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MHT CET 2024 (4 May, Shift 2) · Angular Momentum & its Conservation

Angular Momentum & its Conservation question from MHT CET 2024 (4 May, Shift 2)

Q29MHT CET 2024 · 4 MAY · SHIFT 2Medium

Angular Momentum & its Conservation

A thin uniform circular disc of mass ' MM ' and radius ' RR ' is rotating with angular velocity ' ω\omega ' in a horizontal plane about an axis passing through its centre and perpendicular to its plane. Another disc of same radius but of mass (M3)\left(\frac{M}{3}\right) is placed gently on the first disc co-axially. The new angular velocity will be

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Answer: (b)

  1. No external torque, so angular momentum is conserved: I1ω=(I1+I2)ω′I_1\omega = (I_1+I_2)\omega'.
  2. I1=12MR2I_1 = \frac{1}{2}MR^2, I2=12(M3)R2I_2 = \frac{1}{2}\left(\frac{M}{3}\right)R^2, so I1+I2=12⋅4M3R2I_1+I_2 = \frac{1}{2}\cdot\frac{4M}{3}R^2.
  3. ω′=M4M/3 ω=34ω\omega' = \frac{M}{4M/3}\,\omega = \frac{3}{4}\omega
  4. So the answer is (b) 34ω\frac{3}{4}\omega.
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