 ), found under the Radio Frequency branch (
), found under the Radio Frequency branch ( ) when adding a physics interface, is used to solve a time-domain wave equation for the magnetic vector potential. The sources can be in the form of point dipoles, line currents, or incident fields on boundaries or domains. It is primarily used to model electromagnetic wave propagation in different media and structures when a time-domain solution is required — for example, for non-sinusoidal waveforms or for nonlinear media. Typical applications involve the propagation of electromagnetic pulses.
) when adding a physics interface, is used to solve a time-domain wave equation for the magnetic vector potential. The sources can be in the form of point dipoles, line currents, or incident fields on boundaries or domains. It is primarily used to model electromagnetic wave propagation in different media and structures when a time-domain solution is required — for example, for non-sinusoidal waveforms or for nonlinear media. Typical applications involve the propagation of electromagnetic pulses.| • | Three-component vector (the default) to solve using a full three-component vector for the electric field E. | 
| • | Out-of-plane vector to solve for the electric field vector component perpendicular to the modeling plane, assuming that there is no electric field in the plane. | 
| • | In-plane vector to solve for the electric field vector components in the modeling plane assuming that there is no electric field perpendicular to the plane. | 
| Transient Modeling of a Coaxial Cable: Application Library path RF_Module/Verification_Examples/coaxial_cable_transient |