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: 90

Answer

(a) $291.8\Omega$ (b) greater than

Work Step by Step

(a) We can find the required resistance as $R=Zcos\phi$ We plug in the known values to obtain: $R=(337\Omega) cos(30^{\circ})$ $\implies R=291.8\Omega$ (b) We know that $tan 30^{\circ}=\frac{X_L-X_C}{R}$ $\implies X_L-X_C=R\frac{1}{\sqrt{3}}$ $\implies X_L=\frac{R}{\sqrt{3}}+X_C$ The inductive reactance is given as $X_L=\omega L$ and the capacitance in terms of frequency and capacitance is $X_C=\frac{1}{\omega C}$ Now $X_L=\frac{R}{\sqrt{3}}+X_C$ As $X_L\gt X_C$ $\implies \omega _L\gt \frac{1}{\omega C}$ $\implies \omega \gt \sqrt{\frac{1}{LC}}$ We know that for resonance frequency, the inductive reactance and capacitive reactance are equal in magnitude. Thus, we have $\omega=\sqrt{\frac{1}{LC}}$ and we conclude that the driving frequency is greater than the resonance frequency of the circuit.
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