Question:

A thin rod of mass $m$ and length $2l$ is made to rotate about an axis passing through its centre and perpendicular to it. If its angular velocity changes from $0$ to $\omega$ in time $t$, the torque acting on it is

Updated On: Jul 6, 2022
  • $\frac{ml^2 \omega}{12 t}$
  • $\frac{ml^2 \omega}{3 t}$
  • $\frac{ml^2 \omega}{t}$
  • $\frac{4ml^2 \omega}{3 t}$
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The Correct Option is B

Solution and Explanation

since $\tau=l \alpha$ so,$\tau=\left[\frac{m(2l)^2}{12}\right]\left(\frac{\omega}{t}\right) \,or\,\tau =\frac{m \times 4 l^2 \times \omega }{12 \times t}$ or $\tau=\frac{4ml^2 \omega}{12t}=\left(\frac{ml^2\omega}{3t}\right)$
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Concepts Used:

System of Particles and Rotational Motion

  1. The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
  2. The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.