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: 10.22

Answer

(a) $a = 3.62~m/s^2$ $F_f = 4.83~N$ $\mu_s = 0.313$ (b) $a = 3.62~m/s^2$ $F_f = 9.66~N$ $\mu_s = 0.313$

Work Step by Step

(a) If the ball rolls without slipping, then $\alpha = \frac{a}{R}$. We can use a torque equation to find an expression for the force of static frction $F_f$. $\tau = I\alpha$ $F_f~R = (\frac{2}{3}mR^2)(\frac{a}{R})$ $F_f = \frac{2ma}{3}$ We can use this expression in the force equation for the ball as it moves down the slope. $\sum F = ma$ $mg~sin(\theta) - F_f = ma$ $mg~sin(\theta) - \frac{2ma}{3} = ma$ $\frac{5a}{3} = g~sin(\theta)$ $a = \frac{3g~sin(\theta)}{5}$ $a = \frac{(3)(9.80~m/s^2)~sin(38.0^{\circ})}{5}$ $a = 3.62~m/s^2$ We can use the acceleration to find the force of static friction. $F_f = \frac{2ma}{3}$ $F_f = \frac{(2)(2.00~kg)(3.62~m/s^2)}{3}$ $F_f = 4.83~N$ We can use the force of static friction to find the minimum coefficient of static friction. $F_f = 4.83~N$ $mg~cos(\theta)~\mu_s = 4.83~N$ $\mu_s = \frac{4.83~N}{mg~cos(\theta)}$ $\mu_s = \frac{4.83~N}{(2.00~kg)(9.80~m/s^2)~cos(38.0^{\circ})}$ $\mu_s = 0.313$ (b) Since the acceleration does not depend on mass, the acceleration would not change. $a = 3.62~m/s^2$ Since $F_f = \frac{2ma}{3}$, if the mass doubles, then the force of static friction doubles. $F_f = 2\times (4.83~N) = 9.66~N$ Since $\mu_s$ does not depend on the mass, the minimum value of $\mu_s$ is still $\mu_s = 0.313$.
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