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 872: 100

Answer

$607\mu H, 80.7\Omega$

Work Step by Step

We know that $R^2+(2\pi fL)^2=(\frac{V_{rms}}{I_{rms}})^2$......eq(1) We plug in the known values to obtain: $R^2+[2\pi L(20KHz)^2]^2=(\frac{5V}{45mA})^2$.....eq(2) We plug in the known values in eq(1) to obtain: $R^2+[2\pi L(25KHZ)]^2=(frac{5V}{40mA})^2$.....eq(3) Subtracting eq(2) from eq(3), we obtain: $[2\pi L(25KHz)^2-2\pi L(20KHz)]^2=(\frac{5V}{40mA})^2-(\frac{5V}{45mA})^2$ This simplifies to: $L=6.07\times 10^{-4}H$ $\implies L=607\mu H$ We plug in this value in eq(2) to obtain: $R^2=(\frac{5V}{45\times 10^{-3}A})^2-(2\pi (20KHz))^2(607\mu H)^2$ This simplifies to: $R=80.7\Omega$
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