From 74dcf28e0c41efd6485fb14a7f6e910ebe140fbf Mon Sep 17 00:00:00 2001 From: ben-jaynes <1btjaynes@gmail.com> Date: Wed, 7 Oct 2026 12:14:39 -0700 Subject: [PATCH] vault backup: 2026-10-07 12:14:39 --- ...- Double Integrals in Polar Coordinates.md | 53 +++++++++++-------- 1 file changed, 31 insertions(+), 22 deletions(-) diff --git a/College/AU 26/MATH 224 (Multivar)/Chapter 15.3 - Double Integrals in Polar Coordinates.md b/College/AU 26/MATH 224 (Multivar)/Chapter 15.3 - Double Integrals in Polar Coordinates.md index dd754a5..e1636f1 100644 --- a/College/AU 26/MATH 224 (Multivar)/Chapter 15.3 - Double Integrals in Polar Coordinates.md +++ b/College/AU 26/MATH 224 (Multivar)/Chapter 15.3 - Double Integrals in Polar Coordinates.md @@ -11,28 +11,37 @@ if a function is defined as $f(x,y)$ and the region it is integrated over is pol $$\int_{\alpha}^\beta \int_{a}^b f(r\cos(\theta), r\sin(\theta))r \ dr d\theta$$ -Find the volume of the solid below $z=1-x^2-y^2$ and above the first quadrant on the xy plane +> [!example] Example +> Find the volume of the solid below $z=1-x^2-y^2$ and above the first quadrant on the xy plane +> +> rearranging the equation gives $x^2+y^2=1-z$ which shows that each horizontal slice of the function is a circle centered at $(0,0)$ with a radius of $\sqrt{ 1-z }$ +> +> since the slice of the equation at $z=0$ forms the circle $x^2+y^2=1$ the bounds +> $$\begin{gather} +> 0\leq r \leq 1 \\ 0 \leq \theta \leq \frac{\pi}{2} +> \end{gather}$$ +> can be used to find the volume of the solid. +> +> writing out the integral with these bounds gives +> $$\begin{gather} +> \int \int_{R} f(x,y) dA \\[2ex] \int_{\alpha}^\beta \int_{a}^b f(r\cos(\theta), r\sin(\theta))r \ dr d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-(r\cos \theta)^2-(r\sin \theta)^2)r \ dr d\theta +> \end{gather}$$ +> This integral can now be solved similar to other double integrals +> $$\begin{gather} +> \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-(r\cos \theta)^2-(r\sin \theta)^2)r \ dr d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-r^2\cos^2 \theta-r^2\sin^2 \theta)r \ dr d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-r^2)r \ dr d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \int_{0}^1 r-r^3 \ dr d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \left( \left.\frac{r^2}{2}-\frac{r^4}{4} \right\vert_{0}^1 \right) d\theta \\[2ex] +> \int_{0}^{\frac{\pi}{2}} \frac{1}{4} d\theta \\[2ex] +> V=\frac{\pi}{8} +> \end{gather}$$ -rearranging the equation gives $x^2+y^2=1-z$ which shows that each horizontal slice of the function is a circle centered at $(0,0)$ with a radius of $\sqrt{ 1-z }$ -since the slice of the equation at $z=0$ forms the circle $x^2+y^2=1$ the bounds -$$\begin{gather} - 0\leq r \leq 1 \\ 0 \leq \theta \leq \frac{\pi}{2} -\end{gather}$$ -can be used to find the volume of the solid. +When are polar coordinates useful for evaluating double integrals? +- Domain has a simple formula in terms of $(r,\theta)$ +- Integrand has a simple formula in terms of $(r, \theta)$ -writing out the integral with these bounds gives -$$\begin{gather} - \int \int_{R} f(x,y) dA \\[2ex] \int_{\alpha}^\beta \int_{a}^b f(r\cos(\theta), r\sin(\theta))r \ dr d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-(r\cos \theta)^2-(r\sin \theta)^2)r \ dr d\theta -\end{gather}$$ -This integral can now be solved similar to other double integrals -$$\begin{gather} - \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-(r\cos \theta)^2-(r\sin \theta)^2)r \ dr d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-r^2\cos^2 \theta-r^2\sin^2 \theta)r \ dr d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \int_{0}^1 (1-r^2)r \ dr d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \int_{0}^1 r-r^3 \ dr d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \left( \left.\frac{r^2}{2}-\frac{r^4}{4} \right\vert_{0}^1 \right) d\theta \\[2ex] - \int_{0}^{\frac{\pi}{2}} \frac{1}{4} d\theta \\[2ex] - V=\frac{\pi}{8} -\end{gather}$$ \ No newline at end of file +Polar regions with functions as boundaries can also be integrated similar to cartesian ones +$$\int_{\alpha}^\beta \int_{h_{1}(\theta)}^{h_{2}(\theta)} f(r\cos \theta, r\sin \theta)r \ dr d\theta$$