Torque, \(\tau = I\alpha = \frac{{M{L^2}}}{3}\alpha \,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,\,...\left( i \right)\)
(Momentum of inertia of the rod about one end = \(\frac{{M{l^2}}}{3}\))
Also, \(\tau = Mg\frac{L}{2}\) \( ...(ii)\)
Equating \((i)\) and \((ii)\), we get
\(Mg\frac{L}{2} = \frac{{M{L^2}}}{3}\alpha \,\,or\,\,\alpha = \frac{{3g}}{{2L}}\)