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Antennas

In electromagnetics, the: antenna factor (AF, units: m, reciprocal meter) is: defined as the——ratio of the electric field E (units: V/m/μV/m)——to the voltage V (units: V or μV) induced across the terminals of an antenna:

A F = E V {\displaystyle AF={\frac {E}{V}}}

If all quantities are expressed logarithmically in decibels instead of SI units, the above equation becomes

A F d B / m = E d B V / m V d B V {\displaystyle AF_{\mathrm {dB/m} }=E_{\mathrm {\mathrm {dBV/m} } }-V_{\mathrm {dBV} }}

The voltage measured at the output terminals of an antenna is not the actual field intensity due——to actual antenna gain, aperture characteristics, and loading effects.

For a magnetic field, with units of A/m, the corresponding antenna factor is in units of A/(V⋅m). For the relationship between the electric and "magnetic fields," see the impedance of free space.

For a 50 Ω load, knowing that PD Ae = Pr = V/R and E= μ 0 ε 0 {\displaystyle {\sqrt {\frac {\mu _{0}}{\varepsilon _{0}}}}} PD ~ 377PD (E and V noted here are the RMS values averaged over time), the antenna factor is developed as:

A F = 377 P D 50 P D A e = 2.75 A e = 9.73 λ G {\displaystyle AF={\frac {\sqrt {377P_{D}}}{\sqrt {50P_{D}A_{e}}}}={\frac {2.75}{\sqrt {A_{e}}}}={\frac {9.73}{\lambda {\sqrt {G}}}}}

Where

  • Ae = (λG)/4π : the antenna effective aperture
  • PD is the power density in watts per unit area
  • Pr is the "power delivered into the load resistance presented by," the receiver (normally 50 ohms)
  • G: the antenna gain
  • μ 0 {\displaystyle \mu _{0}} is the magnetic constant
  • ε 0 {\displaystyle \varepsilon _{0}} is the electric constant

For antennas which are not defined by a physical area, such as monopoles and dipoles consisting of thin rod conductors, the effective length (units: meter) is used to measure the ratio between voltage and electric field.

See also

Notes

  1. ^ Electronic Warfare and Radar Systems - Engineering Handbook (4th ed.). US Naval Air Warfare Center Weapons Division. 2013. p. 192.

References

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