The free rod has the same mass and length as in part (a). There is no pivot. Put the rod's initial center of mass at and the impact end at . At impact the combined center of mass is
Conservation of momentum gives the combined center of mass velocity . Evaluate angular momentum about this combined center of mass; the incident ball's perpendicular lever arm is , so its initial magnitude is .
After the perfectly inelastic collision, the parallel axis theorem gives the combined moment of inertia
With negligible external angular impulse, conservation of angular momentum therefore gives
Its sense is that of the incident ball's angular momentum, clockwise in the source diagram. As a consistency check, the final kinetic energy is
Thus , or one fifth of the initial kinetic energy, is dissipated in sticking. Treating the rod's original centre as a fixed pivot would give an incorrect angular velocity.

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