Question:

A thin uniform rod of length ll and mass mm is swinging freely about a horizontal axis passing through its end. Its maximum angular speed is ω\omega. Its centre of mass rises to a maximum height of

Updated On: Jul 27, 2022
  • 132ω2g\frac{1}{3} \frac{\ell^{2}\omega^{2}}{g}
  • 16ωg\frac{1}{6} \frac{\ell\omega}{g}
  • 122ω2g\frac{1}{2} \frac{\ell^{2}\omega^{2}}{g}
  • 162ω2g\frac{1}{6} \frac{\ell^{2}\omega^{2}}{g}
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The Correct Option is D

Solution and Explanation

T.Ei=T.EfT.E_{i}=T.E_{f} 12Iω2=mgh\frac{1}{2}I\omega^{2}=mgh 12×13m2ω2=mghh=162ω2g\frac{1}{2}\times\frac{1}{3}m\ell^{2}\omega^{2}=mgh \Rightarrow h=\frac{1}{6} \frac{\ell^{2}\omega^{2}}{g}
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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.