Physics Technology Update (4th Edition)

Published by Pearson
ISBN 10: 0-32190-308-0
ISBN 13: 978-0-32190-308-2

Chapter 10 - Rotational Kinematics and Energy - Problems and Conceptual Exercises - Page 325: 37

Answer

(a) $v=0.30m/s$ (b) $1.5m/s^2$ (c) $0.15m/s$ (d) $0.75m/s^2$

Work Step by Step

(a) We know that $v=r\omega$ $v=(0.06m)(5.05rad/s)$ $v=0.30m/s$ (b) The centripetal acceleration is given as: $a_{cp}=r\omega^2$ We plug in the known values to obtain: $a_{cp}=(0.06m)(5.05rad/s)^2=1.5m/s^2$ (c) When the radius is reduced to half, the linear speed is also reduced to half $v=\frac{0.303m/s}{2}=0.15m/s$ As the centripetal acceleration is directly proportional to the radius of the CD, therefore, when the radius is reduced to half then the centripetal acceleration is also reduced to half. $\implies a_{cp}=\frac{1.53m/s^2}{2}$ $\implies a_{cp}=0.75m/s^2$
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