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 32 - The Magnetic Field - Exercises and Problems - Page 957: 21

Answer

${\bf 7.0}\;\rm A$

Work Step by Step

According to Ampere's law, the line integral of the magnetic field around a closed path is given by $$\oint \vec B\cdot d\vec s=\mu_0I_{through}$$ where $ I_{through}=I_1+I_3-I_2$ is the current through the area bounded by the integration path. $$\oint \vec B\cdot d\vec s=\mu_0(I_1+I_3-I_2)$$ We can see, from the given graph, and from the right-hand rule, that the magnetic field of $I_2$ is the only field that opposes the path direction. Solving for $I_3$; $$I_3=\dfrac{\oint \vec B\cdot d\vec s}{\mu_0}-I_1+I_2$$ Plug the known; $$I_3=\dfrac{(3.77\times 10^{-6})}{(4\pi \times 10^{-7})}-2+6$$ $$I_3=\color{red}{\bf 7.0}\;\rm A$$
Update this answer!

You can help us out by revising, improving and updating this answer.

Update this answer

After you claim an answer you’ll have 24 hours to send in a draft. An editor will review the submission and either publish your submission or provide feedback.