University Physics with Modern Physics (14th Edition)

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

Chapter 8 - Momentum, Impulse, and Collision - Problems - Exercises - Page 268: 8.67

Answer

(a) $U_s = 5.25~J$ The velocity of each block at this time will be zero because all the energy of the system is stored in the springs. (b) Block A is moving 2.17 m/s to the left. Block B is moving 0.333 m/s to the right.

Work Step by Step

(a) The maximum energy stored in the springs will be equal to the kinetic energy of the two blocks. $U_s = K$ $U_s = \frac{1}{2}m_Av_A^2+\frac{1}{2}m_Bv_B^2$ $U_s = \frac{1}{2}(2.00~kg)(2.00~m/s)^2+\frac{1}{2}(10.00~kg)(0.500~m/s)^2$ $U_s = 5.25~J$ The velocity of each block at this time will be zero because all the energy of the system is stored in the springs. (b) Let $v_A'$ be the final velocity of block A. Let $v_B'$ be the final velocity of block B. Let $m_A = 2.00~kg$ and let $m_B = 10.00~kg$ We can use conservation of momentum to set up an equation. $m_A~v_A + m_B~v_B = m_A~v_A' + m_B~v_B'$ Since the collision is elastic, we can use equation (8.27) to set up another equation. $v_A - v_B = v_B' - v_A'$ $v_A' = v_B' - v_A + v_B$ We can use this expression for $v_A'$ in the first equation. $m_A~v_A + m_B~v_B = m_A~v_B' - m_Av_A + m_Av_B+ m_B~v_B'$ $v_B' = \frac{2m_A~v_A+m_B~v_B -m_Av_B}{m_A+m_B}$ $v_B’ = \frac{(2)(2.00~kg)(2.00~m/s)+(10.00~kg)(-0.500~m/s)- (2.00~kg)(-0.500~m/s)}{(2.00~kg)+(10.00~kg)}$ $v_B' = 0.333~m/s$ We can use $v_B'$ to find $v_A'$. $v_A' = v_B' - v_A + v_B$ $v_A' = 0.333~m/s - 2.00~m/s + (-0.500)~m/s$ $v_A' = -2.17~m/s$ Block A is moving 2.17 m/s to the left. Block B is moving 0.333 m/s to the right.
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