9-2 할리데이 11판 솔루션 일반물리학

$$ \put \begin{cases} A:m_1\\ B:m_2\\ C:m_3\\ \end{cases} $$ $$ \put \begin{cases} 0:\text{Start}\\ 1:\text{After A,B Crash}\\ 2:\text{After B,C Crash}\\ \end{cases} $$ $$ \begin{cases} m_A&=4m\\ m_B&=0.500m_A=2m\\ m_C&=0.500m_B=m \end{cases} $$ $$ \begin{cases} v_{A0}&=2.00\ut{m/s}\\ v_{B0}&=0\\ v_{C0}&=0\\ \end{cases} $$ $$\Delta \Sigma \vec P=0,$$ $$ \text{Elastic Collision}\Harr\vec v_{\text{in}}+ \vec v_{\text{out}}=0,$$ $$\vec v_{Ai}-\vec v_{Bi}+ \vec v_{Af}-\vec v_{Bf}=0,$$ $$ \begin{cases} \vec P_{Ai}+\vec P_{Bi}&=\vec P_{Af}+\vec P_{Bf}\\ \vec v_{Ai}+\vec v_{Af}&=\vec v_{Bi}+\vec v_{Bf}\\ \end{cases} $$ $$ \begin{cases} \vec P_{Ai}&=\vec P_{Af}+\vec P_{Bf}\\ \vec v_{Ai}+\vec v_{Af}&=\vec v_{Bf}\\ \end{cases} $$ $$ \begin{cases} m_A\vec v_{Ai}&=m_A\vec v_{Af}+m_B\vec v_{Bf}\\ \vec v_{Ai}+\vec v_{Af}&=\vec v_{Bf}\\ \end{cases} $$ $$ \therefore \begin{cases} \vec v_{Af}&=\cfrac{m_A-m_B}{m_A+m_B}\vec v_{Ai}\\ \vec v_{Bf}&=\cfrac{2m_A}{m_A+m_B}\vec v_{Ai}\\ \end{cases} $$ $$\ab{a}$$ $$ \begin{aligned} \vec v_{B1}&=\frac{2m_A}{m_A+m_B}\vec v_{A0}\\ &=\frac{2\cdot 4m}{4m+2m}\vec v_{A0}\\ &=\frac{4}{3}\vec v_{A0} \end{aligned} $$ $$ \begin{aligned} \vec v_{C2}&=\frac{2m_B}{m_B+m_C}\vec v_{B1}\\ &=\frac{2\cdot 2m}{2m+m}\cdot\(\frac{4}{3}\vec v_{A0}\)\\ &=\frac{16}{9}\vec v_{A0}\\ &=\frac{32}{9}\ut{m/s}\\ &\approx 3.5555555555555554\ut{m/s}\\ &\approx 3.56\ut{m/s}\\ \end{aligned} $$ $$\ab{b-1}$$ $$v_{C2} \gt v_{A0}~~\(\because v_{C2}=\frac{16}{9}\vec v_{A0}\)$$ $$\ab{b-2}$$ $$ \begin{aligned} \KE_{C2}&=\frac{1}{2}m_C{v_{C2}}^2\\ &=\frac{1}{2}(m)\(\frac{16}{9}\vec v_{A0}\)^2\\ &=\frac{64}{81}\(\frac{1}{2}\cdot 4m\cdot {v_{A0}}^2\)\\ &=\frac{64}{81}\KE_{A0} \end{aligned} $$ $$\therefore \KE_{C2} \lt \KE_{A0}$$ $$\ab{b-3}$$ $$ \begin{aligned} \vec P_{C2}&=m_Cv_{C2}\\ &=(m)\(\frac{16}{9}\vec v_{A0}\)\\ &=\frac{4}{9}\(4m\cdot \vec v_{A0}\)\\ &=\frac{4}{9}\vec P_{A0}\\ \end{aligned} $$ $$\therefore \vec P_{C2} \lt \vec P_{A0}$$