Antenna Unit Converter & Field Calculator
Every conversion you need when moving between a datasheet and a link budget or an EMC report: dBi and dBd, antenna factor, effective aperture, EIRP and ERP, field strength in V/m and dBµV/m, power density, and where the far field of your antenna actually begins.
dBi, dBd, antenna factor and effective aperture
Gain in dBi is measured against an isotropic radiator, while dBd is measured against a half-wave dipole. A half-wave dipole has 2.15 dBi of gain, so dBi = dBd + 2.15. Gain also fixes the effective aperture, Ae = G·λ²/4π: for the same gain, a lower frequency means a physically larger aperture. EMC engineers prefer antenna factor, AF = E/V in dB/m. For a 50 Ω receiver, AF(dB/m) = 20·log10(f in MHz) − G(dBi) − 29.79, so a 0 dBi antenna at 2.4 GHz has an AF of about 37.8 dB/m.
EIRP, ERP and field strength
EIRP is the power an isotropic radiator would need to radiate to produce the same field in the peak direction: transmit power minus feed loss plus antenna gain in dBi. ERP uses the dipole as reference, so ERP = EIRP − 2.15 dB. In free space the power density at distance d is S = EIRP/4πd², and the electric field is E = √(30·EIRP)/d. To report in EMC units, E in dBµV/m = 20·log10(E in V/m) + 120.
Where does the far field start?
The commonly used boundary is the Fraunhofer distance 2D²/λ, at which the phase error across the aperture is 22.5°. Closer in, the radiating near field (Fresnel region) has a pattern that depends on distance, and very close to the antenna the reactive near field stores energy rather than radiating it. Gain and pattern measurements, and the free-space formulas on this page, are only valid in the far field. For electrically small antennas the practical limit is a few wavelengths rather than 2D²/λ.