A linear chain of atoms, interacting with anharmonic forces, one of wh
ose end atoms is forced to vibrate harmonically, is studied as a simpl
e model for kinetic friction between ideal crystalline solids. It is f
ound that there is a transition, as a function of chain length and dri
ving frequency between a regime in which there is dissipation (i.e., t
he internal energy increases as a function of time on the average) and
one in which there is practically no dissipation. This suggests that
there can be dissipationless sliding for sufficiently small solids.