Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 21 - Electromagnetic Induction and Faraday's Law - General Problems - Page 623: 75

Answer

6.01 mJ.

Work Step by Step

The power dissipated by a resistor is $P=I^2R$. The energy dissipated is $E=P\Delta t=I^2R \Delta t$ Calculate the current I, which is created by the induced emf. The emf is given by Faraday’s Law. $$\epsilon=-\frac{\Delta \Phi_B}{\Delta t}=-\frac{A\Delta B}{\Delta t}$$ $$I=\frac{\epsilon}{R}=-\frac{A\Delta B}{R\Delta t}$$ $$ E=P\Delta t=I^2R \Delta t =\frac{A^2(\Delta B)^2}{R^2(\Delta t)^2}R\Delta t$$ $$ E=\frac{A^2(\Delta B)^2}{R (\Delta t) } $$ $$ E=\frac{((0.240m)^2)^2(0-0.665T)^2}{(6.10\Omega) (0.0400s) }=6.01\times10^{-3}J $$
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