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
2 D
Þ:
(5.27)
The solution of (5.21) with the previously mentioned boundary conditions is
m 2 D
K 0 ½
ur
2 D
Þ
exp
½
ur cos q
2 D
Þ
Þ¼ _
pRH u 1
c
ð
r
;
q
(5.28)
K 1 ½
uR
2 D
Þ
K 0 ½
uR
2 D
Þ
cos q
½
uR cos q
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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