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where
2
2
1
2
v) i 1 ,i 2 :=
1 Q kk x k x k v) i 1 ,i 2 + Q 12 x 1 x 2 v) i 1 ,i 2
μ k x k v) i 1 ,i 2 .
(
F
k =
k =
1
We write ( 8.15 ) in matrix form. Setting, for N := N 1 N 2 ,
u m
(u 1 ,...,u N ) ,
u N 2 (i 1 1 ) + i 2 :=
v i 1 ,i 2 ,
=
=
j
we find that ( 8.15 ) is equivalent to
Find u m + 1
N
∈ R
such that for m
=
0 ,...,M
1 ,
I
θt G BS u m + 1
= I
θ)t G BS u m ,
(8.16)
+
( 1
u 0
= u 0 ,
where the matrices I and G BS
are given by
I 1
I 2 ,
I
:=
1
2 Q 11 R 1
1
2 Q 11 I 1
G BS
I 2
Q 12 C 1
C 2
R 2
:=
+
+ μ 1 C 1
I 2
+ μ 2 I 1
C 2
+ r I 1
I 2 .
Herewith, we denote by R k , C k , I k
N k ×
N k , the matrices given in (4.14) with
∈ R
respect to the coordinate direction x k , k
=
1 , 2.
8.4.2 Finite Element Discretization
In the two-dimensional case, the bilinear form a BS (
·
,
·
) in ( 8.9 ) simplifies to
1 Q k
μ k
r
2
2
1
2
a BS (ϕ, φ)
=
x ϕ∂ x k φ d x
+
x k ϕφ d x
+
ϕφ d x.
G
G
G
,k
=
k
=
1
(8.17)
The discretization of the weak formulation ( 8.13 ) relies on finite element spaces
V N H 0 (G) which are spanned by products of hat-functions. To be more precise,
for N 1 ,N 2 ∈ N
we consider
V N :=
span
{
ϕ j (x 1 ,x 2 )
|
1
j
N 1 N 2 }
=
span
{
ϕ N 2 (i 1 1 ) + i 2 (x 1 ,x 2 )
|
1
i k
N k ,k
=
1 , 2
}
=
span
{
b i 1 (x 1 )b i 2 (x 2 )
|
1
i k
N k ,k
=
1 , 2
}
,
(8.18)
where b i k (x k ) are the univariate hat-functions as in (3.18). Note that dim V N = N :=
N 1 N 2 . If the mesh sizes h k =
2 R/(N k +
1 ) in both coordinate directions are con-
h 1
k
stant, we have b i k (x k ) =
max
{
0 , 1
| x k x k,i k |}
, i k =
1 ,...,N k , with mesh
points x k,i k := − R + h k i k , i k =
0 ,...,N k +
1.
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