Biomedical Engineering Reference
In-Depth Information
At high Peclet numbers (Pe
15/
b
) and moderate
M
values, the process is determined by the lami-
nation process of the mixed liquids:
<
1
3
Pe
2
3
b
4
3
1
2
M
p
Þ
t
mixing
z
6
f
1
ð
(7.77)
where function
f
is defined as:
X
1
=
2
erf
X
1
=
2
f
ð
X
Þ¼
ð
Þ
(7.78)
and erf is the error function.
At high Peclet numbers (Pe
>
15/
b
) and small
M
values, the mixing time is:
Pe
1
2
b
3
2
ln
4
p
2
3
M
4
1
4
3
1
b
Pe
t
mixing
z
p
:
(7.79)
Figure 7.32
shows the numerical and analytical results of the dimensionless mixing time in different
regions of Peclet numbers. The three mixing regimes can be clearly observed. At a fixed geometry and
constant diffusion coefficient, the Peclet number is determined by the angular velocity
u
only. In
contrast to a straight channel, high Peclet numbers lead to a short mixing time because of the lami-
nation effect shown in
Fig. 7.31
.
FIGURE 7.32
Dimensionless mixing time as function of Peclet number (b ¼ 0.05, M¼ 0.3, the rectangles show the simulation
result, the lines are analytical results) (after
[44]
).
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