Brinkman’s equation is often used to match solutions of Stokes’ equation to solutions of Darcy’s law at free‐fluid:porous medium interfaces by the introduction of an effectiveviscosity parameter, μe. Theoretical predictions of the dependence of μe on the porosity of the porous medium have given conflicting results. A finite difference solution of Stokes’ equation in three dimensions was used to study fluid flow near the interface between a free fluid and a porous medium. It was found that in order to match solutions of Brinkman’s equation to the numerical solutions, the value of μe had to be greater than the free‐fluid viscosity. Within numerical precision, the effective viscosity μe was monotonically increasing with decreasing porosity. Good fits to the numerical fluid velocity profiles were obtained for porosities ranging from 50% to 80%.

1.
L. D. Landau and E. M. Lifshitz, Fluid Mechanics (Pergamon, London, 1959).
2.
A. E. Scheidegger, The Physics of Flow Through Porous Media (University of Toronto Press, Toronto, 1974), Chap. 4.
3.
E. J.
Garboczi
and
D. P.
Bentz
, “
Computer simulation of the diffusivity of cement-hased materials
,”
J. Mat. Sci.
27
,
2083
(
1992
).
4.
F. R. Phelan, Jr., “Modeling of microscale fibers in fibrous porous media,” in Advanced Composite Materials: New Developments and Applications, Proceedings of the 74th Annual ASM/ESD Advanced Composite Conference (ASM International, Materials Park, OH, 1991), pp. 175–188.
5.
H. C.
Brinkman
, “
A calculation of the viscous force exerted by a flowing fluid on a dense swarm of particles
,”
Appl. Sci. Res. A
1
,
27
(
1947
).
6.
D. A. Nield and A. Bejan, Convection in Porous Media (Springer, New York, 1992), pp. 11–19.
7.
J.
Koplik
,
H.
Levine
, and
A.
Zee
, “
Viscosity renormalization in the Brinkman equation
,”
Phys. Fluids
26
,
2864
(
1983
).
8.
P. M.
Adler
and
P. M.
Mills
, “
Motion and rupture of a porous sphere in a linear flow field
,”
J. Rheol.
23
,
25
(
1979
).
9.
G. S.
Beavers
and
D. D.
Joseph
, “
Boundary conditions at a naturally permeable wall
,”
J. Fluid Mech.
30
,
197
(
1967
).
10.
P. G.
Saffman
, “
On the boundary condition at the surface of a porous medium
,”
Stud. Appl. Math.
50
,
93
(
1971
).
11.
J. Happel and H. Brenner, Low Reynolds Number Hydrodynamics (Noordhoff, Groningen, The Netherlands, 1973).
12.
G. H.
Neale
and
W. K.
Nader
, “
Prediction of transport processes within porous media: Creeping flow relative to a fixed swarm of spherical particles
,”
AIChe J.
20
,
530
(
1974
).
13.
P. G.
Saffman
, “
On the settling speed of free and fixed suspensions
,”
Stud. Appl. Math.
52
,
115
(
1973
).
14.
S.
Kim
and
W. B.
Russell
, “
Modeling of porous media by renormalization of the Stokes equations
,”
J. Fluid Mech.
154
,
269
(
1985
).
15.
L.
Durlofsky
and
J. F.
Brady
, “
Analysis of the Brinkman equation as a model for flow in porous media
,”
Phys. Fluids
30
,
3329
(
1987
).
16.
J.
Rubinstein
, “
Effective equations for flow in random porous media with a large number of scales
,”
J. Fluid Mech.
170
,
379
(
1986
).
17.
N.
Martys
and
E. J.
Garboczi
, “
Length scales relating fluid permeability and electrical conductivity in model 2-D porous media
,”
Phys. Rev. B
46
,
6080
(
1992
).
18.
R. Peyret and T. D. Taylor, Computational Methods for Fluid Flow (Springer, New York, 1983).
19.
R. E.
Larson
and
J. J. L.
Higdon
, “
Microscopic flow near the surface of two dimensional porous media. Part I: Axial flow
,”
J. Fluid Mech.
166
,
449
(
1986
).
20.
R. E.
Larson
and
J. J. L.
Higdon
, “
Microscopic flow near the surface of two dimensional porous media. Part II: Transverse flow
,”
J. Fluid Mech.
178
,
119
(
1987
).
21.
A. S.
Sangani
and
S.
Behl
, “
The planar singular solutions of Stokes’ and Laplace equations and their application to transport processes near porous surfaces
,”
Phys. Fluids A
1
,
21
(
1988
).
22.
H.
Brenner
, “
Rheology of a dilute suspension of axisymmetric Brown-ian particles
,”
Int. J. Multiphase Flow
1
,
195
(
1974
).
This content is only available via PDF.
You do not currently have access to this content.