Physics for Scientists and Engineers: A Strategic Approach with Modern Physics (3rd Edition)

Published by Pearson
ISBN 10: 0321740904
ISBN 13: 978-0-32174-090-8

Chapter 12 - Rotation of a Rigid Body - Exercises and Problems - Page 353: 86

Answer

$ \frac{1}{5}v_0 $

Work Step by Step

The collision is perfectly elastic which means that the energy and the momentum are conserved. $$E_i=E_f$$ $$K_{i1}+K_{i2}=K_{f1}+K_{f2}$$ where $_1$ refers to the cube and $_2$ refers to the rod. $$ \color{red}{\bf\not}\frac{1}{2}mv_0^2+0= \color{red}{\bf\not}\frac{1}{2}mv_1^2+ \color{red}{\bf\not}\frac{1}{2}I_2\omega_2^2$$ $$ mv_0^2=mv_1^2+ I_2\omega_2^2$$ where $I_2$ rod is at its center of mass is given by $\frac{1}{12}ML^2$ $$ mv_0^2=mv_1^2+ \frac{1}{12}ML^2\omega_2^2$$ where $L=d$, and $M=2m$; $$ mv_0^2=mv_1^2+ \frac{1}{12}(2m)d^2\omega_2^2$$ $$ \color{red}{\bf\not}mv_0^2= \color{red}{\bf\not}mv_1^2+ \frac{1}{6} \color{red}{\bf\not}md^2\omega_2^2$$ $$ v_0^2= v_1^2+ \frac{1}{6} d^2\omega_2^2\tag 1$$ And, $$L_i=L_f$$ The linear momentum just before and just after the collision. $$mv_0\dfrac{d}{2}=mv_1\dfrac{d}{2}+I_2\omega_2$$ $$\dfrac{1}{2}mv_0d =\dfrac{1}{2} mv_1d +\frac{1}{12}ML^2 \omega_2$$ $$\dfrac{1}{2} \color{red}{\bf\not}mv_0 \color{red}{\bf\not}d =\dfrac{1}{2} \color{red}{\bf\not}mv_1 \color{red}{\bf\not}d +\frac{1}{12}(2 \color{red}{\bf\not}m)d^{ \color{red}{\bf\not}2} \omega_2$$ $$\dfrac{1}{2} v_0=\dfrac{1}{2} v_1+\dfrac{1}{6}d\omega_2 $$ $$ v_0= v_1+\dfrac{1}{3}d\omega_2 $$ $$ v_0- v_1=\dfrac{1}{3}d\omega_2 $$ Hence, $$ \dfrac{ 3(v_0- v_1)}{d}= \omega_2 $$ Plugging into (1); $$ v_0^2= v_1^2+ \frac{1}{6} d^2\left[ \dfrac{ 3(v_0- v_1)}{d} \right]^2 $$ $$ v_0^2= v_1^2+ \frac{1}{6} \color{red}{\bf\not}d^2 \dfrac{ 9(v_0- v_1)^2}{ \color{red}{\bf\not}d^2} $$ $$ v_0^2= v_1^2+ \dfrac{ 3(v_0- v_1)^2}{2 } $$ $$ 2 v_0^2=2 v_1^2+ 3(v_0^2-2v_0v_1 +v_1^2) $$ $$ 2 v_0^2=2 v_1^2+ 3 v_0^2-6v_0v_1 +3v_1^2 $$ $$ 5v_1^2-6v_0v_1+v_0^2 =0 $$ So that $$v_1=\dfrac{-b\pm\sqrt{b^2-4ac}}{2a}$$ where $a=5$, $b=-6v_0$, $c=v_0^2$ $$v_1=\dfrac{-(-6v_0)\pm\sqrt{(-6v_0)^2-(4\times 5\times v_0^2)}}{2\times 5}$$ $$v_1=\dfrac{ 6v_0 \pm\sqrt{36v_0^2-20 v_0^2}}{10}=\dfrac{6v_0 \pm 4v_0}{10}$$ whether $v_1=v_0$ which is rejected since it means that the rod will have no energy at all (the cube did not hit the rod at all). Or $$\boxed{v_1=\frac{1}{5}v_0}$$ Notice that both velocities are to the right.
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