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Physics · Ch 4 — Work, Energy and Power

Collisions

4.4

Collisions

A collision is any brief, forceful interaction between two (or more) bodies -- carom, billiards and marbles are everyday examples -- and collisions can happen with or without the bodies physically touching (e.g. two charged particles or two planets can "collide" gravitationally/electrically without contact).

Linear momentum is always conserved in every collision. During the brief collision time Δt\Delta t, the first body exerts an impulsive force F⃗12\vec F_{12} on the second, and by Newton's third law the second body exerts an equal and opposite force F⃗21=−F⃗12\vec F_{21} = -\vec F_{12} on the first. Each force produces a change of momentum in the body it acts on:

Δp⃗1=F⃗12 Δt,Δp⃗2=F⃗21 Δt\Delta \vec p_1 = \vec F_{12}\,\Delta t, \qquad \Delta \vec p_2 = \vec F_{21}\,\Delta t

Adding these two equations and using F⃗12=−F⃗21\vec F_{12}=-\vec F_{21} gives Δp⃗1+Δp⃗2=0\Delta \vec p_1 + \Delta \vec p_2 = 0, i.e. Δ(p⃗1+p⃗2)=0\Delta(\vec p_1+\vec p_2)=0. Taking the limit Δt→0\Delta t \to 0, this says the total momentum of the two-body system does not change during the collision:

p⃗1+p⃗2=constant\vec p_1 + \vec p_2 = \text{constant} …