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MHT CET 2026 (19 May, Shift 2) · Angular Momentum & its Conservation

Angular Momentum & its Conservation question from MHT CET 2026 (19 May, Shift 2)

Q12MHT CET 2026 · 19 MAY · SHIFT 2Medium

Angular Momentum & its Conservation

A ring of mass MM and radius RR is rotating with angular speed ω\omega about a fixed vertical axis passing through its centre OO with two point masses each of mass M8\frac{M}{8} at rest at OO. These masses can move radially outwards along two mass-less rods fixed on the ring as shown in figure. At some instant the angular speed of the system is 8ω9\frac{8\omega}{9} and one of the masses is at a distance of 35R\frac{3}{5}R from point OO. At this instant, the distance of the other mass from point OO is

Figure

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Answer: (d)

  1. No external torque: Iiω=If⋅8ω9I_i\omega=I_f\cdot\frac{8\omega}{9}, with Ii=MR2I_i=MR^2 (masses at O).
  2. If=MR2+M8(3R5)2+M8x2=98MR2I_f=MR^2+\frac M8\left(\frac{3R}{5}\right)^2+\frac M8x^2=\frac98MR^2
  3. x28=R28−9R2200=16R2200⇒x2=16R225\frac{x^2}{8}=\frac{R^2}{8}-\frac{9R^2}{200}=\frac{16R^2}{200}\Rightarrow x^2=\frac{16R^2}{25}
  4. x=4R5x=\frac{4R}{5}, so the answer is (d).
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