University Physics with Modern Physics (14th Edition)

Published by Pearson
ISBN 10: 0321973615
ISBN 13: 978-0-32197-361-0

Chapter 27 - Magnetic Field and Magnetic Forces - Problems - Exercises - Page 915: 27.45

Answer

a) $\vec{\tau} = -NIAB \ \vec{a}_x$ and $U = 0$ b) $\vec{\tau} = \vec{0}$ and $U = -NIAB$ c) $\vec{\tau} = NIAB \ \vec{a}_x$ and $U = 0$ d) $\vec{\tau} = \vec{0}$ and $U = NIAB$

Work Step by Step

To calculate the torque, you need this formula : $\vec{\tau} = \vec{\mu} \times \vec{B} = I_{tot} \vec{A} \times \vec{B} = NIA \ \hat{\vec{n}} \times \vec{B}$ where $\hat{\vec{n}}$ is the normal unit vector associated with surface $A$. And for the potential energy : $U = - \vec{\mu} \cdot \vec{B} = - NIA\ \hat{\vec{n}} \cdot \vec{B}$ In this situation, $\vec{B} = B\ \vec{a}_y$ a) $\hat{\vec{n}} = \vec{a}_z$ so $\vec{\tau} = -NIAB \ \vec{a}_x$ and $U = 0$ b) $\hat{\vec{n}} = \vec{a}_y$ so $\vec{\tau} = \vec{0}$ and $U = -NIAB$ c) $\hat{\vec{n}} = -\vec{a}_z$ so $\vec{\tau} = NIAB \ \vec{a}_x$ and $U = 0$ d) $\hat{\vec{n}} = \vec{a}_z$ so $\vec{\tau} = \vec{0}$ and $U = NIAB$
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