NCAR TOY - February 2008
18
Example of a linear operator
For the linear operators the only contributions from averaging in time are the result of modes with the same frequency and wave number. So they only contribute slow modes to the evolution of the slow mode dynamics.
Forcing range: the bulk of the kinetic energy resides here.
Intertial range: motions are dominated by inertial effects and viscous diffusion is negligible
Dissipation range: motions dominated by viscous effects

One of the points in KolmogorovŐs 1941 theory was that, in every turbulent flow at sufficiently high Re, the statistics of the motions of a scales between kd and kf have a universal form uniquely determined by epsilon, the energy dissipation rate, independent of the viscosity, nu.