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 334: 10.67

Answer

$a = \frac{2gb^2}{2b^2+R^2}$ $\alpha =\frac{2gb}{2b^2+R^2}$ $T = \frac{2mgR^2}{2b^2+R^2}$

Work Step by Step

We can set up a torque equation for the yo-yo. $\tau = I\alpha$ $T~b = (\frac{1}{2}mR^2+\frac{1}{2}mR^2)(\frac{a}{b})$ $T = \frac{mR^2a}{b^2}$ We can use this expression in the force equation for the yo-yo. $\sum F = (2m)~a$ $2mg - T = 2ma$ $2mg = 2ma+ \frac{mR^2a}{b^2}$ $2gb^2 = 2ab^2+ R^2a$ $a = \frac{2gb^2}{2b^2+R^2}$ We can use the acceleration $a$ to find the angular acceleration. $\alpha = \frac{a}{b}$ $\alpha =\frac{2gb}{2b^2+R^2}$ We can find the tension in the string. $T = \frac{mR^2a}{b^2}$ $T = (\frac{mR^2}{b^2})(\frac{2gb^2}{2b^2+R^2})$ $T = \frac{2mgR^2}{2b^2+R^2}$
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