Biomedical Engineering Reference
In-Depth Information
V
c
H
D
c
be the dimensionless cell velocity and rewrite equation
(14.8) as
n
=
nP ee
P
H
Y
e
Pe
Let
Pe
=
−
1
from which we readily deduce the concentrations at
the bottom (
Y
= 0) and the top (
Y
=
H
) of the cavity
Pee
Pe
e
Pe
Pe
e
Pe
n
0
=
1
n
;
n
1
=
1
n
−
−
∆
n
=(
n
1
−
n
0
)=
nP e
(14.10)
14.2.2.1
Nondimensional Equations
Nondimensional governing equations may be expressed in the following form,
by choosing
H
and
H
2
/D
c
as length and time scales, respectively.
V
= 0
∇·
(14.11)
D
c
K
V
=
νH
2
−
∇
P
−
RaNe
2
(14.12)
∂N
∂t
+
∇·
(
N V
)+
∇·
(
N
−
Pe
)=
∇
2
N
(14.13)
In terms of the stream function
ψ
, they become
2
ψ
=
Ra
∂N
∂x
∇
(14.14)
∂N
∂t
(
N
−
Pe
)=
(
N V
)+
2
N
+
∇·
∇·
∇
(14.15)
where
V
=
∂ψ
∂ψ
∂x
∂y
,
−
N
=
n
n
0
∆
n
−
and the Rayleigh number
Ra
=
gKHβnP e
νD
c
(14.16)
with initial and boundary conditions
=
e
Pe
N
=
N
=
n
n
0
∆
n
−
−
Pe
−
1
at
t
= 0
(14.17)
(
e
Pe
−
1)
Pe
ψ
=0
,∂N/∂x
=0 at
x
=0
,F
and
ψ
=0
,∂N/∂y
=
PeN
+
Pe/
(
e
Pe
−
1)
at
y
= 0
(14.18)
The diffusion state (14.8) can be expressed in the nondimensional form
N
d
=
e
Pey
−
1
(14.19)
e
Pe
−
1
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