Biomedical Engineering Reference
In-Depth Information
3.1.3 Solid-Fluid Interface Conditions
The solid-fluid interface oY
fs
is characterized by its normal unit vector n directed
toward the solid domain. Concerning the surface charge density, the presence of
the Stern layer and the ionic exchanges quantified by the coefficients a
(homo-
geneous to lengths [
76
]) may generate an electrical jump r
fs
by crossing the
interface from the solid part to the fluid phase. As a result, two different electric
surface charges are introduced, r
f
and r
s
¼
r
f
þ
r
fs
;
referring respectively to the
surface charge density seen from the fluid or the solid. The set of interface con-
ditions is then given by:
/
f
¼
/
s
;
ð
14
Þ
n
¼
r
f
;
e
f
r
/
f
ð
15
Þ
ð
P
Z
:
r
u
e
s
r
/
s
Þ
n
¼
r
s
;
ð
16
Þ
v
¼
du
dt
;
ð
17
Þ
J
n
¼
a
o
n
b
ot
;
ð
18
Þ
S
s
n
¼
S
f
n
:
ð
19
Þ
They correspond, respectively, to the electric potentials continuity and the
electric flux conditions at the interface, to the no-slip condition, to the ionic
exchange property of this interface and to the continuity of the normal stress.
3.2 Upscaling Procedure
An asymptotic periodic homogenization process [
7
,
102
] is carried out to propa-
gate our microscopic description of the phenomena at the upper scale. The prin-
ciple of this procedure is to consider a periodic representative cell Y or
representative volume element (RVE), whose size must be large enough to contain
all relevant microscopic heterogeneities and small enough to ensure the macro-
scopic homogeneity. Let
'
and L be characteristic lengths of the micro- and macro-
scales respectively, and x and X the associated coordinate systems. In order to keep
the independence between these two scales, the ratio g
¼ '=
L must be small in
comparison with 1
:
In our problem, the length
'
associated with the microscale is
typically the pore size length and the length L is typically of the order of the
cortical tissue size.
The general procedure of the periodic homogenization consists in: i. writing the
equations at the microscale in a non-dimensional fashion and giving scaling laws
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