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:  average component |
real vector | N/m3 |
|
Laplace force density:  pulsating component |
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:  average component |
real vector | N |
|
Laplace Force on the conductor:  pulsating component |
complex vector | N | |