Unsteady mixed flows in non uniform closed water pipes: a Full Kinetic Approach

We recall the Pressurized and Free Surface model constructed for the modeling of unsteady mixed flows in closed water pipes where transition points between the free surface and pressurized flow are treated as a free boundary associated to a discontinuity of the gradient of pressure. Then we present a numerical kinetic scheme for the computations of unsteady mixed flows in closed water pipes. This kinetic method that we call FKA for “Full Kinetic Approach” is an easy and mathematically elegant way to deal with multiple transition points when the changes of state between free surface and pressurized flow occur. We use two approaches namely the “ghost waves approach” and the “Full Kinetic Approach” to treat these transition points. We show that this kinetic numerical scheme has the following properties: it is wet area conservative, under a CFL condition it preserves the wet area positive, it treats “naturally” the flooding zones and most of all it is very easy to implement it. Finally numerical experiments versus laboratory experiments are presented and the scheme produces results that are in a very good agreement. We also present a numerical comparison with analytic solutions for free surface flows in non uniform pipes: the numerical scheme has a very good behavior. A code to code comparison for pressurized flows is also conducted and leads to a very good agreement. We also perform a numerical experiment when flooding and drying flows may occur and finally make a numerical study of the order of the kinetic method.

[1]  Derek M. Cunnold,et al.  Observations of 1,1‐difluoroethane (HFC‐152a) at AGAGE and SOGE monitoring stations in 1994–2004 and derived global and regional emission estimates , 2007 .

[2]  Nguyen Trieu Dong Sur une méthode numérique de calcul des écoulements non permanents soit à surface libre, soit en charge, soit partiellement à surface libre et partiellement en charge , 1990 .

[3]  B. Perthame,et al.  A kinetic scheme for the Saint-Venant system¶with a source term , 2001 .

[4]  A kinetic scheme for pressurised flows in non uniform closed water pipes , 2008 .

[5]  Convergence d'un schéma à profils stationnaires pour les équations quasi linéaires du premier ordre avec termes sourcesConvergence of a stationary profiles scheme for the first order quasilinear equations with source terms , 2001 .

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

[7]  Pierre Archambeau,et al.  An exact Riemann solver and a Godunov scheme for simulating highly transient mixed flows , 2011, J. Comput. Appl. Math..

[8]  Christian Bourdarias,et al.  A conservative model for unsteady flows in deformable closed pipes and its implicit second-order finite volume discretisation , 2008 .

[9]  Michael Westdickenberg,et al.  Gravity driven shallow water models for arbitrary topography , 2004 .

[10]  C. Bourdarias,et al.  Air entrainment in transient flows in closed water pipes: a two-layer approach , 2009, 0910.0334.

[11]  Mehmet Ersoy Modélisation, analyse mathématique et numérique de divers écoulements compressibles ou incompressibles en couche mince. , 2010 .

[12]  David C. Wiggert Transient flow in free-surface, pressurized systems , 1972 .

[13]  Christian Bourdarias,et al.  A kinetic formulation for a model coupling free surface and pressurised flows in closed pipes , 2008 .

[14]  B. Dewals,et al.  Simulation numérique des écoulements mixtes hautement transitoires dans les conduites d'évacuation des eaux , 2009 .

[15]  Benoît Perthame,et al.  Kinetic formulation of conservation laws , 2002 .

[16]  Musandji Fuamba Contribution on transient flow modelling in storm sewers , 2002 .

[17]  E. Benjamin Wylie,et al.  Fluid Transients in Systems , 1993 .

[18]  Philippe G. LeFloch,et al.  A Godunov-type method for the shallow water equations with discontinuous topography in the resonant regime , 2011, J. Comput. Phys..

[19]  Benjamin Dewals,et al.  A fast universal solver for 1D continuous and discontinuous steady flows in rivers and pipes , 2011 .

[20]  Christian Bourdarias,et al.  A Kinetic Scheme for Transient Mixed Flows in Non Uniform Closed Pipes: A Global Manner to Upwind All the Source Terms , 2009, J. Sci. Comput..

[21]  A kinetic scheme for pressurized flows in non uniform pipes , 2008, 0812.0105.

[22]  Christian Bourdarias,et al.  A finite volume scheme for a model coupling free surface and pressurised flows in pipes , 2007 .

[23]  D. Kröner,et al.  The minimum entropy principle for compressible fluid flows in a nozzle with discontinuous cross-section , 2008 .

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

[25]  C. Bourdarias,et al.  A mathematical model for unsteady mixed flows in closed water pipes , 2011, 1106.2081.

[26]  Christian Bourdarias,et al.  A kinetic scheme for unsteady pressurised flows in closed water pipes , 2008, J. Comput. Appl. Math..

[27]  C. Dafermos Generalized characteristics in hyperbolic systems of conservation laws , 1989 .

[28]  Mai Duc Thanh,et al.  Numerical Solutions to Compressible Flows in a Nozzle with Variable Cross-section , 2005, SIAM J. Numer. Anal..

[29]  J. A. McCorquodale,et al.  Transient conditions in the transition from gravity to surcharged sewer flow , 1982 .

[31]  Charles C. S. Song,et al.  Transient Mixed-Flow Models for Storm Sewers , 1983 .

[32]  Jean-Pierre Vilotte,et al.  Numerical modeling of self‐channeling granular flows and of their levee‐channel deposits , 2006 .

[33]  Pilar García-Navarro,et al.  An implicit method for water flow modelling in channels and pipes , 1994 .

[34]  Yves Zech,et al.  Numerical and experimental water transients in sewer pipes , 1997 .