University Physics with Modern Physics (14th Edition)

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

Chapter 6 - Work and Kinetic Energy - Problems - Exercises - Page 196: 6.31

Answer

(a) $d = \frac{v_0^2}{2~g~\mu_k}$ (b) (i) The minimum stopping distance $d$ would be halved. (ii) The minimum stopping distance $d$ would increase by a factor of 4. (iii) The minimum stopping distance $d$ would increase by a factor of 2.

Work Step by Step

(a) $W = K_2 - K_1$ $-F_f~d = 0-\frac{1}{2}mv_0^2$ $mg~\mu_k~d = \frac{1}{2}mv_0^2$ $d = \frac{v_0^2}{2~g~\mu_k}$ (b) We can use the minimum stopping distance $d = \frac{v_0^2}{2~g~\mu_k}$ to answer the following questions. (i) If $\mu_k$ doubled, then the stopping distance $d$ would be halved. (ii) If $v_0$ doubled, then the stopping distance $d$ would increase by a factor of 4. (iii) If both $\mu_k$ and $v_0$ doubled, then the stopping distance $d$ would increase by a factor of 2.
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