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 28 - The Electric Potential - Exercises and Problems - Page 834: 29

Answer

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Work Step by Step

$$\color{blue}{\bf [a]}$$ It is obvious that the electric potential $V$ is always positive everywhere which means that the two charges must be positive. As a proof, we can see at $a\lt x\lt b$, the electric potential is also positive. $$\color{blue}{\bf [b]}$$ It seems that the two charges are equal in magnitude due to the symmetry of the given figure at the middle point between the two charges. Hence, $$\boxed{\dfrac{|q_a|}{|q_b|}=1} $$ $$\color{blue}{\bf [c]}$$ Since the two charges are positive, the elctric field at $x\gt b$ is pointing to the right, at $x\lt a$ is pointing to the left, and at $a\lt x\lt b$ is a vector sum of the two electric fields which must zero at the middle distance between both charges. See the figure below.
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