Calculus (3rd Edition)

Published by W. H. Freeman
ISBN 10: 1464125260
ISBN 13: 978-1-46412-526-3

Chapter 15 - Differentiation in Several Variables - 15.6 The Chain Rule - Exercises - Page 810: 51

Answer

Using both rectangular and polar expressions for $\Delta f$, we verify that $f\left( {x,y} \right) = x$ and $f\left( {x,y} \right) = y$ are harmonic.

Work Step by Step

1. We have $f\left( {x,y} \right) = x$ We evaluate the Laplace operator using a. rectangular expression The partial derivatives are ${f_x} = 1$, ${\ \ \ }$ ${f_y} = 0$ ${f_{xx}} = 0$, ${\ \ \ }$ ${f_{yy}} = 0$ Therefore, $\Delta f = {f_{xx}} + {f_{yy}} = 0$. Since $\Delta f = {f_{xx}} + {f_{yy}} = 0$, $f$ is harmonic. b. polar expression In polar coordinates, we have $f\left( {r,\theta } \right) = r\cos \theta $ The partial derivatives are ${f_r} = \cos \theta $, ${\ \ \ }$ ${f_\theta } = - r\sin \theta $ ${f_{rr}} = 0$, ${\ \ \ }$ ${f_{\theta \theta }} = - r\cos \theta $ Using Eq. (13) we get $\Delta f = {f_{rr}} + \frac{1}{{{r^2}}}{f_{\theta \theta }} + \frac{1}{r}{f_r}$ $\Delta f = - \frac{1}{r}\cos \theta + \frac{1}{r}\cos \theta = 0$ Since $\Delta f = 0$, $f$ is harmonic. 2. We have $f\left( {x,y} \right) = y$ We evaluate the Laplace operator using a. rectangular expression The partial derivatives are ${f_x} = 0$, ${\ \ \ }$ ${f_y} = 1$ ${f_{xx}} = 0$, ${\ \ \ }$ ${f_{yy}} = 0$ Therefore, $\Delta f = {f_{xx}} + {f_{yy}} = 0$. Since $\Delta f = 0$, $f$ is harmonic. b. polar expression In polar coordinates, we have $f\left( {r,\theta } \right) = r\sin \theta $ The partial derivatives are ${f_r} = \sin \theta $, ${\ \ \ }$ ${f_\theta } = r\cos \theta $ ${f_{rr}} = 0$, ${\ \ \ }$ ${f_{\theta \theta }} = - r\sin \theta $ Using Eq. (13) we get $\Delta f = {f_{rr}} + \frac{1}{{{r^2}}}{f_{\theta \theta }} + \frac{1}{r}{f_r}$ $\Delta f = - \frac{1}{r}\sin \theta + \frac{1}{r}\sin \theta = 0$ Since $\Delta f = 0$, $f$ is harmonic.
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