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Rev 2.02<br />
E9A10<br />
Antenna bandwidth is the frequency range over which an antenna satisfies a performance requirement.<br />
Performance examples would be – Gain - SWR or impedance - Beam width - etc<br />
E9A11<br />
Antenna efficiency is calculated by (radiation resistance / total resistance) x 100%.<br />
Can also be calculated by the equation: Efficiency = Radiated Power / Input power<br />
E9A12<br />
The efficiency of an HF quarter-wave grounded vertical antenna can be improved by installing a good radial<br />
system.<br />
E9A13<br />
Soil conductivity is the most important factor in determining ground losses for a ground-mounted vertical antenna<br />
operating in the 3-30 MHz range.<br />
E9A14<br />
If an antenna has 3.85 dB gain over a 1/2-wavelength dipole then it has 6 dB gain over an isotropic antenna.<br />
The gain over isotropic source for an antenna with a 3.85 dB gain over a dipole antenna would be an additional<br />
2.14 dB of gain. Remember dipole gain over an isotropic source is 2.14 dB or 3.85 dB +1.14dB or 5.99dB<br />
E9A15<br />
An antenna has 9.85 dB of gain over a 1/2-wavelength dipole when it has 12 dB of gain over an isotropic antenna.<br />
Remember that a dipole has 2.14 dB of gain as referenced to an isotropic antenna.<br />
12 dB -2.14 dB or gain =9.86dB<br />
E9A16<br />
The radiation resistance of an antenna is the value of a resistance that would dissipate the same amount of power<br />
as that radiated from an antenna.<br />
E9B - Antenna patterns: E and H plane patterns; gain as a function of pattern; antenna design (computer<br />
modeling of antennas); Yagi antennas<br />
E9B01<br />
The orientation of its electric field (E Field) determines the free-space polarization of an antenna.<br />
Jack Tiley <strong>AD7FO</strong> Page 87 3/15/2009