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On the closure problem for Darcy's law
Authors:Jean Barrere  Olivier Gipouloux  Stephen Whitaker
Affiliation:(1) Modélisation Avancée des Systèmes Thermiques et Ecoulements Réels, ENSCPB Université de Bordeaux I, 351 Cours de la Libération, F-33405 Talence Cedex, France;(2) Centre de Recherche en Mathématique de Bordeaux, U.A. CNRS 226, Université de Bordeaux I, 351 Cours de la Libération, F-33405 Talence Cedex, France;(3) Laboratoire Energétique de Phénomènes de Transfert, U. A. CNRS 87, Université de Bordeaux I, Esplanade des Arts et Métiers, F-33405 Talence Cedex, France;(4) Present address: Department of Chemical Engineering, University of California, 95616 Davis, CA, USA
Abstract:In a previous derivation of Darcy's law, the closure problem was presented in terms of an integro-differential equation for a second-order tensor. In this paper, we show that the closure problem can be transformed to a set of Stokes-like equations and we compare solutions of these equations with experimental data. The computational advantages of the transformed closure problem are considerable.Roman Letters Abetasgr interfacial area of theBgr-sgr interface contained within the macroscopic system, m2 - Abetae area of entrances and exits for theBgr-phase contained within the macroscopic system, m2 - Abetasgr interfacial area of theBgr-sgr interface contained within the averaging volume, m2 - Abetae area of entrances and exits for theBgr-phase contained within the averaging volume, m2 - B second-order tensor used to respresent the velocity deviation - b vector used to represent the pressure deviation, m–1 - C second-order tensor related to the permeability tensor, m–2 - D second-order tensor used to represent the velocity deviation, m2 - d vector used to represent the pressure deviation, m - g gravity vector, m/s2 - I unit tensor - K epsibetaC–1,–epsibetalangDrangbeta, Darcy's law permeability tensor, m2 - L characteristic length scale for volume averaged quantities, m - ellbeta characteristic length scale for thebeta-phase, m - li i=1, 2, 3, lattice vectors, m - nbetasgr unit normal vector pointing from theBgr-phase toward thesgr-phase - nbetae outwardly directed unit normal vector at the entrances and exits of theBgr-phase - pbeta pressure in thebeta-phase, N/m2 - langpbetarangbeta intrinsic phase average pressure, N/m2 - 
$$tilde p_beta  $$
pbetalangpbetarangbeta, spatial deviation of the pressure in theBgr-phase, N/m2 - r position vector locating points in theBgr-phase, m - r0 radius of the averaging volume, m - t time, s - vbeta velocity vector in thebeta-phase, m/s - langvbetarangbeta intrinsic phase average velocity in thebeta-phase, m/s - langvbetarang phase average or Darcy velocity in the -phase, m/s - 
$$tilde v_beta  $$
vbetalangvbetarangbeta, spatial deviation of the velocity in theBgr-phase m/s - V averaging volume, m3 - Vbeta volume of theBgr-phase contained in the averaging volume, m3Greek Letters epsibeta Vbeta/V volume fraction of theBgr-phase - rgrbeta mass density of theBgr-phase, kg/m3 - mgrbeta viscosity of theBgr-phase, Nt/m2
Keywords:Volume averaging  Stokes flow  closure problem  Darcy's law
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