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The Bowling ball

This is a favorite and a classic that I learned from Prof. Walker who taught this course for many years. Imagine throwing a bowling ball down a bowling alley at an initial velocity, tex2html_wrap_inline120 without any rotation. The forces acing on the ball are of the ''worst'' type : friction. Still you can actually determine exactly what will be the final velocity of the bowling ball using the conservation of angular momentum: We chose a point of reference about which friction has no torque which is any point in the floor and most convenient is a point that the ball passes immediately over as it skids/rolls. Initially the angular momentum of the ball is
equation45
in the final state where the ball rolls without sliding the angular momentum will be
equation47
Here we are using the very important equation for the angular momentum of an object which both is moving with translation as well as rotation. If tex2html_wrap_inline122 is the vector from the point of reference to the center of mass of the object then it can be shown that
equation50
This equation will be the cornerstone for us to use angular momentum in problems that involve rotation as well as translation.

Back to our problem, since there is no sliding in the final state we have the rolling relation :
equation56
so we can write :
equation58
since friction generates no torque about the floor we have
eqnarray60
We can even calculate exactly how much kinetic energy is dissipated by friction namely
equation62
I leave it as an exercise to derive this latter expression!



Collin Broholm
Mon Oct 27 12:07:57 EST 1997