Question:medium

A uniform rod of length l and mass m is free to rotate in a vertical plane about A. The rod initially in horizontal position is released. The initial angular acceleration of the rod is : (Moment of inertia of rod about A is \(\bigg(\frac{ml^2}{3}\bigg)\)

Updated On: Apr 28, 2026
  • \(\frac{3g}{2l}\)
  • \(\frac{2l}{3g}\)
  • \(\frac{3g}{2I^2}\)
  • mg\(\big(\frac{l}{2}\big)\)
Show Solution

The Correct Option is A

Solution and Explanation

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:

  1. The gravitational force \( mg \) acts vertically downward at the center of mass of the rod, which is at a distance \( \frac{l}{2} \) from point \( A \).
  2. Since the rod is free to rotate about point \( A \), we can apply the equation of rotational motion to find the initial angular acceleration \( \alpha \).

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.

Was this answer helpful?
0