Biomedical Engineering Reference
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u
condition
D 0. Furthermore, since is not a Lipschitz function, the
ALE mapping is not necessarily a Lipschitz function either, and, as a result, u is
not necessarily an H 1 function on F . Therefore we need to redefine the function
spaces for the fluid velocity by introducing
r
F Df u
V
W u 2 V F .t/g;
where u is defined in ( 2.108 ). Under the assumption 1 C . z />0, z
2 Œ0;1,the
F :
following defines a scalar product on
V
Z
.1 C / u
v D . u ; v / H 1 . F .t// :
. u ; v /
v
u
D
Cr
Wr
F
V
F
F ,so
F is
u is an isometric isomorphism between
Therefore, u
7!
V F .t/ and
V
V
F .0;T/ and
.0;T/ are defined as
also a Hilbert space. The function spaces
W
W
F instead
before, but with
V
V F .t/. More precisely:
F .t//;
F .0;T/ D L 1 .0;T I L 2 . F // \ L 2 .0;T I V
W
(2.136)
F .0;T/ W W .0;T/ W S .0;T/ W
u .t; z ;1/D @ t .t; z / e r ;.t; z / D d.t; z ;1/g:
W .0;T/ Df. u ;;d/ 2 W
(2.137)
The corresponding test space is defined by
F V W V S / W
q .t; z ;1/D .t; z / e r ; .t; z ;1/D .t; z / e r g:
Q .0;T/ Df. q ; ; / 2 C c .Œ0;T/I V
(2.138)
.0;T/ is a weak solution of prob-
lem ( 2.111 )-( 2.118 ) defined on the reference domain F ,ifforevery. q ; ; / 2
Q .0;T/ the following equality holds:
Definition 2.2. We s a y t h a t . u ;;d/ 2 W
Z T
Z
Z T
b . u ; u ; q /C2 Z T
0
Z
.1 C / D . u / W D . q /
.1 C / u @ t q C
0
F
0
F
Z T
Z
Z T
Z 1
Z T
Z 1
1
2
.@ t / u q
@ t @ t C
@ z @ z
0
F
0
0
0
0
Z T
Z
Z T
@ t d @ t C
a S .d; /
0
S
0
Z T
0 hF.t/; q i in=out C
Z
Z 1
Z
D
u 0 q .0/ C
v 0 .0/ C
V 0 .0/:
0
0
S
(2.139)
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