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Question: Two particles A and B of mass 2m and m respectively are attached to the ends of a light inextensible...

Two particles A and B of mass 2m and m respectively are attached to the ends of a light inextensible string of length 4a which passes over a small smooth peg at a height 3a from an inelastic table. The system is released from rest with each particle at a height a from the table. Find

(i) The speed of B when A strikes the table. (ii) The time that elapses before A first hits the table. (iii) The time for which A is resting on the table after the first collision & before it is first jerked off.

Answer

i) 2ga3\sqrt{\frac{2ga}{3}} ii) 6ag\sqrt{\frac{6a}{g}} iii) 6ag\sqrt{\frac{6a}{g}}

Explanation

Solution

The problem describes a system of two masses connected by a string over a pulley. We need to analyze its motion in three parts.

System Setup:

  • Mass of particle A (mAm_A) = 2m
  • Mass of particle B (mBm_B) = m
  • Length of string = 4a
  • Height of the peg from the table = 3a
  • Initial height of each particle from the table = a
  • The system is released from rest.

Analysis of Initial State and Motion: Since both particles are initially at height 'a' and the peg is at '3a', the length of the string on A's side is (3a - a) = 2a, and on B's side is (3a - a) = 2a. The total string length is 2a + 2a = 4a, which is consistent with the given information. When particle A strikes the table, it falls a distance of 'a'. Consequently, particle B rises a distance of 'a'.

1. Calculate the acceleration of the system: Let T be the tension in the string and aa' be the acceleration of the system. For particle A (moving downwards): mAgT=mAam_A g - T = m_A a' 2mgT=2ma(1)2mg - T = 2m a' \quad (1)

For particle B (moving upwards): TmBg=mBaT - m_B g = m_B a' Tmg=ma(2)T - mg = m a' \quad (2)

Adding (1) and (2): (2mgT)+(Tmg)=2ma+ma(2mg - T) + (T - mg) = 2m a' + m a' mg=3mamg = 3m a' a=g3a' = \frac{g}{3}

Part (i): The speed of B when A strikes the table. Particle A falls a distance s=as = a. The initial velocity u=0u = 0. Using the kinematic equation v2=u2+2asv^2 = u^2 + 2a's: v2=02+2(g3)(a)v^2 = 0^2 + 2 \left(\frac{g}{3}\right) (a) v2=2ga3v^2 = \frac{2ga}{3} v=2ga3v = \sqrt{\frac{2ga}{3}}

Part (ii): The time that elapses before A first hits the table. Particle A falls a distance s=as = a. Initial velocity u=0u = 0. Using the kinematic equation s=ut+12at2s = ut + \frac{1}{2}a't^2: a=0t+12(g3)t2a = 0 \cdot t + \frac{1}{2} \left(\frac{g}{3}\right) t^2 a=g6t2a = \frac{g}{6} t^2 t2=6agt^2 = \frac{6a}{g} t=6agt = \sqrt{\frac{6a}{g}}

Part (iii): The time for which A is resting on the table after the first collision & before it is first jerked off.

  • Moment A strikes the table:

    • A comes to rest (velocity = 0).
    • B is moving upwards with velocity v=2ga3v = \sqrt{\frac{2ga}{3}}.
    • B's height from the table is now a+a=2aa + a = 2a.
    • At this instant, the string becomes slack as A is no longer pulling it.
  • Motion of B after A hits the table:

    • B continues to move upwards under gravity with initial velocity v=2ga3v = \sqrt{\frac{2ga}{3}} and acceleration aB=ga_B = -g.
    • Time for B to reach its highest point (t1t_1): Using vf=vi+aBt1v_f = v_i + a_B t_1: 0=2ga3gt10 = \sqrt{\frac{2ga}{3}} - g t_1 t1=1g2ga3=2a3gt_1 = \frac{1}{g} \sqrt{\frac{2ga}{3}} = \sqrt{\frac{2a}{3g}}
    • Height B rises further (s1s_1): Using vf2=vi2+2aBs1v_f^2 = v_i^2 + 2a_B s_1: 0=(2ga3)2+2(g)s10 = \left(\sqrt{\frac{2ga}{3}}\right)^2 + 2(-g) s_1 0=2ga32gs10 = \frac{2ga}{3} - 2g s_1 s1=a3s_1 = \frac{a}{3}
    • Maximum height of B from the table = 2a+a3=7a32a + \frac{a}{3} = \frac{7a}{3}.
  • B falls back down and the string becomes taut:

    • A is resting on the table (height 0). The peg is at height 3a.
    • For the string to become taut, the length of the string on A's side (from peg to A) is 3a.
    • Therefore, the length of the string on B's side (from peg to B) must be 4a3a=a4a - 3a = a.
    • This means B must fall until its height from the table is 'a'.
    • B starts falling from its maximum height 7a3\frac{7a}{3} with initial velocity u=0u=0.
    • Distance B needs to fall (s2s_2) = 7a3a=4a3\frac{7a}{3} - a = \frac{4a}{3}.
    • Time taken for B to fall this distance (t2t_2): Using s2=ut2+12gt22s_2 = ut_2 + \frac{1}{2}gt_2^2: 4a3=0+12gt22\frac{4a}{3} = 0 + \frac{1}{2} g t_2^2 t22=8a3gt_2^2 = \frac{8a}{3g} t2=8a3gt_2 = \sqrt{\frac{8a}{3g}}
  • Total time A is resting on the table: This is the sum of the time B takes to go up and come back down until the string is taut. Trest=t1+t2=2a3g+8a3gT_{rest} = t_1 + t_2 = \sqrt{\frac{2a}{3g}} + \sqrt{\frac{8a}{3g}} Trest=2a3g+42a3gT_{rest} = \sqrt{\frac{2a}{3g}} + \sqrt{4 \cdot \frac{2a}{3g}} Trest=2a3g+22a3gT_{rest} = \sqrt{\frac{2a}{3g}} + 2\sqrt{\frac{2a}{3g}} Trest=32a3g=92a3g=18a3g=6agT_{rest} = 3\sqrt{\frac{2a}{3g}} = \sqrt{9 \cdot \frac{2a}{3g}} = \sqrt{\frac{18a}{3g}} = \sqrt{\frac{6a}{g}}