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 266: 8.49

Answer

(a) After the collision, the speed of the neutron is $\frac{v_A}{3}$, where $v_A$ was the original speed. (b) $K_2 = \frac{K_1}{9}$ (c) Ten collisions should reduce the speed of a neutron to 1/59000 of its original value.

Work Step by Step

Let $v_A'$ be the final velocity of the neutron. Let $v_B'$ be the final velocity of the deuteron. Let $m_A = 1u$ and let $m_B = 2u$ We can use conservation of momentum to set up an equation. $m_A~v_A + 0 = m_A~v_A' + m_B~v_B'$ Since the collision is elastic, we can use equation (8.27) to set up another equation. $v_A - 0 = v_B' - v_A'$ $v_A' = v_B' - v_A$ We can use this expression for $v_A'$ in the first equation. $m_A~v_A + 0 = m_A~v_B' - m_Av_A + m_B~v_B'$ $v_B' = \frac{2m_A~v_A}{m_A+m_B}$ $v_B' = \frac{(2)(1u)(v_A)}{(1u)+(2u)}$ $v_B' = \frac{2v_A}{3}$ We can use $v_B'$ to find $v_A'$. $v_A' = v_B' - v_A$ $v_A' = \frac{2v_A}{3} - v_A = \frac{-v_A}{3}$ After the collision, the speed of the neutron is $\frac{v_A}{3}$, where $v_A$ was the original speed. (b) $K_1 =\frac{1}{2}uv_A^2$ $K_2 = \frac{1}{2}u(\frac{v_A}{3})^2$ $K_2 = \frac{1}{9}\times \frac{1}{2}uv_A^2$ $K_2 = \frac{K_1}{9}$ (c) $(\frac{1}{3})^n = \frac{1}{59000}$ $3^n = 59000$ $n~ln(3)= ln(59000)$ $n = \frac{ln(59000)}{ln(3)}$ $n = 10.0$ Ten collisions should reduce the speed of a neutron to 1/59000 of its original value.
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