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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