(3) \(\frac{MR^2ω^2_1}{4}\)
Fig shows cylinder with vertical string pulled up by a force F. As C.M of cylinder is at rest; F = Mg. The torque; \(\tau\) ; due to applied force about O is
\(\tau=F.R=MgR\)
The M.I of cylinder about its symmetry axis = I = \(\frac{MR^2}{2}\)
α = The angular accleration of cylinder = \(\frac{\tau}{1}=\frac{2g}{R}\)
Let ω be the total angle describe by cylinder as it accquires angular speed ω1 . Then