“…A plausible argument can be made for equipartition, that is, that•Vs• = ,,v'/2 ........................... (s)at least on an average basis. On the other hand, from(7) we see that H increases more rapidly for the large wave-number (l/L) components of the turbulent fluid, which therefore preempt the supply of kinetic energy. Thus, H would vary wi• the size of the eddy.…”