Physics: Principles with Applications (7th Edition)

Published by Pearson
ISBN 10: 0-32162-592-7
ISBN 13: 978-0-32162-592-2

Chapter 8 - Rotational Motion - General Problems - Page 227: 80

Answer

The torque required is $\tau = 2.1~m\cdot N$. The torque comes from the muscles of David's body acting on the end of the sling in David's hand.

Work Step by Step

$\omega = (75~rpm)(2\pi \frac{rad}{rev})(\frac{1~m}{60~s}) = 2.5~\pi~rad/s$ We can find the angular acceleration $\alpha$: $\alpha = \frac{\omega}{t} = \frac{2.5\pi~rad/s}{5.0~s}$ $\alpha = \frac{\pi}{2.0}~rad/s^2$ We can find the torque required to produce the acceleration: $\tau = I \alpha = ((0.60~kg)\cdot (1.5~m)^2)( \frac{\pi}{2.0}~rad/s^2)$ $\tau = 2.1~m\cdot N$ The torque required is $\tau = 2.1~m\cdot N$. The torque comes from the muscles of David's body acting on the end of the sling in David's hand.
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