When does decaying 2D turbulence reach its statistical-mechanics equilibrium? · revision history

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Title
When does decaying 2D turbulence reach its statistical-mechanics equilibrium?
Plain
Freely decaying flat turbulence organizes itself into a few large vortices or jets, and a theory from statistical mechanics predicts the final pattern by maximizing a mixing entropy. The prediction works in some cases and fails in others, and no rule says when.
Precise
For 2D Euler or high-Re Navier-Stokes flow from given initial vorticity in a bounded or periodic domain, the Miller-Robert-Sommeria theory predicts the late-time coarse-grained vorticity as the maximum-entropy state constrained by energy and by all integrals of functions of vorticity (Casimirs). Determine the conditions on initial vorticity distribution, domain geometry and Re under which the observed late-time state matches the prediction, and characterize the incomplete relaxation where it does not. Answer: a criterion validated by DNS and experiment.
Settled by
Ensembles of high-resolution DNS and soap-film or thin-layer experiments compared with computed equilibria, with a criterion that predicts agreement or failure in advance.
Kind
phenomenon
Answer type
classification
References
(empty)
Literature status
open
Status note
Cases of agreement and of incomplete relaxation are reviewed in Bouchet and Venaille, Physics Reports 2012.
Posed since
(empty)