(a) As the mass is concentrated at the centre of the rod, therefore,
$mg \times \frac{l}{2} = \frac{1}{2}I\omega^{2} = \frac{1}{2}\left( \frac{ml^{2}}{3} \right)\omega^{2}$
or $l^{2}\omega^{2} = 3gl$
[image:7_image104.emf]
Velocity of other end of the rod
$v = l\omega = \sqrt{3gl}$