Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 33 - Electromagnetic Induction - Exercises and Problems - Page 1001: 66

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Work Step by Step

$$\color{blue}{\bf [a]}$$ We know that the potential difference through an inductor is given by $$\Delta V_L=-L\dfrac{dI}{dt}$$ where $I=I_0\sin (\omega t)$, so $$\Delta V_L=-I_0L\dfrac{d }{dt}\sin (\omega t)$$ $$\boxed{\Delta V_L=-\omega I_0L \cos(\omega t)}$$ $$\color{blue}{\bf [b]}$$ Maximum voltage occurs when $\cos(\omega t)=1$, so $$(\Delta V_L)_{\rm max}= \omega I_0L $$ where $\omega=2\pi f$; $$(\Delta V_L)_{\rm max}= 2\pi fI_0L $$ Solving for $I_0$; $$I_0=\dfrac{(\Delta V_L)_{\rm max}}{ 2\pi fL}$$ Plug the known; $$I_0=\dfrac{(0.20)}{-2\pi (500\times 10^3)(50\times 10^{-6})}$$ $$I_0=\color{red}{\bf 1.27}\;\rm mA$$
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