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JEE Main 2020 (3 Sep, Shift 2) · Rotational Kinematics & Dynamics

Rotational Kinematics & Dynamics question from JEE Main 2020 (3 Sep, Shift 2)

Q50JEE Main 2020 · 3 SEP · SHIFT 2Difficult

Rotational Kinematics & Dynamics

A uniform rod of length ‘ll’ is pivoted at one of its ends on a vertical shaft of negligible radius. When the shaft rotates at angular speed ω\omega the rod makes an angle θ\theta with it (see figure). To find θ\theta equate the rate of change of angular momentum (direction going into the paper) ml212ω2sin⁡θcos⁡θ\frac{ml^{2}}{12}\omega^{2}\sin\theta\cos\theta about the centre of mass (CM) to the torque provided by the horizontal and vertical forces FH and FV about the CM. The value of θ\theta is then such that:

Figure

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Answer: (b)

  1. CM moves in a circle of radius l2sin⁡θ\tfrac{l}{2}\sin\theta: FV=mgF_V = mg, FH=mω2l2sin⁡θF_H = m\omega^2\tfrac{l}{2}\sin\theta.
  2. Torque about CM: FVl2sin⁡θ−FHl2cos⁡θ=ml212ω2sin⁡θcos⁡θF_V\tfrac{l}{2}\sin\theta - F_H\tfrac{l}{2}\cos\theta = \dfrac{ml^2}{12}\omega^2\sin\theta\cos\theta
  3. mgl2=mω2l2cos⁡θ(14+112)=mω2l2cos⁡θ3\dfrac{mgl}{2} = m\omega^2 l^2\cos\theta\left(\dfrac{1}{4} + \dfrac{1}{12}\right) = \dfrac{m\omega^2 l^2\cos\theta}{3}
  4. cos⁡θ=3g2lω2\cos\theta = \dfrac{3g}{2l\omega^2}, so the answer is (b).
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