Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 23 - Magnetic Flux and Faraday's Law of Induction - Problems and Conceptual Exercises - Page 834: 88

Answer

Please see the work below.

Work Step by Step

(a) We know that $\epsilon=-NA(\frac{\Delta B}{\Delta t})$ $\epsilon=-N(\pi r^2)(\frac{\Delta B}{\Delta t})$ We plug in the known values to obtain: $\epsilon=-(155)(\frac{\pi(0.0375m}{4})^2)(0)$ $\epsilon=0V $ (b) As $\epsilon=-N(\pi r^2)(\frac{\Delta B}{\Delta t})$ We plug in the known values to obtain: $\epsilon=(-155)(\pi\frac{(0.0375m)^2}{4})(\frac{-0.01T-0.02T}{5\times 10^{-3}s})$ $\epsilon=1.0V $ (c) At time $ t=15ms $ the induced emf is zero because the rate of change of the magnetic field is zero. As $\epsilon=-N(\pi r^2)(\frac{\Delta B}{\Delta t})$ We plug in the known values to obtain: $\epsilon=-(155)\frac{\pi(0.0375m)^2}{4}(0)$ $\epsilon=0V $ (d) We know that $\epsilon=-N(\pi r^2)(\frac{\Delta B}{\Delta t})$ We plug in the known values to obtain: $\epsilon=-(155)(\frac{\pi(0.375m)^2}{4})(\frac{0.01T-(-0.01T)}{10\times 10^{-3}s})$ $\epsilon=-0.3V $
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