A uniform rod of mass and length is falling freely with it's center of mass moving with a velocity and both the ends horizontal, without any form of rotational motion. One of it's ends suddenly gets hinged and the rod starts rotating about that end.
If the angular speed with which the rod starts rotating is , find .
Neglect air resistance and friction at the hinge also take .
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Though there is torque of gravity, the duration of impact of hinging about one end is almost negligible hence, the angular momentum about that point is conserved. Using this fact,
L = I ω ⟹ m v 2 l = 3 m l 2 ⋅ ω ⟹ ω = 2 l 3 v