The Transition Boundary Condition is used on interior boundaries to model a sheet of a medium that should be geometrically thin but does not have to be electrically thin. It represents a discontinuity in the tangential electric field. Mathematically it is described by a relation between the electric field discontinuity and the induced surface current density:
The Surface Roughness and
Surface Current Density subnodes are available from the context menu (right-click the parent node) or from the
Physics toolbar,
Attributes menu.
Select an Electric displacement field model —
Relative permittivity (the default),
Refractive index,
Loss tangent, loss angle,
Loss tangent, dissipation factor,
Dielectric loss,
Drude-Lorentz dispersion model, or
Debye dispersion model. See the
Wave Equation, Electric node,
Electric Displacement Field section, for all settings.
Select the Electrically thick layer check box (cleared by default) to make the two domains adjacent to the boundary uncoupled. Use this setting, for instance, when the thickness is greater than three times of the skin depth. When the
Electrically thick layer check box is cleared, enter a
Thickness d (SI unit: m). The default is 0.01 m.
Select a Defined by option —
Electrical conductivity (default) or
Resistivity. Enter a
Electrical conductivity σ (SI unit: S/m), Relative permittivity
εr, Relative permeability
μr of the material to be evaluated, and frequency
f0 (SI unit: Hz). Then click the
Compute Skin Depth button to compute the skin depth for the particular material specified by the above input values. The result is displayed in the settings window below the
Compute Skin Depth button
.