University Physics with Modern Physics (14th Edition)

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

Chapter 10 - Dynamics of Rotational Motion - Problems - Exercises - Page 333: 10.60

Answer

The required force is 1300 N.

Work Step by Step

We can find the tension in the rope pulling up the crate. $\sum F = ma$ $T - mg = ma$ $T = m(g+a)$ $T = (50~kg)(9.80~m/s^2+1.40~m/s^2)$ $T = 560~N$ We can find the angular acceleration of the cylinder. $\alpha = \frac{a}{R}$ $\alpha = \frac{1.40~m/s^2}{0.25~m}$ $\alpha = 5.6~rad/s^2$ We can use the angular acceleration to find the required force $F$ on the crank. $\sum \tau = I \alpha$ $(F)(0.12~m) - T~R = I\alpha$ $F= \frac{I\alpha+T~R}{0.12~m}$ $F= \frac{(2.9~kg~m^2)(5.6~rad/s^2)+(560~N)(0.25~m)}{0.12~m}$ $F = 1300~N$ The required force is 1300 N.
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