A uniform rod AB of length l, and mass m is free to rotate about point A. The rod is released from rest in the horizontal position. Given that the moment of inertia of the rod about A is \(\frac{ml^2}{3}\), the initial angular acceleration of the rod will be : |
\(\frac{mgl}{2}\) \(\frac{3}{2}gl\) \(\frac{3g}{2l}\) \(\frac{2g}{3l}\) |
\(\frac{3g}{2l}\) |
Weight of the rod will produce torque, \(\tau = mg × \frac{l}{2}\) Also, \(\tau = I\alpha\) and I = \(\frac{ml^2}{3}\) \(\frac{ml^2}{3} \alpha = mg × \frac{l}{2}\) \(\alpha = \frac{3g}{2l}\) |