $$<\/p>\n\n\n\n<p>I hope you like this article on integration of root x interesting and useful<\/p>\n\n\n\n<div class=\"wp-block-group has-ast-global-color-4-background-color has-background is-layout-constrained wp-container-core-group-is-layout-ca99af60 wp-block-group-is-layout-constrained\" style=\"border-radius:17px;margin-top:var(--wp--preset--spacing--20);margin-bottom:var(--wp--preset--spacing--20);padding-top:var(--wp--preset--spacing--20);padding-right:var(--wp--preset--spacing--50);padding-bottom:var(--wp--preset--spacing--20);padding-left:var(--wp--preset--spacing--50)\"><div class=\"wp-block-group__inner-container\">\n<p class=\"has-medium-font-size\">Other Integration Related Articles<\/p>\n\n\n\n<figure class=\"wp-block-table is-style-regular\" style=\"padding-right:0;padding-left:0;font-size:16px\"><table style=\"border-style:none;border-width:0px\"><tbody><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-tan-inverse-x\/\">Integration of tan inverse x<\/a><\/td><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-cos-inverse-x\/\">Integration of cos inverse x<\/a><\/td><\/tr><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-cos-square-x\/\">Integration of cos square x<\/a><\/td><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-fractional-part-of-x\/\">Integration of fractional part of x<\/a><\/td><\/tr><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-uv-formula\/\">integration of uv formula<\/a><\/td><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-log-x\/\">integration of log x<\/a><\/td><\/tr><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-sin-inverse-x\/\">integration of sin inverse x<\/a><\/td><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-constant\/\">Integration of constant term<\/a><\/td><\/tr><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-hyperbolic-functions\/\">integration of hyperbolic functions<\/a><\/td><td><a data-type=\"post\" data-id=\"5701\" href=\"https:\/\/physicscatalyst.com\/article\/integration-formulas-list\/\">List of Integration Formulas <\/a><\/td><\/tr><tr><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-log-sinx\/\">integration of log sinx<\/a><\/td><td><a href=\"https:\/\/physicscatalyst.com\/article\/integration-of-sin-x-cos-x-dx\/\">integration of sin x cos x dx<\/a><\/td><\/tr><\/tbody><\/table><\/figure>\n<\/div><\/div>\n","protected":false},"excerpt":{"rendered":"<p>The integral of the root x, can be found using power rule. The integral of $\\sqrt x $ with respect to (x) is: \\[\\int \\sqrt x \\, dx =\\frac{2}{3} x^{3\/2} + C\\] Here, (C) represents the constant of integration, which is added because the process of integration determines the antiderivative up to an arbitrary constant. [&hellip;]<\/p>\n","protected":false},"author":8,"featured_media":0,"comment_status":"open","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_uag_custom_page_level_css":"","site-sidebar-layout":"default","site-content-layout":"","ast-site-content-layout":"default","site-content-style":"default","site-sidebar-style":"default","ast-global-header-display":"","ast-banner-title-visibility":"","ast-main-header-display":"","ast-hfb-above-header-display":"","ast-hfb-below-header-display":"","ast-hfb-mobile-header-display":"","site-post-title":"","ast-breadcrumbs-content":"","ast-featured-img":"","footer-sml-layout":"","theme-transparent-header-meta":"","adv-header-id-meta":"","stick-header-meta":"","header-above-stick-meta":"","header-main-stick-meta":"","header-below-stick-meta":"","astra-migrate-meta-layouts":"set","ast-page-background-enabled":"default","ast-page-background-meta":{"desktop":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"ast-content-background-meta":{"desktop":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"tablet":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""},"mobile":{"background-color":"var(--ast-global-color-5)","background-image":"","background-repeat":"repeat","background-position":"center center","background-size":"auto","background-attachment":"scroll","background-type":"","background-media":"","overlay-type":"","overlay-color":"","overlay-opacity":"","overlay-gradient":""}},"footnotes":""},"categories":[498],"tags":[],"class_list":["post-8879","post","type-post","status-publish","format-standard","hentry","category-maths"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.4 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>integration of root x - physicscatalyst&#039;s Blog<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/physicscatalyst.com\/article\/integration-of-root-x\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"integration of root x - physicscatalyst&#039;s Blog\" \/>\n<meta property=\"og:description\" content=\"The integral of the root x, can be found using power rule. 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The integral of $\\sqrt x $ with respect to (x) is: \\[\\int \\sqrt x \\, dx =\\frac{2}{3} x^{3\/2} + C\\] Here, (C) represents the constant of integration, which is added because the process of integration determines the antiderivative up to an arbitrary constant.&hellip;","_links":{"self":[{"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/posts\/8879","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/users\/8"}],"replies":[{"embeddable":true,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/comments?post=8879"}],"version-history":[{"count":2,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/posts\/8879\/revisions"}],"predecessor-version":[{"id":8881,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/posts\/8879\/revisions\/8881"}],"wp:attachment":[{"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/media?parent=8879"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/categories?post=8879"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physicscatalyst.com\/article\/wp-json\/wp\/v2\/tags?post=8879"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}