Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 27 - Gauss's Law - Exercises and Problems - Page 808: 45

Answer

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Work Step by Step

According to Gauss’s law, $$\oint \vec E d \vec A=\dfrac{Q_{in}}{\epsilon_0}$$ Hence, $$EA_{sphere}=\dfrac{Q_{in}}{\epsilon_0}$$ So the electric field is given by $$E=\dfrac{Q_{in}}{A_{sphere}\epsilon_0}$$ $$E=\dfrac{Q_{in}}{4\pi r^2\epsilon_0}$$ where $r$ is the radius of the Gaussian sphere. We will use this formula to find the electric field for both cases. $$\color{blue}{\bf [a]}$$ $\bullet$ when $r\lt R$, $$E=\dfrac{Q_{in}}{4\pi r^2\epsilon_0}$$ where $Q_{in}=0$ since the charge is uniformly distributed on the sphere's outer surface. This means that there is no charge inside this plastic hollow sphere. $$\boxed{\vec E=\bf 0\;\rm N/C}$$ $$\color{blue}{\bf [b]}$$ $\bullet$ when $r\gt R$, $$E=\dfrac{Q_{in}}{4\pi r^2\epsilon_0}$$ where $Q_{in}=Q$ $$E=\dfrac{Q}{4\pi r^2\epsilon_0}$$ Hence, $$\boxed{\vec E=\dfrac{ 1}{4\pi \epsilon_0}\dfrac{Q}{r^2}\;\hat r}\tag{Outward}$$
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