The part of the nonlinear term in the Navier-Stokes equation which represen
ts coupling to the small-scale modes may be averaged out by introducing a w
eak conditional average with asymptotic freedom in wavenumber. A residual d
eterministic part, while important for individual realizations, makes a neg
ligible contribution to the renormalization of the dissipation rate. This i
s because the full ensemble average, needed to establish the energy balance
, relaxes the constraint on the conditional average.