Supplied conductors application: post-processing quantities
Solving process: reminder
With the application Supplied conductors, the solving process requires two steps, as presented in the table below.
PEEC computation (independent on the application) |
---|
computation of resistances and partial self-inductances (R, L) of each
element of the conductor, computation of partial mutual inductances (M) among all the parallel elements of the conductor |
Computation of the current |
---|
solving the electric equations ⇒ value of the current in each element |
Post-processing |
---|
magnetic flux density, Joule losses, Laplace force,… |
Local quantities
The local quantities issued from computation are presented in the table below.
Quantity | Unit | Explanation | |
---|---|---|---|
Current density in conductors: ![]() |
complex vector | A/m2 | |
Magnetic flux density: ![]() |
complex vector | T | Analytical (or semi- analytical): Biot and Savart |
Power losses density in conductors (by Joule effect): dP | real scalar | W/m3 |
![]() |
Laplace force density: ![]() |
real vector | N/m3 |
![]() |
Laplace force density: ![]() |
complex vector | N/m3 |
Global quantities
The global quantities issued from the computation are presented in the table below.
Quantity | Unit | Explanation | |
---|---|---|---|
Total current carrying the conductor: ![]() |
complex scalar | A |
![]() |
Power losses in the conductor (by Joule effect): P | real scalar | W |
![]() |
Laplace Force on the conductor: ![]() |
real vector | N |
![]() |
Laplace Force on the conductor: ![]() |
complex vector | N |