Biomedical Engineering Reference
In-Depth Information
4.4.3
Contact vs No-Contact
We discuss now on the possibility of contacts in weak and classical solutions to
(FRBI). This question is tackled by Vázquez and Zuazua [ 61 ] on the following one-
dimensional baby-model introduced in [ 60 ]:
8
<
@ t u C u @ x u @ xx u D 0; in R nfh i .t/g i D 1;:::;n
u .t;h i .t// D h i .t/; for i D 1;:::;n;
Œ@ x u .t;h i .t// D m i h i .t/; for i D 1;:::;n:
(4.77)
:
In this system the h i 's stand for the position of the bodies (which are points in
the one-dimensional case). For simplicity, we assume that they are numbered in
increasing order: h i <h i C 1 . The two last equations mimic the no-slip boundary
conditions and body dynamics, respectively. We used the convention that:
Πu .t;h/ D
x ! h;x>h u .t;x/
lim
x ! h;x<h u .t;x/;
lim
8 t>0; 8 h 2 R :
In the first equation, of viscous Burgers type, we introduced the parameter >0
which stands for the viscosity of the fluid, and 2 R a dimensionless parameter.
For this system, J.L. Vázquez and E. Zuazua prove among other results that,
whatever the choice of the initial data:
2 L 2 . R /; .h i ; h i / 2 R 2n ; s.t.
u 0
i 2f 1;:::;n 1 g jh i C 1 h i j >0;
inf
the system ( 4.77 ) admits a unique global solution in which no contact between rigid
bodies occurs in finite time:
i ¤ j jh i C 1 .t/ h i .t/j >0;
inf
8 t>0:
In this one-dimensional case, the regularity estimate for classical solutions yields
the bound:
Z T
" n 1
2 # dt<C 0 .T/;
Z h i C 1 .t/
X
X
n
m i j h i j
2 d z C
j@ xx u .t; z /j
(4.78)
0
h i .t/
i D 1
i D 1
where C 0 depends on initial data and T only. Applying classical arguments to
the no-slip boundary condition seen as a differential equation, this control on
@ xx u induces that h i C 1 might not collide h i in finite time. The result extends
to the case of L 2 initial data due to the classical smoothening properties of the
viscous Burgers equations. In the multi-dimensional case, the regularity estimate
for solutions to (FRBI) relies on ellipticity of the Stokes problem which depends
itself on the minimal distance between two rigid boundaries (see [ 15 , Sect. 4.1]).
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