Fundamentals of Physics Extended (10th Edition)

Published by Wiley
ISBN 10: 1-11823-072-8
ISBN 13: 978-1-11823-072-5

Chapter 40 - All About Atoms - Problems - Page 1247: 12

Answer

$4.27\times 10^{-5}\;rad/s$

Work Step by Step

The iron sphere initially had no net magnetic moment. Under external magnetic field, the magnetic moment arises due to the spin angular momentum of the aligned loosely bound electrons. Each atom has one loosely bound electron. If $m$ be the mass of the sphere, then the number of loosely bound electrons in the iron is given by $n=\frac{mN_A}{M}$, where $N_A$ is the Avogadro's number and $M$ is the molar mass of iron. Thus, total As the field aligns $12\%$ of the loosely bound electrons, the total spin angular momentum of the loosely bound electrons is $L_e=\frac{0.12mN_A}{M}(m_s\hbar)$ If $I$ be the moment of inertia, and $\omega$ is the angular speed of the sphere, then the angular momentum of the sphere is $L_s=I\omega$ In the given condition, $L_s=L_e$ or, $I\omega=\frac{0.12mN_A}{M}(m_s\hbar)$ or, $\omega=\frac{0.12mN_A}{IM}(m_s\hbar)$ or, $\omega=\frac{0.12mN_A}{(\frac{2}{5}mR^2)M}(m_s\hbar)$ or, $\omega=\frac{0.6N_A}{2R^2M}(m_s\hbar)$ Substituting given values, $\omega=\frac{0.6\times 6.022\times 10^{23}}{2\times(0.002)^2\times0.0558}(\frac{1}{2}\times\frac{6.63\times10^{-34}}{2\pi})\;rad/s$ $\implies \omega\approx 4.27\times 10^{-5}\;rad/s$ $\therefore$ The angular speed of the sphere is $4.27\times 10^{-5}\;rad/s$.
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.