Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 24 - Electric Potential - Problems - Page 711: 20

Answer

At $~~x = -\frac{d}{2},~~$ then $V_{net} = 0$

Work Step by Step

We can write a general equation for the net electric potential: $V_{net} = \frac{1}{4\pi~\epsilon_0}\sum \frac{q_i}{r_i}$ It is given that $V_{net} = 0$ at the point $x = \frac{d}{4}$ We can write an expression for the net electric potential at a point due to these two charges: $V_{net} = \frac{1}{4\pi~\epsilon_0}~(\frac{q_1}{r_1}+\frac{q_2}{r_2})$ $V_{net} = \frac{1}{4\pi~\epsilon_0}~(\frac{q_1}{d/4}+\frac{q_2}{3d/4})$ $V_{net} = \frac{1}{4\pi~\epsilon_0}~(\frac{4q_1}{d}+\frac{4q_2}{3d})$ If $V_{net} = 0$ at $x = \frac{d}{4},$ then $(\frac{4q_1}{d}+\frac{4q_2}{3d}) = 0$ Then: $q_2 = -3q_1$ If $(\frac{q_1}{r_1}-\frac{3q_1}{r_2}) = 0$, then $V_{net} = 0$ If $~~r_2 = 3r_1~~$ then $V_{net} = 0$ Suppose $x$ is a negative value of $x$ where $V_{net} = 0$ Then $~~r_1 = -x~~$ and $~~r_2 = d-x$ We can find $x$: $r_2 = 3r_1$ $d-x = -3x$ $-2x = d$ $x = -\frac{d}{2}$ At $~~x = -\frac{d}{2},~~$ then $V_{net} = 0$
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