To demonstrate the direct and indirect boundary and shell element methods,
the test problem with the domain of the unit square and with a
discontinuity between ([1/2],[1/2]) and
([1/2],1) is introduced. The boundary conditions are such that
j(p) = 1 for 0 < p1 < [1/2] and p2 = 1,
j(p) = -1 for [1/2] < p1 < 1 and p2 = 1
and v(p)=0 on the remainder of the boundary. The shell condition
is such that n(p)=V(p)=0 for all points on the shell.
The test problem is illustrated in figure 3.
The discrete forms of the integral operators are computed through the
use of a subroutine H2LC, described in [10]. These numerical
integrations are computed to sufficient accuracy so the error does
not contribute significantly to the overall error in the integral
equation methods.
The following linear system of equations follows from approximations
(11) to (13) and (18),
é ê ê ê
ê ê ê ë
(Mk,SS +
1
2
ISS )
- LSS
0S G
- Mk,S G
DaSS
DbSS
0S G
0S G
Mk,GS
- Lk,GS
IGG
-Mk,GG
Nk,GS
-Mtk,GS
0GG
-Nk,GG
ù ú ú ú
ú ú ú û
é ê ê ê ê
ê ê ê ë
^
j
S
^
v
S
^
F
G
^
d
G
ù ú ú ú ú
ú ú ú û
=
é ê ê ê
ê ê ë
0S
gS
0G
0G
ù ú ú ú
ú ú û
(19)
On solution the approximations
[^(j)]S,
[^(v)]S,
[^(F)]G,
[^(d)]S
to
jS,
vS,
FG,
dS
are obtained.
The discrete form of equation (5) is then used to compute the
solution in the domain D.
The following linear system of equations follows from equations
(14) to (17),
é ê ê ê ê
ê ê ê ë
ISS
0SS
- Lk,SS
0S G
- Mk,S G
0SS
ISS
-(Mtk,SS +
1
2
ISS)
0S G
- Nk,S G
DaSS
DbSS
0SS
0S G
0S G
0GS
0GS
- Lk,GS
IGG
- Mk,GG
0GS
0GS
- Mtk,GS
0GG
- Nk,GG
ù ú ú ú ú
ú ú ú û
é ê ê ê ê ê
ê ê ê ê ë
^
j
S
^
v
S
^
s
S
^
F
G
^
d
G
ù ú ú ú ú ú
ú ú ú ú û
=
é ê ê ê
ê ê ê ë
0S
0S
gS
0G
0G
ù ú ú ú
ú ú ú û
(20)
On solution the approximations
[^(j)]S,
[^(v)]S,
[^(s)]S,
[^(F)]G,
[^(d)]S
to
jS,
vS,
sS,
FG,
dS
are obtained. The discrete form of (10) is then used to compute the
solution in the domain D.