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The effective antenna noise figure F a for a vertical loop antenna and its application to extremely low frequency/very low frequency atmospheric noise
Author(s) -
FraserSmith Antony C.
Publication year - 2007
Publication title -
radio science
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.371
H-Index - 84
eISSN - 1944-799X
pISSN - 0048-6604
DOI - 10.1029/2005rs003387
Subject(s) - noise (video) , atmospheric noise , antenna (radio) , physics , noise figure , very low frequency , acoustics , loop antenna , antenna noise temperature , noise temperature , atmospherics , optics , computational physics , telecommunications , antenna factor , infrasound , antenna measurement , computer science , phase noise , meteorology , bandwidth (computing) , amplifier , astronomy , artificial intelligence , image (mathematics)
Expressions tabulated for the effective antenna noise figure F a usually assume an electric field antenna, since most measurements of radio noise are made on the electric field of the noise. Furthermore, the International Radio Consultative Committee (CCIR) noise model predictions for F a are made only for electrically short grounded vertical monopoles over a perfect ground. However, at frequencies lower than those traditionally used for communications, i.e., at extremely low frequencies (ELF; frequencies in the range 3 Hz to 3 kHz) and very low frequencies (VLF; frequencies in the range 3–30 kHz), it is common for magnetic field loop antennas to be used, and the tabulated expressions for F a do not apply. This communication reports the derivation of an expression for F a as measured by a small vertical magnetic loop antenna and its subsequent application to ELF/VLF radio noise measurements made at a variety of locations around the world. There is good agreement between the measured F a values and estimates of maximum and minimum F a values for the ELF/VLF range published by Spaulding and Hagn in 1978, but an improved fit to the measurements can be obtained by making moderate adjustments to the maximum and minimum values at both the low (10–100 Hz) and high (8–32 kHz) frequency limits.