Ehrenfest's theorem states that as a quantum state evolves in time, th
e rate of change of the expectation value of momentum is equal to the
expectation value of the force. In the familiar ''particle-in-a-box,''
however, the probability of finding the particle at a wall-the only p
lace where forces act-is zero, so at first glance it appears that the
expectation value of the force should vanish for any state, which woul
d violate Ehrenfest's theorem. This argument is flawed, however, since
the forces at the walls of the box are infinite. We consider the box
as a limit of a very deep square well and confirm that Ehrenfest's the
orem emerges safe and sound. (C) 1996 American Association of Physics
Teachers.