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: 6.26

Answer

(a) W = mgh (b) $v = \sqrt{2gh}$ (c) v = 17.1 m/s

Work Step by Step

(a) The component of gravity parallel to the plane is $mg~sin(\alpha)$. The work done is $mg~sin(\alpha)~d$, where $d$ is the distance along the plane. Note that $d = \frac{h}{sin(\alpha)}$. Then: $W = mg~sin(\alpha)~d$ $W = mg~sin(\alpha)\frac{h}{sin(\alpha)}$ $W = mgh$ The component of gravity perpendicular to the plane is $mg~cos(\alpha)$. Since it is perpendicular to the direction of motion, the work done is zero. The total work done by gravity is $W = mgh$, which is the same as if the mass had fallen straight down from a height of $h$. (b) $KE_1 + W = KE_2$ $0 + mgh = \frac{1}{2}mv^2$ $v = \sqrt{2gh}$ Since the work done by gravity does not depend on the angle $\alpha$, the amount of kinetic energy at the bottom only depends on the height $h$. Thus the speed at the bottom does not depend on the angle $\alpha$. (c) $v = \sqrt{2gh}$ $v = \sqrt{(2)(9.80~m/s^2)(15.0~m)}$ $v = 17.1~m/s$
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