fS![]() |
= | ![]() |
+ | q . n0 . V0 | ![]() |
0 | ||
fS![]() |
= | ![]() |
+ | ![]() |
+ | q . n1 . V1 | = | 0 |
![]() |
||||||||
fSn0 | = | I01 | ![]() |
0 | ||||
fSn1 | = | I10 | + | I12 | = | 0 | ||
![]() |
![]() |
= |
![]() ![]() ![]() |
= |
- ![]() |
Iij | = |
I(ni, nj,![]() ![]() |
= | - Iji |
At the boundary, the constitutive relations are
f![]() |
= | ![]() |
- | ![]() |
= | 0 |
fn0 | = | n0 | - | N0 | = | 0 |
fIC | = | IC | + | fSn0 | = | 0 |
fQC | = | QC | + |
fS![]() |
= | 0 |
The boundary constitutive relations will be used to determine the quantity
values at the boundary while the segment constitutive relations will be used to build up an
expression for the boundary charge QC and for the boundary current
IC. This is achieved by the boundary models which set the appropriate
entries in the transformation matrix
B which reads
tx, y | ![]() |
![]() |
n0 | n1 | IC | QC |
![]() |
||||||
![]() |
1 | |||||
n0 | ||||||
n1 | 1 | |||||
IC | 1 | |||||
QC | 1 |
The solution vector x contains the following quantities
x | = |
![]() ![]() ![]() ![]() ![]() |
For voltage controlled contacts with V0 applied to the contact one gets
f![]() |
= | ![]() |
- | V0 | = | 0 |
When applying the current I0 to the contact
f changes to
f![]() |
= | IC | - | I0 | = | 0 |
The system matrix for iteration step k is
jx, y | ![]() |
n0 | ![]() |
IC | QC | r |
![]() |
-1 | 1 |
f![]() |
|||
n0 | -1 | fn0k | ||||
![]() |
-1 |
f![]() |
||||
IC |
- ![]() |
- ![]() |
-1 | fICk | ||
QC |
- ![]() |
-q . V0 | -1 | fQCk |
As the constitutive relations for the quantities , n0, and IC
are eliminated first, one ends up with the following matrix
jx, y | ![]() |
r |
![]() |
- ![]() |
f![]() ![]() ![]() ![]() |