Important length and time scales for this phenomenon vary as the negative one-forth and negative one-half of the specific power dissipation; those scales and a one-thirds power law governing it in the mean are named for Kolmogorov.
In the phase spaces of continuum Newtonian systems, transitions to this behavior occur at Hopf bifurcations. Important length and time scales for this phenomenon vary as the negative one-forth and negative one-half of the specific power dissipation; those scales and a one-thirds power law governing it in the mean are named for Kolmogorov. The Reynolds time-averaging theorem was created to allow valid physical laws in the presence of this behavior, in spite of its chaotic nature. FTP, name this type of flow which occurs in general at high values of the Reynolds number.
In the phase spaces of continuum Newtonian systems, transitions to this behavior occur at Hopf bifurcations.
turbulence [or turbulent flow; prompt on "quasi-chaos" or word forms thereof]