University Physics with Modern Physics (14th Edition)

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

Chapter 14 - Periodic Motion - Problems - Exercises - Page 464: 14.70

Answer

(a) $f = 0.464~Hz$ $A = 0.343~m$ $T = 2.16~s$ (b) The time it takes for the system to return to the point of the collision is $1.08~s$

Work Step by Step

(a) We can use conservation of momentum to find the speed of the two blocks just after the collision. $(m+m)v_2 = mv_1$ $v_2 = \frac{v_1}{2}$ $v_2 = \frac{2.00~m/s}{2}$ $v_2 = 1.00~m/s$ Let $M$ be the the total mass of the two blocks. We can find the frequency. $f = \frac{1}{2\pi}~\sqrt{\frac{k}{M}}$ $f = \frac{1}{2\pi}~\sqrt{\frac{170.0~N/m}{20.0~kg}}$ $f = 0.464~Hz$ We can find the amplitude. $\frac{1}{2}kA^2 = \frac{1}{2}Mv_{max}^2$ $A = \sqrt{\frac{M}{k}}~v_{max}$ $A = \sqrt{\frac{20.0~kg}{170.0~N/m}}~(1.00~m/s)$ $A = 0.343~m$ We can find the period. $T = \frac{1}{f}$ $T = \frac{1}{0.464~Hz}$ $T = 2.16~s$ (b) For the system to return to the point of the collision, the blocks need to move through half of one cycle. We can find the time this takes. $t = \frac{T}{2} = \frac{2.16~s}{2} = 1.08~s$
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