A uniform rod of length 2L is placed with one end in contact with horizontal and is then inclined at an angle $ \alpha $ to the horizontal and allowed to fall without slipping at contact point. When it becomes horizontal, its angular velocity will be…..
By Conservation of Energy P.E. of rod = Rotational K.E. $ M.g {1 \over 2} sin d = { 1 \over 2} I \omega^2 = { 1 \over 2} { mL^2 \over 3} \omega^2 $ $ \therefore \omega = \sqrt { 3 g sin \alpha \over L } $ As here l = 2 L $ \omega = \sqrt { 3g sin \alpha \over 2L } $