The rod AB of length I and mass m can rotate freely about A in a vertical plane. A point mass m is
attached to the other end of the rod and the system is released from its horizontal position. The initial
angular acceleration is
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(i)τ=Iα
So,
2
mgl
=
3
1
ml
2
(α)
⇒α=
2l
3g
(ii) Tangential acceleration of point A=g
But as angular velocity of point is zero so, angular acceleration will be zero.
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