Gain: Difference between revisions

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Related wiki pages [[Antennas]], [[Antenna Design]], [[Radiated Power Measurement]], [[SWR]]
Related wiki pages [[Antennas]], [[Antenna Design]], [[Decibels]], [[Radiated Power Measurement]], [[SWR]]


==What is Gain?==
==What is Gain?==
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=== Gain compared to a half wave dipole - dBD===
=== Gain compared to a half wave dipole - dBD===


The gain of an antenna is the relative increase in radiation at the maximum point expressed as a value in dB above a standard. The standard to which other antennas are compared is usually a ½-wavelength dipole. The standard antenna is given a reference gain of 0dBD (zero decibel referenced to dipole). This comes from:
The gain of an antenna is the relative increase in radiation at the maximum point expressed as a value in [[Decibels | dB ]] above a standard. The standard to which other antennas are compared is usually a ½-wavelength dipole. The standard antenna is given a reference gain of 0dBD (zero decibel referenced to dipole). This comes from:


<math> \mbox{gain} = 10 \times \log \left( \frac {Pe}{Pi} \right) </math>
<math> \mbox{gain} = 10 \times \log \left( \frac {Pe}{Pi} \right) </math>

Revision as of 16:14, 4 April 2009

Related wiki pages Antennas, Antenna Design, Decibels, Radiated Power Measurement, SWR

What is Gain?

Gain compared to a half wave dipole - dBD

The gain of an antenna is the relative increase in radiation at the maximum point expressed as a value in dB above a standard. The standard to which other antennas are compared is usually a ½-wavelength dipole. The standard antenna is given a reference gain of 0dBD (zero decibel referenced to dipole). This comes from:

<math> \mbox{gain} = 10 \times \log \left( \frac {Pe}{Pi} \right) </math>

Where Pe is effective radiated power and Pi is input power

An antenna with the effective radiated power of three times the input power would therefore have a gain of:

Pe = 3, Pi = 1

<math> 10 \times \log \left( \frac {3}{1} \right) = 4.77\mbox{dBD} </math>

Gain compared to an isotropic readiator = dBi

An isotropic radiator is a theoretical "point source" antenna that radiates the same amount of energy in all directions. Although an isotropic antenna cannot be constructed, it is sometimes useful to compare actual antennas to it.

Comparison of dBD and dBi

Graphically, the radiation patterns of isotropic and dipole antennas - for equal power inputs - can be represented thus:

Vk4yeh dbi vs dbd.jpg

The area between the isotropic radiator circle and the half wave circle radiator circle represents a gain difference of approximately 2.15dB

hence, <math> dBi = dBD + 2.15 </math>