Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 20 - Electric Potential and Electric Potential Energy - Problems and Conceptual Exercises - Page 718: 23

Answer

(a) $-\sqrt{2}Q$ (b) negative

Work Step by Step

(a) We know that $r_2=\sqrt{r^2+r^2}$ $\implies r_2=\sqrt{2}r$ The net potential at point A is given as $V_A=\frac{Kq_1}{r_1}+\frac{Kq_2}{r_2}$ Given that the net potential at point A is zero, we have: $\implies \frac{Kq_1}{r_1}+\frac{Kq_2}{r_2}=0$ $\implies \frac{q_1}{r_1}+\frac{q_2}{r_2}=0$ $\implies q_2=-(\frac{q_1}{r_1})r_2$ We substitute $+Q$ for $q_1$, r for $r_1$ and $\sqrt{2}r$ for $r_2$ $\implies q_2=-(\frac{+Q}{r})\sqrt{2}r$ $\implies q_2=-\sqrt{2} Q$ (b) We know that $V_B=K(\frac{q_1}{r_1}+\frac{q_2}{r_2})$ $\implies V_B=K(\frac{+Q}{\sqrt{2}r}+(\frac{-\sqrt{2}Q}{r}))$ $\implies V_B=\frac{-KQ}{\sqrt{2}r}$ Thus, the negative electric potential exists at point B.
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