The Electromagnetic Waves, Transient Interface
The Electromagnetic Waves, Transient (temw) interface (), 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 this physics interface is added, these default nodes are also added to the Model BuilderWave Equation, Electric, Perfect Electric Conductor, and Initial Values. Then, from the Physics toolbar, add other nodes that implement, for example, boundary conditions and mass sources. You can also right-click Electromagnetic Waves, Transient to select physics features from the context menu.
Except where indicated, most of the settings are the same as for The Electromagnetic Waves, Frequency Domain Interface.
Settings
The Label is the default physics interface name.
The Name is used primarily as a scope prefix for variables defined by the physics interface. Refer to such physics interface variables in expressions using the pattern <name>.<variable_name>. In order to distinguish between variables belonging to different physics interfaces, the name string must be unique. Only letters, numbers and underscores (_) are permitted in the Name field. The first character must be a letter.
The default Name (for the first physics interface in the model) is temw.
Components
This section is available for 2D and 2D axisymmetric components.
Select the Electric field components solved for. Select:
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.
Dependent Variables
The dependent variable (field variable) is for the Magnetic vector potential A. The name can be changed but the names of fields and dependent variables must be unique within a model.
Discretization
To display this section, click the Show button () and select Discretization.
Transient Modeling of a Coaxial Cable: Application Library path RF_Module/Verification_Examples/coaxial_cable_transient