Biomedical Engineering Reference
In-Depth Information
1.4
δ
1.2
1
Edge of the RBC core
Tube wall
0.8
0.6
0.4
0.2
δ
0
10
20
30
40
0
0.5
1
1.5
2
2.5
3
3.5
μ
μ
x( m)
cell-free layer thickness ( m)
Fig. 10.16. An example of a CFL edge (left) and local CFL thickness distribution (right) for H t
=
0
.
45 and D
=
20
μ
m (from [51])
the LD-RBC suspensions the viscosities were computed, with and without rouleaux,
as functions of the shear rate over the range 0
0 s 1 . RBC suspen-
sion viscosities were normalized by the viscosity values of their suspending media.
These data are compared in Fig. 10.17(a) as relative viscosity against shear rate at
constant hematocrit. The MS-RBC model viscosity curves lie very close to the vis-
cosities measured in three different laboratories. The model, consisting only of RBCs
in suspension, clearly captures the effect of aggregation on the viscosity at low shear
005 s 1
.
to 1000
.
Chien et al. (1966), whole blood
Chien et al. (1966), Ringer ES
LD-RBC (aggregation)
LD-RBC (no aggregation)
γ
10 3
γ =0.052 s -1
γ =0.052 s -1 &
MS-RBC (no aggregation)
MS-RBC (aggregation)
LD-RBC (no aggregation)
LD-RBC (aggregation)
=52.0 s -1
10 2
10 2
x
x
x x x x x x x x
10 1
10 1
10 0
10 0
0
20
40
60
10 -2
10 -1
10 0
10 1
10 2
10 3
(a)
(b)
-1
Hematocrit (%)
Shear rate (s )
Fig. 10.17. Validation of simulation results for whole blood and Ringer erythrocyte solutions
(ESs). (a) Plot of non-Newtonian viscosity relative to solvent viscosity as a function of shear rate at
H t
45 % and 37 o C : simulated curves of this work, as indicated, and experimental points: Whole
blood: green crosses - Merrill et al. [76]; black circles - Chien et al. [77], black squares - Skalak
et al. [78]. Ringer ES: red circles - Chien et al. [77]; red squares - Skalak et al. [78]. (b) Plot of
relative viscosity as a function of hematocrit ( H t ) at shear rates 0
=
0 (blue) s 1 :
simulated (LD-RBC points), and Chien et al. [77] experimental fits for whole blood (solid lines)
and Ringer ES (dashed lines) (from [61])
.
052 (black) and 52
.
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