On the closure problem for Darcy's law |
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Authors: | Jean Barrere Olivier Gipouloux Stephen Whitaker |
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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 |
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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 A![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) interfacial area of the - interface contained within the macroscopic system, m2 - A e area of entrances and exits for the -phase contained within the macroscopic system, m2 - A![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) interfacial area of the - interface contained within the averaging volume, m2 - A e area of entrances and exits for the -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 ![epsi](/content/vw27558ttqh0v2j5/xxlarge949.gif) C–1,–![epsi](/content/vw27558ttqh0v2j5/xxlarge949.gif) ![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) D![rang](/content/vw27558ttqh0v2j5/xxlarge9002.gif) , Darcy's law permeability tensor, m2 - L characteristic length scale for volume averaged quantities, m - ![ell](/content/vw27558ttqh0v2j5/xxlarge8467.gif) characteristic length scale for the -phase, m - li i=1, 2, 3, lattice vectors, m - n![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) unit normal vector pointing from the -phase toward the -phase - n e outwardly directed unit normal vector at the entrances and exits of the -phase - p pressure in the -phase, N/m2 - p![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) ![rang](/content/vw27558ttqh0v2j5/xxlarge9002.gif) intrinsic phase average pressure, N/m2 - p – p![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) ![rang](/content/vw27558ttqh0v2j5/xxlarge9002.gif) , spatial deviation of the pressure in the -phase, N/m2 - r position vector locating points in the -phase, m - r0 radius of the averaging volume, m - t time, s - v velocity vector in the -phase, m/s - v![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) ![rang](/content/vw27558ttqh0v2j5/xxlarge9002.gif) intrinsic phase average velocity in the -phase, m/s - v![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) phase average or Darcy velocity in the -phase, m/s - v – v![beta](/content/vw27558ttqh0v2j5/xxlarge946.gif) ![rang](/content/vw27558ttqh0v2j5/xxlarge9002.gif) , spatial deviation of the velocity in the -phase m/s - V averaging volume, m3 - V volume of the -phase contained in the averaging volume, m3Greek Letters ![epsi](/content/vw27558ttqh0v2j5/xxlarge949.gif) V /V volume fraction of the -phase - ![rgr](/content/vw27558ttqh0v2j5/xxlarge961.gif) mass density of the -phase, kg/m3 - ![mgr](/content/vw27558ttqh0v2j5/xxlarge956.gif) viscosity of the -phase, Nt/m2 |
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Keywords: | Volume averaging Stokes flow closure problem Darcy's law |
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