Multi-dimensional shear shallow water flows: Problems and solutions

Abstract The mathematical model of shear shallow water flows of constant density is studied. This is a 2D hyperbolic non-conservative system of equations that is mathematically equivalent to the Reynolds-averaged model of barotropic turbulent flows. The model has three families of characteristics corresponding to the propagation of surface waves, shear waves and average flow (contact characteristics). The system is non-conservative: for six unknowns (the fluid depth, two components of the depth averaged horizontal velocity, and three independent components of the symmetric Reynolds stress tensor) one has only five conservation laws (conservation of mass, momentum, energy and mathematical ‘entropy’). A splitting procedure for solving such a system is proposed allowing us to define a weak solution. Each split subsystem contains only one family of waves (either surface or shear waves) and contact characteristics. The accuracy of such an approach is tested on 2D analytical solutions describing the flow with linear with respect to the space variables velocity, and on the solutions describing 1D roll waves. The capacity of the model to describe the full transition scenario as commonly seen in the formation of roll waves: from uniform flow to 1D roll waves, and, finally, to 2D transverse ‘fingering’ of the wave profiles, is shown.

[1]  E. Toro Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .

[2]  Richard Saurel,et al.  A multiphase model with internal degrees of freedom: application to shock–bubble interaction , 2003, Journal of Fluid Mechanics.

[3]  O. V. Troshkin On wave properties of an incompressible turbulent fluid , 1990 .

[4]  Lev Truskinovsky,et al.  Kinks versus Shocks , 1993 .

[5]  R. Saurel,et al.  Estimation of the turbulent energy production across a shock wave , 2006, Journal of Fluid Mechanics.

[6]  David Lannes,et al.  Fully nonlinear long-wave models in the presence of vorticity , 2014, Journal of Fluid Mechanics.

[7]  S. L. Gavrilyuk,et al.  Diffuse interface model for compressible fluid - Compressible elastic-plastic solid interaction , 2012, J. Comput. Phys..

[8]  S. Gavrilyuk,et al.  Formation and coarsening of roll-waves in shear shallow water flows down an inclined rectangular channel , 2017 .

[9]  Richard Saurel,et al.  Shock jump relations for multiphase mixtures with stiff mechanical relaxation , 2007 .

[10]  M. Baer,et al.  A two-phase mixture theory for the deflagration-to-detonation transition (ddt) in reactive granular materials , 1986 .

[11]  R. R. Brock,et al.  Development of Roll-Wave Trains in Open Channels , 1969 .

[12]  S. Gavrilyuk,et al.  The classical hydraulic jump in a model of shear shallow-water flows , 2013, Journal of Fluid Mechanics.

[13]  G. D. Maso,et al.  Definition and weak stability of nonconservative products , 1995 .

[14]  B. V. Leer,et al.  Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .

[15]  Geometric evolution of the Reynolds stress tensor , 2010 .

[16]  P. LeFloch,et al.  Hyperbolic Systems of Conservation Laws: The Theory of Classical and Nonclassical Shock Waves , 2002 .

[17]  Nicolas Favrie,et al.  A thermodynamically compatible splitting procedure in hyperelasticity , 2014, J. Comput. Phys..

[18]  V. Teshukov Gas-dynamic analogy for vortex free-boundary flows , 2007 .

[19]  D. Stewart,et al.  Two-phase modeling of deflagration-to-detonation transition in granular materials: Reduced equations , 2001 .

[20]  A. A. Chesnokov,et al.  Spilling breakers in shallow water: applications to Favre waves and to the shoaling and breaking of solitary waves , 2016, Journal of Fluid Mechanics.

[21]  Kyle T. Mandli Finite Volume Methods for the Multilayer Shallow Water Equations with Applications to Storm Surges , 2011 .

[22]  Structural Stability of Shock Solutions of Hyperbolic Systems in Nonconservation Form via Kinetic Relations , 2008 .

[23]  R. R. Brock Development of roll waves in open channels , 1967 .

[24]  R. Abgrall,et al.  A Multiphase Godunov Method for Compressible Multifluid and Multiphase Flows , 1999 .

[25]  N. Besse On the Waterbag Continuum , 2011 .

[26]  S. Gavrilyuk Multiphase Flow Modeling via Hamilton’s Principle , 2011 .

[27]  Smadar Karni,et al.  Multicomponent Flow Calculations by a Consistent Primitive Algorithm , 1994 .

[28]  S. Gavrilyuk,et al.  Modelling turbulence generation in solitary waves on shear shallow water flows , 2015, Journal of Fluid Mechanics.

[29]  D. J. Benney Some Properties of Long Nonlinear Waves , 1973 .

[30]  R. LeVeque Numerical methods for conservation laws , 1990 .

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

[32]  O. Pironneau,et al.  Analysis of the K-epsilon turbulence model , 1994 .

[33]  D. Wilcox Turbulence modeling for CFD , 1993 .

[34]  Khaled Saleh,et al.  A positive and entropy-satisfying finite volume scheme for the Baer-Nunziato model , 2016, J. Comput. Phys..

[35]  Nicolas Favrie,et al.  Multi-solid and multi-fluid diffuse interface model: Applications to dynamic fracture and fragmentation , 2015, J. Comput. Phys..

[36]  Rémi Abgrall,et al.  Two-Layer Shallow Water System: A Relaxation Approach , 2009, SIAM J. Sci. Comput..

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

[38]  Martin Mork,et al.  Topographic effects in stratified flows resolved by a spectral method , 1993 .

[39]  On the Number of Conserved Quantities for the Two‐Layer Shallow‐Water Equations , 2001 .

[40]  L. V. Ovsyannikov Two-layer “Shallow water” model , 1979 .

[41]  H. Chanson,et al.  reaking bore : Physical observations of roller characteristics , 2015 .

[42]  Sergey Gavrilyuk,et al.  Élaboration d'un modèle d'écoulements turbulents en faible profondeur : application au ressaut hydraulique et aux trains de rouleaux , 2013 .

[43]  I. Bohachevsky,et al.  Finite difference method for numerical computation of discontinuous solutions of the equations of fluid dynamics , 1959 .

[44]  S. Gavrilyuk,et al.  A new model of roll waves: comparison with Brock’s experiments , 2012, Journal of Fluid Mechanics.

[45]  G. Russo,et al.  ANALYTICAL AND NUMERICAL SOLUTIONS OF THE SHALLOW WATER EQUATIONS FOR 2D ROTATIONAL FLOWS , 2004 .

[46]  CONSERVATION LAWS FOR ONE-DIMENSIONAL SHALLOW WATER MODELS FOR ONE AND TWO-LAYER FLOWS , 2006 .