University Physics with Modern Physics (14th Edition)

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

Chapter 5 - Applying Newton's Laws - Problems - Exercises - Page 164: 5.58

Answer

(a) $a = 4.64~m/s^2$ (upward) (b) $T = 105~N$

Work Step by Step

(a) $a = \frac{v^2}{r} = \frac{(4.20~m/s)^2}{3.80~m}$ $a = 4.64~m/s^2$ The magnitude of the acceleration is $a = 4.64~m/s^2$. Since the ball is moving in a circle and there is no tangential acceleration at the bottom point, the acceleration is directed straight up toward the middle of the circle. (b) We can find the tension $T$ in the rope. $\sum F = \frac{mv^2}{r}$ $T - mg = \frac{mv^2}{r}$ $T = \frac{mv^2}{r} + mg$ $T = \frac{(71.2~N)(4.20~m/s)^2}{(9.80~m/s^2)(3.80~m)} + 71.2~N$ $T = 105~N$
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