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Question: Two identical masses A and B are on same vertical line. A is released from rest while B is simultane...

Two identical masses A and B are on same vertical line. A is released from rest while B is simultaneously projected upwards with a velocity of 50 m/s. Find the velocity of the combined mass just after collision considering perfectly inelastic collision. (g = 10 m/s²)

Answer

15 m/s

Explanation

Solution

To find the velocity of the combined mass just after the perfectly inelastic collision, we need to follow these steps:

  1. Determine the time when the two masses collide.
  2. Calculate the velocities of both masses just before the collision.
  3. Apply the principle of conservation of linear momentum for a perfectly inelastic collision.

Let's set up a coordinate system where the ground is at y=0y=0 and the upward direction is positive.

Given:

  • Initial height of A, yA0=50y_{A0} = 50 m.
  • Initial velocity of A, uA=0u_A = 0 m/s (released from rest).
  • Initial height of B, yB0=0y_{B0} = 0 m.
  • Initial velocity of B, uB=50u_B = 50 m/s (upwards).
  • Acceleration due to gravity, g=10g = 10 m/s².
  • Masses are identical, let mA=mB=mm_A = m_B = m.

Step 1: Determine the time of collision (t)

The position of mass A at time tt is given by:

yA(t)=yA0+uAt12gt2y_A(t) = y_{A0} + u_A t - \frac{1}{2}gt^2

yA(t)=50+(0)t12(10)t2y_A(t) = 50 + (0)t - \frac{1}{2}(10)t^2

yA(t)=505t2y_A(t) = 50 - 5t^2

The position of mass B at time tt is given by:

yB(t)=yB0+uBt12gt2y_B(t) = y_{B0} + u_B t - \frac{1}{2}gt^2

yB(t)=0+50t12(10)t2y_B(t) = 0 + 50t - \frac{1}{2}(10)t^2

yB(t)=50t5t2y_B(t) = 50t - 5t^2

The collision occurs when yA(t)=yB(t)y_A(t) = y_B(t):

505t2=50t5t250 - 5t^2 = 50t - 5t^2

50=50t50 = 50t

t=1t = 1 s

So, the collision occurs after 1 second.

Step 2: Calculate the velocities of A and B just before collision

The velocity of an object under constant acceleration is given by v=u+atv = u + at. Here, a=ga = -g (since upward is positive).

For mass A:

vA=uAgtv_A = u_A - gt

vA=0(10)(1)v_A = 0 - (10)(1)

vA=10v_A = -10 m/s (downwards)

For mass B:

vB=uBgtv_B = u_B - gt

vB=50(10)(1)v_B = 50 - (10)(1)

vB=40v_B = 40 m/s (upwards)

Step 3: Apply conservation of linear momentum

For a perfectly inelastic collision, the two masses stick together and move with a common final velocity, VfV_f. The total momentum before the collision equals the total momentum after the collision.

mAvA+mBvB=(mA+mB)Vfm_A v_A + m_B v_B = (m_A + m_B) V_f

Since mA=mB=mm_A = m_B = m:

m(10)+m(40)=(m+m)Vfm(-10) + m(40) = (m+m) V_f

10m+40m=2mVf-10m + 40m = 2m V_f

30m=2mVf30m = 2m V_f

Vf=30m2mV_f = \frac{30m}{2m}

Vf=15V_f = 15 m/s

The positive sign for VfV_f indicates that the combined mass moves upwards just after the collision.

The height at which collision occurs is yA(1)=505(1)2=45y_A(1) = 50 - 5(1)^2 = 45 m or yB(1)=50(1)5(1)2=45y_B(1) = 50(1) - 5(1)^2 = 45 m.

The velocity of the combined mass just after collision is 15 m/s upwards.

Explanation of the solution:

  1. Determine the time of collision by equating the position equations of masses A and B, considering their initial conditions and motion under gravity. This yields t=1t=1 s.
  2. Calculate the individual velocities of masses A and B just before collision using kinematic equations (v=ugtv = u - gt) at t=1t=1 s. vA=10v_A = -10 m/s (downwards) and vB=40v_B = 40 m/s (upwards).
  3. Apply the principle of conservation of linear momentum for a perfectly inelastic collision: mAvA+mBvB=(mA+mB)Vfm_A v_A + m_B v_B = (m_A + m_B) V_f. Since masses are identical (mA=mB=mm_A=m_B=m), substitute the values to find the final common velocity Vf=15V_f = 15 m/s.