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Collisions

We want to use the conservation laws for linear momentum to study a fascinating and important type of physical phenomenon: collisions. What first comes to mind when we hear this word is two objects banging into each other, and this is the situation which we shall first consider. However as you will see tomorrow and in problems there are a large range of situations which we would not normally think of as collisions put which are in fact accounted for by similar considerations as work for the standard case of collision between two particles. Basically what we shall understand by a collision is

An event within an isolated system of particles in which internal forces dominate external forces over a specific limited period of time
Because we have stated that internal forces dominate the dynamics we have that
The total linear momentum is conserved in a collision: tex2html_wrap_inline229

First consider the simplest case of a collision between two particles denoted 1 and 2. We label properties of particles by their number and physical quantities which change in the collision by i and f for initial and final.

Because it is a collision linear momentum of the system consisting of both particles is conserved. Thus we write
equation10
for the momentum of the particles before the collision and
equation17
for the total momentum after the collision. We have
 eqnarray24
Note that as opposed to the energy conservation law momentum conservation in general produces a vector equation so we really have as many equations as dimensions in the collision problem. On the other hand there are also lots of unknowns. Say we know the initial conditions ie tex2html_wrap_inline231, and tex2html_wrap_inline233 but do not know the final velocities tex2html_wrap_inline235 and tex2html_wrap_inline237. Momentum conservation produces half the number of equations we need so more information will be necessary. We get one more equation from the requirement that energy is conserved
equation45
Here I introduced tex2html_wrap_inline239 which is the increase in the internal energy of the system following the collision. If I am in one dimension and I know tex2html_wrap_inline239 then I have two equations with two unknown. As soon as I go to higher dimensions I still do not have enough equations to figure out what happens after a collision with known initial parameters.

We consider simple examples first:




next up previous
Next: Common velocity after collision Up: No Title Previous: No Title

Collin Broholm
Wed Oct 8 10:04:19 EDT 1997