Mixing and coherent structures in two-dimensional viscous flows

Abstract

We introduce a dynamical description based on a probability density $\varphi (\sigma ,x,y,t)$ of the vorticity $\sigma$ in two-dimensional viscous flows such that the average vorticity evolves according to the Navier-Stokes equations. A time-dependent mixing index is defined and the class of probability densities that maximizes this index is studied. The time dependence of the Lagrange multipliers can be chosen in such a way that the masses $m(σ,t):=\intdxdy ϕ(σ,x,y,t)$ associated with each vorticity value $\sigma$ are conserved. When the masses $m(\sigma ,t)$ are conserved then 1) the mixing index satisfies an H-theorem and 2) the mixing index is the time-dependent analogue of the entropy employed in the statistical mechanical theory of inviscid 2D flows [Miller, Weichman & Cross, Phys. Rev. A \textbf{45} (1992); Robert & Sommeria, Phys. Rev. Lett. \textbf{69}, 2776 (1992)]. Within this framework we also show how to reconstruct the probability density of the quasi-stationary coherent structures from the experimentally determined vorticity-stream function relations and we provide a connection between this probability density and an appropriate initial distribution.

References in corpus (2)

• Late states of incompressible 2D decaying vorticity fields
• Evolution of the vorticity-area density during the formation of coherent structures in two-dimensional flows