Introduction to Electrodynamics 4e

Published by Pearson Education
ISBN 10: 9332550441
ISBN 13: 978-9-33255-044-5

Chapter 2 - Section 2.3 - Divergence and Curl of Electrostatic Fields - Problem - Page 76: 11

Answer

For $r\ge R$, $\vec{E} = {\sigma\times R^2 \over \epsilon_0\times r^2}\hat{r}$ For $r< R, \vec{E}=0$

Work Step by Step

Consider a gaussian spherical surface of radius $r$ where $r\ge R$ According to Gauss Law, $$\oint \vec{E}\cdot \vec{da} = \frac{Q_{enc}}{\epsilon_{0}} = \frac{\sigma\times 4\pi R^2}{\epsilon_0}$$ At all places of the Gaussian surface, $\vec{E}$ and $\vec{da}$ point in the same direction i.e $\hat{r}$ $$E\times 4\pi r^2 = {\sigma\times 4\pi R^2 \over \epsilon_0}$$ $$\vec{E} = {\sigma\times R^2 \over \epsilon_0\times r^2}\hat{r}$$ Now, For $r< R, Q_{enc} = 0$ and hence $\vec{E}=0$
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