MCQMediumJEE 2025Elastic & Inelastic Collisions

JEE Physics 2025 Question with Solution

As shown below, bob A of a pendulum having massless string of length RR is released from 6060^\circ to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take gg as acceleration due to gravity):

Pendulum bob A of mass m suspended from a fixed support by a string, released from 60 degrees to the vertical, striking bob B of mass m/2 resting on a frictionless horizontal table at the center.
  • A

    13Rg\frac{1}{3} \sqrt{Rg}

  • B

    Rg\sqrt{Rg}

  • C

    23Rg\frac{2}{3} \sqrt{Rg}

  • D

    43Rg\frac{4}{3} \sqrt{Rg}

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: Bob A of mass mm is released from 6060^\circ to the vertical on a pendulum of length RR. Bob B has mass m2\frac{m}{2} and is initially at rest. The collision is elastic.

Find: The magnitude of velocity of bob A after collision.

First find the speed of A just before collision using conservation of mechanical energy. The vertical drop from 6060^\circ is RRcos60=R2R - R\cos 60^\circ = \frac{R}{2}, so

u2=2g(R2)=gRu^2 = 2g\left(\frac{R}{2}\right) = gR

Hence, the speed just before impact is

u=gRu = \sqrt{gR}

Let the velocities of A and B just after collision be v1v_1 and v2v_2 respectively.

Using conservation of momentum along the line of impact,

mν=mv1+m2v2m\nu = mv_1 + \frac{m}{2}v_2

which gives

2v1+v2=2ν...(i)2v_1 + v_2 = 2\nu \qquad \text{...(i)}

Since the collision is elastic, coefficient of restitution e=1e = 1. Therefore,

e=v2v1ν=1e = \frac{v_2 - v_1}{\nu} = 1

so

v2v1=ν...(ii)v_2 - v_1 = \nu \qquad \text{...(ii)}

From equation (ii)\text{(ii)},

v2=v1+νv_2 = v_1 + \nu

Substitute into equation (i)\text{(i)}:

2v1+(v1+ν)=2ν2v_1 + (v_1 + \nu) = 2\nu 3v1=ν3v_1 = \nu v1=ν3v_1 = \frac{\nu}{3}

Now substitute ν=gR\nu = \sqrt{gR}:

v1=13gRv_1 = \frac{1}{3}\sqrt{gR}

Therefore, the magnitude of velocity of bob A after collision is 13gR\frac{1}{3}\sqrt{gR}. The correct option is A.

The solution's lists option C in the answer key, but the extracted solution working and final boxed result give 13gR\frac{1}{3}\sqrt{gR}, so the solution has been followed.

Energy and restitution breakdown

Given: The pendulum bob starts from rest at 6060^\circ to the vertical and strikes a lighter bob at the lowest point.

Find: Speed of bob A after an elastic collision.

The height fallen by bob A is obtained from geometry:

h=RRcos60h = R - R\cos 60^\circ h=RR2=R2h = R - \frac{R}{2} = \frac{R}{2}

So just before collision,

mgh=12mν2mgh = \frac{1}{2}m\nu^2 mg(R2)=12mν2mg\left(\frac{R}{2}\right) = \frac{1}{2}m\nu^2 ν2=gR\nu^2 = gR ν=gR\nu = \sqrt{gR}

Now apply the two collision relations:

  1. Momentum conservation:
mν=mv1+m2v2m\nu = mv_1 + \frac{m}{2}v_2
  1. Elastic collision condition:
v2v1=νv_2 - v_1 = \nu

These two equations are sufficient to determine v1v_1 and v2v_2.

Multiply the momentum equation by 2m\frac{2}{m}:

2ν=2v1+v22\nu = 2v_1 + v_2

Using v2=v1+νv_2 = v_1 + \nu,

2ν=2v1+v1+ν2\nu = 2v_1 + v_1 + \nu ν=3v1\nu = 3v_1 v1=ν3=13gRv_1 = \frac{\nu}{3} = \frac{1}{3}\sqrt{gR}

Hence, bob A moves after collision with speed 13gR\frac{1}{3}\sqrt{gR}.

Common mistakes

  • Using the initial potential energy drop as mgRmgR instead of mgR2mg\frac{R}{2}. This is wrong because the bob is released from 6060^\circ to the vertical, so the actual drop is R(1cos60)=R2R(1-\cos 60^\circ) = \frac{R}{2}. Always compute the vertical height change from geometry first.

  • Applying only conservation of momentum and ignoring elasticity. Momentum alone gives one equation with two unknown final speeds. For an elastic collision, also use e=1e=1 or equivalently the relative speed condition.

  • Writing the restitution equation with the wrong sign, such as v1v2=νv_1 - v_2 = \nu. This is incorrect because coefficient of restitution uses speed of separation over speed of approach along the line of impact, giving v2v1=νv_2 - v_1 = \nu here.

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