Fundamentals of Physics Extended (10th Edition)

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

Chapter 15 - Oscillations - Problems - Page 443: 113c

Answer

$a = \frac{F}{m}$

Work Step by Step

We can find the angular acceleration about the center of mass due to the force $F$: $\tau = I \alpha$ $\frac{L}{6} F = (\frac{1}{12}mL^2) \alpha$ $\alpha = \frac{2F}{mL}$ We can find the linear acceleration at $O$ as a result of the angular acceleration: $a = \alpha~\frac{L}{2}$ $a = (\frac{2F}{mL}) (\frac{L}{2})$ $a = \frac{F}{m}$
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