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Inverse Collision

Now consider a situation which we could call an inverse collision in which two objects are initially at rest. For simplicity and because it does have some practical relevance we choose the one-dimensional case. An internal event causes the objects to separate and move with in general different final velocities tex2html_wrap_inline149 and tex2html_wrap_inline151. Clearly no external forces act on this system so momentum is conserved: and must remain zero at all times
equation7
This equation clearly is not enough to determine the velocities, we must know something about how much internal energy is converted to kinetic energy. We denote this energy tex2html_wrap_inline153 and requirement that as always energy is conserved gives us
equation12
We now have two equations with two unknowns from which we can determine the final velocities to be
eqnarray21
We cannot determine the directions but we now that they will be opposite. Note the beautiful symmetry in these expressions upon interchanging the indices. We certainly should require the physical situation is not changed by re-labeling the particles. I leave you to derive these expression your self. They become especially simple in the case where the objects have equal masses: tex2html_wrap_inline155
equation29
We will perform two experiments to illustrate the inverse collision





Collin Broholm
Tue Oct 14 11:55:58 EDT 1997