$A$ massless rod of length $2l$ has equal point masses $m$ attached to its two ends as shown in the figure. The rod is rotating about an axis passing through its centre and making an angle $\alpha$ with the axis. The magnitude of the rate of change of angular momentum of the rod,i.e.,$\left|\frac{dL}{dt}\right|$,is equal to:

  • A
    $2ml^3\omega^2\sin\alpha\cos\alpha$
  • B
    $ml^2\omega^2\sin 2\alpha$
  • C
    $ml^2\sin 2\alpha$
  • D
    $m^{1/2}l^{1/2}\omega\sin\alpha\cos\alpha$

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