Rotational Energy
So far, we have covered kinetic energy, and
frictional energy. Since we have covered one more kind of dynamic to the cue
ball, we must consider the rotational energy.
Kt = (1/2)mv2
Fd = fkDx
Kr = (1/2)Iw2
When the ball is slipping it means that the ball is translating without any rotation.
Then when it begins not to slip, there is rotation however don't forget that there is
also its corresponding tangential velocity. The center of the ball, is not rotating
but rather simply translating in all cases. And in this special non-slip case, the
acceleration and the velocity of the center of mass is given by:
vcm = wR
acm = aR
Where R is the radius of the rotating object.
A cue ball is moving and slips for 5 meters then begins to roll without
slipping and there is zero net external force, how do we describe this using
conservation of energy?
Ei = (1/2)mvcm2 + fk(5)
Ef = (1/2)mvcm2 + (1/2)Iw2
The intial state of energy is given by the kinetic energy of translation and the mechanical
dissipation through friction. The final state of energy is given by the kinetic evergy of
the object's tangential velocity and its energy of rotation.
Sample Problem
A cue is slipping at 10rev/s for 10m and hits an object ball which was
initially at rest. The object ball begins to roll without slipping and the cue comes
to rest at moment of impact. What is the angular velocity of the object ball?
(mk = 0.25, R = 5cm and equal masses for both balls)