A mass m travels in a straight line with velocity v0 perpendicular to a uniform stick of mass m and length L, which is initially at rest. The distance from the centre of the stick to the path of the travelling mass is h (see figure). Now the travelling mass m collides elastically with the stick, and the centre of the stick and the mass m are observed to move with equal speed v after the collision. Assuming that the travelling mass m can be treated as a point mass, it follows that the distance h must be
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mv0 = 2mv
v =
mv0h = mvh +
⟹ h = ω
e = 1 = ⟹ v0 = ωh
= ⟹ h =
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