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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