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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