It is shown that for a collection of n classical harmonic oscillators, the
long-time distribution of potential energies P is approximated by sin(m)(pi
P) for n greater than or equal to 4, where m=(8n/pi(2)-1/root 2) and P is
scaled to lie between 0 and 1. As n-->infinity, the distribution tends to a
delta-function centered about P=0.5. When coupling is present between the
oscillators, the effective value of m is reduced, so that the breadth of th
e potential energy distribution reflects the degree of randomization in the
system. (C) 1999 American Institute of Physics. [S0021-9606(99)00617-0].