Because we are assuming that the collisions are mostly elastic, we have conservation of momentum and conservation of kinetic energy. When hitting the cue ball into another ball, we can use the equation mAvA = mAvA’ + mBvB’ with A being the cue ball and B being the ball it hit (at rest). Because the masses of the cue ball are the same as the other balls on the table, we can say that mA and mB are the same. Therefore, we have vA = vA’ + vB’.
Because we are assuming it is an elastic collision, kinetic energy is conserved, meaning that we have KEi = KEf . We can rewrite as ½ mA(vA)2 = ½ mA(vA’)2 + ½ mB(vB)2 . Again, because mA and mB are the same, we have (vA)2 = (vA’)2 + (vB’)2 .
Therefore, using the two equations above, we can draw the velocity vectors to form a triangle as shown below, except V1A is vA and V2A is vA’ and V2B is vB’.
As a result, ball A moves in a direction perpendicular to that of ball B after the collision, assuming that the collision is not head-on.
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