Biomedical Engineering Reference
In-Depth Information
y
p
in the polar coordinate system as shown in
Fig. 5.11
, the
boundary condition of the solute flow is, after Fick's law:
d
c
d
r
x
2
Defining the variable
r
¼
þ
r¼R
¼
D
¼
m
2
j
(5.24)
2
pRHD
where
H
is the height of the mixing chamber above the injection nozzle. Assuming a small mixing ratio
(
m
2
m
1
), the following boundary condition is acceptable for
(5.23)
:
d
r
r¼N
¼
d
0
:
(5.25)
Equation
(5.23)
can be rewritten for the polar coordinate system as
d
2
u
2
D
2
G
d
r
2
þ
1
r
d
d
r
G ¼
0
:
(5.26)
The solution of
(5.26)
is the modified Bessel function of the second kind and zero order:
G ¼
K
0
½
ur
=ð
2
D
Þ:
(5.27)
The solution of
(5.21)
with the previously mentioned boundary conditions is
m
2
D
K
0
½
ur
=ð
2
D
Þ
exp
½
ur
cos
q
=ð
2
D
Þ
Þ¼
_
pRH
u
1
c
ð
r
;
q
(5.28)
K
1
½
uR
=ð
2
D
Þ
K
0
½
uR
=ð
2
D
Þ
cos
q
½
uR
cos
q
=ð
2
D
Þ
exp
where
q
is the angular variable of the polar coordinate system.
FIGURE 5.12
Dimensionless concentration distribution around the injection nozzle: (a) Pe
¼
0.1 and (b) Pe
¼
1.
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