Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (4th Edition)

Published by Pearson
ISBN 10: 0133942651
ISBN 13: 978-0-13394-265-1

Chapter 32 - AC Circuits - Exercises and Problems - Page 925: 27

Answer

(a) $f_0 = 200~kHz$ (b) $f_0 = 141~kHz$

Work Step by Step

We can write an expression for the resonance frequency: $\omega_0 = \frac{1}{\sqrt{L~C}}$ $2\pi~f_0 = \frac{1}{\sqrt{L~C}}$ $f_0 = \frac{1}{2\pi~\sqrt{L~C}}$ (a) Note that the resonance frequency $f_0$ does not depend on the resistor value. $f_0 = 200~kHz$ (b) If the capacitor value is doubled, then the resonance frequency $f_0$ decreases by a factor of $\frac{1}{\sqrt{2}}$ $f_0 = (\frac{1}{\sqrt{2}})~(200~kHz) = 141~kHz$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.