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 998: 31

Answer

${\bf 8.66}\;\rm T/s$

Work Step by Step

We have here a loop coil and a changing flux, so we must have an induced current. We know that the induced emf $\varepsilon$ is given by $$\varepsilon=\left|\dfrac{d\Phi}{dt}\right|=IR$$ where $\phi =AB\cos\theta$ and here $A$ is constant and $\theta=0^\circ$, so that $$ A \left|\dfrac{dB}{dt}\right|=IR$$ And for $N$ turns. $$ \pi r^2N \left|\dfrac{dB}{dt}\right|=IR$$ Hence, $$ \left|\dfrac{dB}{dt}\right|=\dfrac{IR}{ \pi r_{\rm coil}^2N}\tag 1$$ Now we need to find $R$ of the whole wire where $R$ is given by $$R=\dfrac{\rho L}{A}=\dfrac{\rho L}{\pi r^2}$$ where $L$ is the whole length of the wire that is given by $L=2\pi r_{\rm coil} N$ $$R =\dfrac{2\color{red}{\bf\not} \pi r_{\rm coil} N\rho_{\rm Cu} }{\color{red}{\bf\not} \pi r_{\rm wire}^{ 2}}$$ $$R =\dfrac{2 r_{\rm coil} N\rho_{\rm Cu} }{ r^2_{\rm wire} }$$ Plug into (1), $$ \left|\dfrac{dB}{dt}\right|=\dfrac{2\color{red}{\bf\not} r_{\rm coil} \color{red}{\bf\not} N\rho_{\rm Cu} I }{ \pi r_{\rm coil}^{\color{red}{\bf\not} 2}r^2_{\rm wire} \color{red}{\bf\not} N} $$ $$ \left|\dfrac{dB}{dt}\right|=\dfrac{2 \rho_{\rm Cu} I }{ \pi r_{\rm coil} r^2_{\rm wire} } $$ Plug the known; $$ \left|\dfrac{dB}{dt}\right|=\dfrac{2 (1.7\times 10^{-8})(2) }{ \pi (4\times 10^{-2}) (0.25\times 10^{-3})^2 } $$ $$ \left|\dfrac{dB}{dt}\right|=\color{red}{\bf 8.66}\;\rm T/s$$
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