Biomedical Engineering Reference
In-Depth Information
FS interface displacement at t = 1 ms
FS interface displacement at t = 6 ms
FS interface displacement at t = 12 ms
0.52
0.52
0.52
fluid−thick structure
fluid−thin−thick structure
0.51
0.51
0.51
0.5
0.5
0.5
0
2
4
6
0
2
4
6
0
2
4
6
z axis (cm)
z axis (cm)
z axis (cm)
FS interface velocity at t = 1 ms
FS interface velocity at t = 12 ms
FS interface velocity at t = 6 ms
10
10
10
5
5
5
0
0
0
−5
−5
−5
−10
−10
−10
0
2
4
6
0
2
4
6
0
2
4
6
z axis (cm)
z axis (cm)
z axis (cm)
Fig. 2.20 Fluid-structure interface displacement ( top ) and velocity ( bottom ) obtained using a
multi-layered wall model and the single-layered model from [ 22 ], shown at times t D 1 ms,
t D 6 ms, and t D 12 ms
Fig. 2.21 Regularizing effects of point mass. These figures originally appeared as Fig. 1 and Fig. 2
(left) in [ 107 ] and are reprinted by permission of c American Mathematical Society 2014. The
initial data ( left panel ) is smoothed out as the transmitted wave traveling to the right passes through
the point mass ( right panel )
form. The transmitted wave, which passes through the point mass, gets smoothed
out to H 2 .0;L/ regularity in displacement, and H 1 .0;L/ regularity in velocity. A
numerical simulation of this phenomenon was shown in [ 107 ]. Figure 2.21 shows
one of the results from [ 107 ]. The panel on the left shows the initial displacement
in H 1 .0;L/ with zero initial velocity, located just left from the point mass. The
panel on the right shows the solution at time T D 10s at which the reflected
and transmitted waves have formed, with the displacement of the reflected wave
on the left of the point mass still in H 1 .0;L/, but with the displacement of the
transmitted wave, shown to the right of the point mass, belonging to H 2 .0;L/.For
a reader with further interest in the area of simplified coupled problems we mention
[ 91 , 123 , 134 , 145 ].
2.8
Conclusions
This chapter addresses an operator splitting approach to study multi-physics prob-
lems related to FSI with application to hemodynamics. The methodology is based on
 
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