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see Theorem A.1 in Vogelius [1983]. Following the usual procedure (see, e.g.,
Theorem III.4.5) we have
2 µ(ε(u h
+
( div v, p h
=
P h u), ε(v)) 0
Q h p) 0
u ,v
for all v
X h ,
λ 1 (p h Q h p, q) 0
for all q M h .
The functionals u and p can be expressed in terms of u P h u and p Q h p . From
the estimates (3.32) and (3.33) we immediately obtain
( div (u h P h u), q) 0
= p ,q
u 1 + p 0 ch f 0 .
Hence,
u u h 1 + λ div u p h 0 ch f 0 , ( 3 . 34 )
where c is a constant independent of λ . The finite element method (3.31) h is robust.
Nonconforming methods are also very popular for treating nearly incom-
pressible materials. The finite element discretization (3.31) h of the saddle point
problem can also be interpreted as a nonconforming method, and this discretiza-
tion will serve as a model for analyzing nonconforming methods for the problem
with a small parameter.
H 1
3.9 Remark.
L 2 () be the solution of
the finite element discretization (3.31) h . Define a discrete divergence operator by
div h : H 1 () M h
( div h v, q) 0 = ( div v, q) 0
Let u h
X h
() and p h
M h
( 3 . 35 )
for all q M h .
Then u h is also the solution of the variational problem
2 µ ε(v)
2
0
2
0
+ λ
div h v
, v −→
min
v X h
!
( 3 . 36 )
Indeed, the solution u h of (3.36) is characterized by
2 µ(ε(u h ), ε(v)) 0 + λ( div h u h , div h v) 0 = , v
for all v X h .
Setting p h :
= λ div h u h by analogy to (3.30), we have
2 µ(ε(u h ), ε(v)) 0 + ( div h v, p h ) 0 = , v
for all v X h ,
λ 1 (p h ,q) 0
M h .
Here the operator div h is met only in inner products with the other factor in M h .
Now, from the definition (3.35) we know that the operator div h may be replaced
here by div. Therefore, u h together with p h :
( div h u h ,q) 0
=
0
for all q
λ div h u h satisfy (3.31) h .
We turn to the analysis of (3.36). The inequality (3.32) 2 implies the estimate
=
div v 1 , but in most of the nonconforming methods there
is only a weaker estimate available. Moreover, the discrete divergence does not
result from an orthogonal projection in many cases. A basis for an alternative is
offered by the following regularity result in Theorem 3.1 of Arnold, Scott, and
Vogelius [1989]. Given u with div u H 1 (), there exists w H 2 () H 0 ()
such that
div v
div h v 0 ch
div w = div u and w 2 c div u 1 .
( 3 . 37 )
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