Phase transition in time-reversible Navier-Stokes equations - Archive ouverte HAL Access content directly
Journal Articles Physical Review E Year : 2019

Phase transition in time-reversible Navier-Stokes equations

Sergey Nazarenko
  • Function : Author
  • PersonId : 828400
Giorgio Krstulovic
Simon Thalabard
  • Function : Author
  • PersonId : 960545

Abstract

We present a comprehensive study of the statistical features of a three-dimensional time-reversible Navier-Stokes (RNS) system, wherein the standard viscosity ν is replaced by a fluctuating thermostat that dynamically compensates for fluctuations in the total energy. We analyze the statistical features of the RNS steady states in terms of a non-negative dimensionless control parameter Rr, which quantifies the balance between the fluctuations of kinetic energy at the forcing length scale f and the total energy E0. For small Rr, the RNS equations are found to produce "warm" stationary statistics, e.g. characterized by the partial thermalization of the small length-scales. For large Rr, the stationary solutions have features akin to standard hydrodynamic ones: They have compact energy support in k-space and are essentially insensitive to the truncation scale kmax. The transition between the two statistical regimes is observed to be smooth but rather sharp. Using insights from a diffusion model of turbulence (Leith model), we argue that the transition is in fact akin to a continuous phase transition, where Rr indeed behaves as a thermodynamic control parameter, e.g. a temperature. A relevant order-parameter can be suitably defined in terms of a (normalized) enstrophy, while the symmetry breaking parameter h is identified as (one over) the truncation scale kmax. We find that the signatures of the phase transition close to the critical point R r can essentially be deduced from a heuristic mean-field Landau free energy. This point of view allows us to reinterpret the relevant asymptotics in which the dynamical ensemble equivalence conjectured by Gallavotti, Phys.Lett.A, 223, 1996 could hold true. We argue that Gallavotti's limit is precisely the joint limit Rr > → R r and h > → 0, with the overset symbol ">" indicating that these limits are approached from above. The limit therefore relates to the statistical features at the critical point. In this regime, our numerics indicate that the low-order statistics of the 3D RNS are indeed qualitatively similar to those observed in direct numerical simulations of the standard Navier-Stokes (NS) equations with viscosity chosen so as to match the average value of the reversible viscosity. This result suggests that Gallavotti's equivalence conjecture could indeed be of relevance to model 3D turbulent statistics, and provides a clear guideline for further numerical investigations at higher resolutions.
Fichier principal
Vignette du fichier
halRNS.pdf (1.21 Mo) Télécharger le fichier
Origin : Files produced by the author(s)
Loading...

Dates and versions

hal-02346672 , version 1 (05-11-2019)

Identifiers

Cite

Vishwanath Shukla, Bérengère Dubrulle, Sergey Nazarenko, Giorgio Krstulovic, Simon Thalabard. Phase transition in time-reversible Navier-Stokes equations. Physical Review E , 2019, 100 (4), ⟨10.1103/PhysRevE.100.043104⟩. ⟨hal-02346672⟩
106 View
44 Download

Altmetric

Share

Gmail Facebook X LinkedIn More