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 228: 89

Answer

(a) $\alpha = \frac{3g}{2l}$ (b) $a = \frac{3g}{2}$

Work Step by Step

(a) We can use a torque equation to find the angular acceleration $\alpha$ of the rod. The torque is provided by gravity. Therefore, $\tau = I \alpha$ $r\cdot Mg = (\frac{1}{3}Ml^2)~\alpha$ $\alpha = \frac{3~r~g}{l^2} = \frac{(3)(l/2)(g)}{l^2}$ $\alpha = \frac{3g}{2l}$ (b) Now, we find the linear acceleration through the formula: $a = \alpha ~l = (\frac{3g}{2l}~rad/s^2)(l)$ $a = \frac{3g}{2}$
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