2010: Problem 14

Topic: Collisions
Concepts: 1D elastic collision, Energy dissipation


Solution:

By conservation of energy, the velocity of m1m_1 when it reaches m2m_2 is

12m1v12=12m1v12μm1gd\frac{1}{2}m_1v_1’^2=\frac{1}{2}m_1v_1^2-\mu m_1gd
v1=v122μgdv_1’=\sqrt{v_1^2-2\mu gd}

Using the elastic collision equation, the velocity of m2m_2 right after the collision is

v2=2m1m1+m2v1v_2=\frac{2m_1}{m_1+m_2}v_1′

We conserve energy again to find how far m2m_2 slides:

12m2v22=μm2gd2\frac{1}{2}m_2v_2^2=\mu m_2gd_2
d2=v222μg=12μg(2m1m1+m2)2(v122μgd)=4m12(m1+m2)2(v122μgd)=1.79md_2=\frac{v_2^2}{2\mu g}=\frac{1}{2\mu g}\left(\frac{2m_1}{m_1+m_2}\right)^2(v_1^2-2\mu gd)=\frac{4m_1^2}{(m_1+m_2)^2}\left(\frac{v_1^2}{2\mu g}-d\right)=1.79\,\mathrm{m}

so the answer is B.

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