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 719: 37

Answer

(a) $0.86J$ (b) less than (c) $-0.54J$

Work Step by Step

(a) We know that $r_{32}=\sqrt{(0.25m)^2+(0.16m)^2}$ $r_{32}=0.296m$ $W=-Kq_2(\frac{q_1}{r_{12}}+\frac{q_2}{r_{32}})$ We plug in the known values to obtain: $W=-(8.99\times 10^{9}Nm^2/C^2)(+2.7\times 10^{-6}C)(\frac{-6.1\times 10^{-6}C}{0.25m}+\frac{-3.3\times 10^{-6}C}{0.296m})$ $\implies W=0.86J$ (b) We know that the repulsive force for the charges $-6.1\mu C$ and $-3.3\mu C$ is of greater magnitude when compared to the attractive force between the charges $-6.1\mu C$ and $+2.7\mu C$. Thus, we conclude that the work done in the given case is less than that determined in part (a). (c) We can determine the required work done as follows: $W=-Kq_1(\frac{q_3}{r_{13}}+\frac{q_2}{r_{12}})$ We plug in the known values to obtain: $W=-(8.99\times 10^{9}Nm^2/C^2)(-6.1\times 10^{-6}C)(\frac{-3.3\times 10^{-6}C}{0.16m}+\frac{2.7\times 10^{-6}C}{0.25m})$ This simplifies to: $W=-0.54J$
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