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Model Decomposition

Numerically efficient equivalent sources for complex sources and receivers.

Sources

aperture_field.pngAperture field

Aperture excitations may be used to specify a planar, cylindrical or spherical aperture of measured or calculated field values that are impressed as an excitation. The field values are converted into an equivalent array of electric and magnetic dipoles in the solution.

spherical_modes.pngSpherical modes

An impressed spherical mode excitation can be defined based on pre-calculated spherical modes.  These spherical modes are either radiating to infinity or incident onto a structure , i.e. converging on the coordinate system origin.

This excitation option can thus be used for both the synthesis of an arbitrary electromagnetic field and also for the determination of the response of a receiving antenna due to the incident modes.

radiation_pattern.pngRadiation pattern

The radiation pattern of an antenna may be used as an impressed source from a particular point in space.  This radiation pattern may be imported from measured data or from pre-computed far-field solutions.

Receivers

The respective ideal receiving antennas form the receiving complement to the respective impressed sources.  Ideal receiving antennas are good domain decomposition tools when the following assumptions are made:

  • The antenna is considered to be matched (i.e. no mismatch loss is taken into account)
  • The antenna and model are assumed to have no impact on each other during the solution phase (no coupling is taken into account)

 

rx_antenna_farfield.pngFar-field antenna

The antenna exists at a particular point in space and has spatial receiving properties of a far-field pattern imported from simulated or measured data.

rx_antenna_nearfield.pngNear-field antenna

The antenna consists of near-field apertures that serve as weights for receiving energy via the specified aperture points.

receiving_antenna_spherical_modes.pngSpherical modes

Similar to the far-field antenna, a spherical mode antenna exists at a particular point in space, but is defined by spherical modes, rather than a far-field pattern.  The combination of the spherical modes effectively define how energy incident upon it is received by the antenna from any particular direction.