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MHT CET 2024 (3 May, Shift 2) · Motion of Centre of Mass

Motion of Centre of Mass question from MHT CET 2024 (3 May, Shift 2)

Q4MHT CET 2024 · 3 MAY · SHIFT 2Medium

Motion of Centre of Mass

In projectile motion two particles of masses m1m_1 and m2m_2 have velocities V⃗1\vec{V}_1, and V⃗2\vec{V}_2 respectively at time t=0t = 0. Their velocities becomeV1′→\overrightarrow{V_1'}and V2′→\overrightarrow{V_2'} at time 2 t while still moving in air. The value of [(m1V1′→+m2V2′→)−(m1V⃗1+m2V⃗2)]\left[\left(m_1\overrightarrow{V_1'} + m_2\overrightarrow{V_2'}\right) - \left(m_1\vec{V}_1 + m_2\vec{V}_2\right)\right] is ( g=g = acceleration due to gravity)

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Answer: (d)

  1. The external force on the pair is (m1+m2)g(m_1+m_2)g downward, so Δp⃗=(m1+m2)g⃗ Δt\Delta\vec{p} = (m_1+m_2)\vec{g}\,\Delta t.
  2. The time interval is from 00 to 2t2t, so Δt=2t\Delta t = 2t.
  3. ∣Δp⃗∣=2(m1+m2)gt|\Delta\vec{p}| = 2(m_1+m_2)gt (directed downward).
  4. So the answer is (d) 2(m1+m2)gt2(m_1+m_2)gt.
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