List of Field Quantities in 2D Extractor
The following field quantities are available in 2D Extractor, depending on the solution.
CG Fields
| Phi | |
|
Mag_Phi |
The magnitude of Phi. |
|
PhiAtPhase |
The real part of Phi at a particular value of phase. |
| E | |
|
VectorE |
The electric field. This is a complex vector quantity. |
|
Mag_E |
The magnitude of E. |
| J | |
| Mag_Jcg | The magnitude of Jcg. |
|
VectorJcg |
The conduction current density vector. This is the material conductivity multiplied by the electric field vector E. |
| Other | |
|
EnergyCG |
The energy density of the electric fields. |
R/L Fields
| A | |
|
VectorA |
The magnetic vector potential. This is a complex vector quantity. |
|
Flux_Lines |
A plot showing contours of constant magnitude of A. |
| B | |
|
VectorB |
The magnetic flux density vector. This is a complex vector quantity. |
|
Mag_B |
The magnitude of B. |
| H | |
|
VectorH |
The magnetic field vector. This is a complex vector quantity. |
|
Mag_H |
The magnitude of H. |
| J | |
|
VectorJrl |
The conduction current density. |
|
Jrl |
The magnitude of VectorJrl. |
| Other | |
|
Emloss |
In RL solution, emloss combines the ohmic loss and dielectric loss. Emloss is represented by:
|
|
EdgeLossDensity |
Edge loss density represents losses associated with impedance boundary applied on conductive surfaces on the boundary of the solution domain or on surface of excluded objects. It assumes an exponential spatial decay (toward the interior of the respective material) of induced current magnitudes and of associated losses. Integrating the loss along the edge produces the entire loss associated with the "edge." It is represented by:
|
|
EnergyRL |
The energy density of the magnetic fields, as represented by:
|
|
Temperature_RL |
Temperature distribution imported from a thermal solver such as Ansys Mechanical. |