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 330: 10.14

Answer

(a) $T = 42.0~N$ (b) $v = 11.8~m/s$ (c) $t = 1.69~s$ (d) $F = 160~N$

Work Step by Step

(a) We can set up an equation for the cylinder. Let $m_c$ be the mass of the cylinder. $\tau = I\alpha$ $TR = \frac{1}{2}m_cR^2(\frac{a}{R})$ $a = \frac{2T}{m_c}$ We can use this expression in the force equation for the bucket. Let $m_b$ be the mass of the bucket. $m_bg-T = m_ba$ $m_bg-T = m_b(\frac{2T}{m_c})$ $m_c~m_bg-m_cT = 2m_bT$ $T = \frac{m_c~m_bg}{2m_b+m_c}$ $T = \frac{(15.0~kg)(12.0~kg)(9.80~m/s^2)}{(2)(15.0~kg)+12.0~kg}$ $T = 42.0~N$ (b) We can find the acceleration. $a = \frac{2T}{m_c}$ $a = \frac{(2)(42.0~N)}{12.0~kg}$ $a = 7.00~m/s^2$ We can find the speed after the bucket falls 10.0 meters. $v^2=v_0^2+2ay = 0 +2ay$ $v = \sqrt{2ay} = \sqrt{(2)(7.00~m/s^2)(10.0~m)}$ $v = 11.8~m/s$ (c) We can find the time to fall 10.0 meters. $y = \frac{1}{2}at^2$ $t = \sqrt{\frac{2y}{a}}$ $t = \sqrt{\frac{(2)(10.0~m)}{7.00~m/s^2}}$ $t = 1.69~s$ (d) The upward force exerted by the axle on the cylinder is equal in magnitude to the sum of the cylinder's weight and the tension pulling downward on the cylinder. $F = m_cg+T$ $F = (12.0~kg)(9.80~m/s^2)+42.0~N$ $F = 160~N$
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.