University Physics with Modern Physics (14th Edition)

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

Chapter 9 - Rotation of Rigid Bodies - Problems - Exercises - Page 299: 9.77

Answer

(a) $I = 0.00225~kg~m^2$ (b) $v = 3.40~m/s$ (c) $v = 4.95~m/s$ The final speed is greater when the string is farther away from the axis of rotation since it is easier for the tension in the string to rotate the disks. Because the tension in the string decreases, the final speed of the block increase

Work Step by Step

(a) $I = \frac{1}{2}M_1R_1^2+\frac{1}{2}M_2R_2^2$ $I = \frac{1}{2}(0.80~kg)(0.0250~m)^2+\frac{1}{2}(1.60~kg)(0.0500~m)^2$ $I = 0.00225~kg~m^2$ (b) The kinetic energy of the block and the disks will be equal to the magnitude of the change in potential energy. $KE = PE$ $\frac{1}{2}mv^2+\frac{1}{2}I\omega^2 = mgh$ $mv^2+I(\frac{v}{R_1})^2 = 2mgh$ $v^2 = \frac{2mgh}{m+\frac{I}{R_1^2}}$ $v = \sqrt{\frac{2mgh}{m+\frac{I}{R_1^2}}}$ $v = \sqrt{\frac{(2)(1.50~kg)(9.80~m/s^2)(2.00~m)}{1.50~kg+\frac{0.00225~kg~m^2}{(0.0250~m)^2}}}$ $v = 3.40~m/s$ (c) The kinetic energy of the block and the disks will be equal to the magnitude of the change in potential energy. $KE = PE$ $\frac{1}{2}mv^2+\frac{1}{2}I\omega^2 = mgh$ $mv^2+I(\frac{v}{R_2})^2 = 2mgh$ $v^2 = \frac{2mgh}{m+\frac{I}{R_2^2}}$ $v = \sqrt{\frac{2mgh}{m+\frac{I}{R_2^2}}}$ $v = \sqrt{\frac{(2)(1.50~kg)(9.80~m/s^2)(2.00~m)}{1.50~kg+\frac{0.00225~kg~m^2}{(0.0500~m)^2}}}$ $v = 4.95~m/s$ The final speed is greater when the string is farther away from the axis of rotation since it is easier for the tension in the string to rotate the disks. Because the tension in the string decreases, the final speed of the block increases.
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