Numerical analysis of a Reynolds Stress Model for turbulent mixing: the one-dimensional case

A mixed hyperbolic-parabolic, non conservative, Reynolds Stress Model (RSM), is studied. It is based on an underlying set of Langevin equations, and allows to describe turbulent mixing, including transient demixing effects as well as incomplete mixing. Its mathematical structure is analysed, and specific regimes, related to acoustic-like, Riemann-type, or self-similar solutions, are identified. A second-order accurate numerical scheme is proposed in arbitrary curvilinear geometry. Its accuracy and convergence behaviour are tested by comparison with analytical solutions in the different regimes. The numerical scheme can be generalized to multi-dimensional configurations, with potentially cylindrical symmetry, on unstructured meshes. Mathematics Subject Classification. 65M12, 65M22, 76F25. Received May 9, 2020. Accepted July 13, 2021.

[1]  Christophe Berthon,et al.  An entropy preserving MOOD scheme for the Euler equations , 2013 .

[2]  Arindam Banerjee,et al.  Development and validation of a turbulent-mix model for variable-density and compressible flows. , 2010, Physical review. E, Statistical, nonlinear, and soft matter physics.

[3]  Roland Duclous,et al.  DIFFUSION LIMIT OF THE SIMPLIFIED LANGEVIN PDF MODEL IN WEAKLY INHOMOGENEOUS TURBULENCE , 2015 .

[4]  B. Nkonga,et al.  A Godunov-Type Solver for the Numerical Approximation of Gravitational Flows , 2014 .

[5]  Serge Gauthier,et al.  A second-order turbulence model for gaseous mixtures induced by Richtmyer—Meshkov instability , 2005 .

[6]  Benoît Merlet,et al.  Error estimate for finite volume scheme , 2007, Numerische Mathematik.

[7]  F. Poggi,et al.  Velocity measurements in turbulent gaseous mixtures induced by Richtmyer–Meshkov instability , 1998 .

[8]  J. Clérouin,et al.  Sudden diffusion of turbulent mixing layers in weakly coupled plasmas under compression. , 2019, Physical review. E.

[9]  O. Soulard,et al.  Modeling of Reynolds Stress Models for Diffusion Fluxes Inside Shock Waves , 2014 .

[10]  M. Uhlmann,et al.  An approximate solution of the Riemann problem for a realisable second-moment turbulent closure , 2002 .

[11]  F. Guillois,et al.  Permanence of large eddies in Richtmyer-Meshkov turbulence with a small Atwood number , 2018, Physical Review Fluids.

[12]  K. Molvig,et al.  Plasma viscosity with mass transport in spherical inertial confinement fusion implosion simulations , 2015, 1509.01274.

[13]  J. Ristorcelli Exact statistical results for binary mixing and reaction in variable density turbulence , 2017 .

[14]  F. Bouchut Nonlinear Stability of Finite Volume Methods for Hyperbolic Conservation Laws: and Well-Balanced Schemes for Sources , 2005 .

[15]  Christophe Berthon,et al.  AN APPROXIMATE NONLINEAR PROJECTION SCHEME FOR A COMBUSTION MODEL , 2003 .

[16]  F. Lagoutière,et al.  Probabilistic Analysis of the Upwind Scheme for Transport Equations , 2007, 0712.3217.

[17]  O. Soulard,et al.  Evaluation of augmented RSM for interaction of homogeneous turbulent mixture with shock and rarefaction waves , 2014 .

[18]  Victor Montagud-Camps Turbulence , 2019, Turbulent Heating and Anisotropy in the Solar Wind.

[19]  Stephen B. Pope,et al.  On the relationship between stochastic Lagrangian models of turbulence and second‐moment closures , 1994 .

[20]  F. Guillois,et al.  A two-scale Langevin PDF model for Richtmyer–Meshkov turbulence with a small Atwood number , 2020 .

[21]  S. Pope PDF methods for turbulent reactive flows , 1985 .

[22]  P. Arnault Modeling viscosity and diffusion of plasma for pure elements and multicomponent mixtures from weakly to strongly coupled regimes , 2013 .

[23]  O. Soulard,et al.  A turbulent mixing Reynolds stress model fitted to match linear interaction analysis predictions , 2010 .

[24]  B. Gréa The dynamics of the k–ϵ mix model toward its self-similar Rayleigh–Taylor solution , 2015 .

[25]  Roland Schiestel Méthodes de Modélisation et de Simulation des Ecoulements Turbulents , 2006 .

[26]  Denis Veynante,et al.  Turbulent combustion modeling , 2002, VKI Lecture Series.

[27]  Chi-Wang Shu,et al.  Strong Stability-Preserving High-Order Time Discretization Methods , 2001, SIAM Rev..

[28]  Jacob A. McFarland,et al.  Large-eddy simulation and Reynolds-averaged Navier-Stokes modeling of a reacting Rayleigh-Taylor mixing layer in a spherical geometry , 2018, Physical Review E.

[29]  Roland Schiestel,et al.  Modeling and Simulation of Turbulent Flows , 2008 .

[30]  K. Mackay,et al.  Modeling gas–shell mixing in ICF with separated reactants , 2020 .

[31]  J. Williamson Low-storage Runge-Kutta schemes , 1980 .

[32]  Bruno Després,et al.  A cell-centered Lagrangian hydrodynamics scheme on general unstructured meshes in arbitrary dimension , 2009, J. Comput. Phys..

[33]  Alexandre Favre,et al.  La Turbulence en mécanique des fluides : bases théoriques et expérimentales, méthodes statistiques , 1976 .

[34]  Y. Bury,et al.  Turbulent transition of a gaseous mixing zone induced by the Richtmyer-Meshkov instability , 2020, Physical Review Fluids.

[35]  K. Nishihara,et al.  Asymptotic growth in the linear Richtmyer–Meshkov instability , 1997 .

[36]  J. Clouet,et al.  The Rosseland approximation for radiative transfer problems in heterogeneous media , 1997 .

[37]  K. Carlson,et al.  Turbulent Flows , 2020, Finite Analytic Method in Flows and Heat Transfer.

[38]  Pierre-Henri Maire,et al.  Contribution to the numerical modeling of Inertial Confinement Fusion , 2011 .

[39]  J. Haas,et al.  Experimental and Numerical Investigation of the Growth of an Air/SF6 Turbulent Mixing Zone in a Shock Tube , 2017 .