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 1002: 84

Answer

${\bf 159}\;\rm A/s$

Work Step by Step

Let's assume that the resistance of the solenoid is zero and it is an ideal one at which the magnetic field at any instant is the same everywhere within the solenoid. Recalling that $$E=\dfrac{r}{2}\left| \dfrac{dB}{dt}\right|$$ where $B=\dfrac{\mu_0 NI}{l}$ where $N/l=n$, so $$E=\dfrac{\mu_0 n r}{2}\left| \dfrac{d I }{dt}\right|$$ Hence, $$\left| \dfrac{d I }{dt}\right|=\dfrac{2E}{\mu_0 n r}$$ Plug the known; $$\left| \dfrac{d I }{dt}\right|=\dfrac{2(5\times 10^{-4})}{(4\pi\times 10^{-7})(1000)(0.5\times 10^{-2})}$$ $$\left| \dfrac{d I }{dt}\right|=\color{red}{\bf 159}\;\rm A/s$$
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