Physics Technology Update (4th Edition)

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

Chapter 24 - Alternating-Current Circuits - Problems and Conceptual Exercises - Page 871: 88

Answer

(a) $3.44mA$ (b) $10.5nF$

Work Step by Step

(a) We can find the rms current as follows: The impedance of the circuit is $Z=\sqrt{R^2+X_L^2}$ $\implies Z=\sqrt{(1150)^2+(3967)^2}$ $\implies Z=4130\Omega$ Now $I_{rms}=\frac{V_{rms}}{Z}$ $\implies I_{rms}=\frac{14.2}{4.30}$ $I_{rms}=0.003438A$ $\implies I_{rms}=3.44mA$ (b) We can determine the required capacitance as follows: $\frac{1}{\omega C}=\omega L\pm (\frac{V_{rms}^2}{I_{rms}^2})^{\frac{1}{2}}$ We plug in the known values to obtain: $\frac{1}{\omega C}=3967\pi [(\frac{14.2}{1.719\times 10^{-3}})^2-(1150)^2]^{\frac{1}{2}}$ This simplifies to: $\frac{1}{\omega C}=12147$ or $\frac{1}{\omega C}=-4213$ $\implies C=1.047\times 10^{-9}F=1.047nF$ or $C=-30.2\times 10^{-9}F=-30.2nF$ As the capacitance is not negative, therefore $C=-30.2nF$ is wrong and we have $C=10.5nF$
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