Biomedical Engineering Reference
In-Depth Information
The symmetry condition at the
z
*-axis is
vu
1
vy
*
y
*
¼
0
¼
0
:
(5.42)
At the interface between the sample flow and the sheath flow, the velocity and the shear rate are
continuous:
8
<
u
2
r
z
*
¼
u
1
r
z
*
;
;
y
*
¼r
¼ b
vu
2
y
*
¼r
:
vu
1
vy
*
(5.43)
:
vy
*
For a flat channel (
h
1), the position of the interface can be estimated as
1
r
¼
(5.44)
þ
2
bk
1
where
k
m
1
is the flow rate ratio between the sheath streams and the mixing streams. A Fourier
analysis with the above boundary conditions results in the coefficients of
(5.40)
:
¼
_
m
2
=
b
sinh
qr
cosh
2
qr
cosh
q
sinh
3
qr
cosh
q
sinh
2
qr
sinh
q
cosh
q
A
1
¼
A
0
½
ð
b
1
Þ
sinh
2
qr
ð
b
1
Þ
ð
cosh
q
cosh
qr
Þþð
b
1
Þ
sinh
qr
cosh
qr
b
cosh
2
qr
sinh
qr
cosh
2
q
sinh
3
qr
cosh
2
q
cosh
q
ð
cosh
q
cosh
qr
Þ=½
sinh
2
qr
cosh
qr
sinh
q
cosh
q
ð
b
Þ
1
b
cosh
2
qr
cosh
q
sinh
2
qr
cosh
q
A
2
¼
A
0
½
ð
b
1
Þ
sinh
qr
cosh
qr
sinh
q
(5.45)
ð
cosh
q
cosh
qrÞ=½b
cosh
2
qr
sinh
2
q
sinh
2
qr
cosh
2
q
ðb
1
Þ
sinh
qr
ðb
1
Þ
sinh
qr
cosh
qr
sinh
q
cosh
q
B
1
¼
0
Þ=½b
cosh
2
qr
cosh
q
sinh
2
qr
cosh
q
B
2
¼
A
0
½ðb
1
Þ
sinh
qr
ð
cosh
q
cosh
qr
ð
b
1
Þ
sinh
qr
cosh
qr
sinh
q
4
h
2
n
þ
1
where
A
0
¼ð
Þ
3
p
3
.
Figure 5.15
shows the typical dimensionless velocity distribution
inside the flow channel for the same flow rate in all streams (
k
1
ð
2
n
1
Þ
1). The theoretical model is depicted
with the solid lines in
Fig. 5.15
. The velocity of the sample flow is lower if the sample flow is more
viscous than the sheath flow (
b
¼
<
1) (
Fig. 5.15
(a)). If the sheath flows are more viscous (
b
>
1), the
sample flow is faster (
Fig. 5.15
(b)).
5.5.3
Combination of hydrodynamic focusing and sequential segmentation
Both hydrodynamic focusing and sequential segmentation can be combined to improve convective/
diffusive mixing in a microchannel
[29]
. The concept reduces mixing paths in both transversal and
axial directions.
Figure 5.16
describes this mixing concept. The micromixer has four inlets and one
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