Technical Notes   

Radiated Fields

When HFSS calculates radiation fields, the values of the fields over the radiation surface are used to compute the fields in the space surrounding the device. This space is typically split into two regions — the near-field region and the far-field region. The near-field region is the region closest to the source. In general, the electric field E(x,y,z) external to the region bounded by a closed surface may be written as

(1)

where

• s represents the radiation boundary surfaces.

• j is the imaginary unit,.

• w is the angular frequency, 2pf.

• m₀ is the relative permeability of the free space, 4p´10^-7 Wb/Am.

• H_tan is the component of the magnetic field that is tangential to the surface.

• E_normal is the component of the electric field that is normal to the surface.

• E_tan is the component of the electric field that is tangential to the surface.

• G is the free space Green’s function, given by

(2)

where

• k₀ is the free space wave number,

• r and represent field points and source points on the surface, respectively.

• e₀ is the permittivity of free space, 1/(c²m₀)

• e_r is the relative permittivity of a dielectric.

• m_r is the relative permeability of a dielectric.

This r dependence is characteristic of a spherical wave, a key feature of far fields. The far field is a spherical TEM wave with the following equation:

(3)

 

where h₀ is the intrinsic impedance of free space, .

You can select the material in which the objects are embedded (the default is vacuum). In that case, the Green's function and the intrinsic impedance of that material will be used, so the far field will be correct. See Global Material Environment.

When calculating the near fields, HFSS uses the general expressions given in (Assigning Boundaries

Assigning Excitations

Spherical Cross-Sections

Maximum Near Field Data

Selecting a Far Field Quantity to Plot