Theory of Intelligence
11TH•Physics•Force And Motion•Inelastic Collision in Two Dimensions

2.11 Inelastic Collision in Two Dimensions

Stick-together collisions in a plane, kinetic-energy loss, and everyday examples.

2.11 Inelastic Collision in Two Dimensions

The macroscopic collisions are generally inelastic and do not conserve Kinetic energy.

The perfect inelastic collision is one in which the colliding objects stick together to make a single mass after collision. Its analysis can be carried out as follows:

Let us take two balls having masses m1m_{1} and m2m_{2} moving with velocities, v1v_{1} and v2v_{2}, respectively, in a two-dimensional xyxy-plane. Assume that the first body is moving along the xx-axis while the second body moves in a direction, making an angle θ\theta with xx-axis. Both the bodies collide at the origin as shown in the figure 2.17.

After collision, bodies stick together, having combined mass M=m1+m2M = m_{1} + m_{2}, which moves with velocity vv, making an angle ϕ\phi with xx-axis.

Momentum in the xx-direction:

m1v1+m2v2cos⁡θ=Mvcos⁡ϕ…(2.38)m_{1}v_{1} + m_{2}v_{2}\cos\theta = Mv\cos\phi \quad \ldots (2.38)

Momentum in the yy-direction:

0+m2v2sin⁡θ=Mvsin⁡ϕ…(2.39)0 + m_{2}v_{2}\sin\theta = Mv\sin\phi \quad \ldots (2.39)

Equation 2.38 and 2.39 can be used to find the final velocity.

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