A thin bar of mass M and length L is free to rotate about a fixed horizontal axis through a point at its end. The bar is brought to a horizontal position and then released. The angular velocity when it reaches the lowest point is :
Here ,
△v=mgl2△v=K.E=12Iω2=16ml2ω2=ml2ω26=mgl2⇒ω=√3gl∴ω∝1√l
and independent of m