In this problem, we are dealing with a uniform rod of length \( l \) and mass \( m \) which is free to rotate about point \( A \) in a vertical plane. The task is to determine the initial angular acceleration of the rod given that the moment of inertia about \( A \) is \( \frac{ml^2}{3} \).
Let's analyze the forces acting on the rod when it is released from a horizontal position:
The torque \( \tau \) about point \( A \) due to the gravitational force is given by:
\(\tau = mg \cdot \frac{l}{2}\)
According to Newton's second law for rotation, the torque is also equal to the moment of inertia times angular acceleration, \( I \alpha \):
\(\tau = I \alpha\)
Substituting the given moment of inertia and torque:
\(mg \cdot \frac{l}{2} = \left(\frac{ml^2}{3}\right) \alpha\)
Simplifying this equation for angular acceleration \( \alpha \):
\(\alpha = \frac{mg \cdot \frac{l}{2}}{\frac{ml^2}{3}}\)
Finally, simplify the expression:
\(\alpha = \frac{3g}{2l}\)
Hence, the initial angular acceleration of the rod is \(\frac{3g}{2l}\), which corresponds to the first option provided. This is the correct answer.