Gain: Difference between revisions

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Related wiki pages [[Antennas]], [[Antenna Design]], [[Decibels]], [[Radiated Power Measurement]], [[SWR]]
==What is Gain?==
==What is Gain?==


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:
=== Gain compared to a half wave dipole - dBD===


gain = <math> 10*log(\frac {Pe}{Pi}) </math>
The gain of an antenna is the relative increase in radiation at the maximum point expressed as a value in [[Decibels | 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>


Where '''Pe''' is effective radiated power and '''Pi''' is input power
Where '''Pe''' is effective radiated power and '''Pi''' is input power
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An antenna with the effective radiated power of three times the input power would therefore have a gain of:
An antenna with the effective radiated power of three times the input power would therefore have a gain of:


<math> 10*log(\frac {3}{1}) </math> = 4.77dBD.
''Pe'' = 3,  ''Pi'' = 1
 
<math>10\times\log\left(\frac {3}{1}\right) = 4.77\mbox{dBD} </math>
 
===Gain compared to an isotropic radiator = 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:
 
[[image:Vk4yeh_dbi_vs_dbd.jpg |400px]]
 
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>
 
===Comparative gain of various antenna types===
 
{| width="750" border="1" cellpadding="6"
| Antenna Type
| dB gain over isotropic radiator
| dB gain over half-wave dipole
|-
| Isoptropic radiator
| 0
| -2.1
|-
| Ground plane
| +0.3
| -1.8
|-
| half-wave dipole
| +2.1
| 0
|-
| 5/8 wave dipole
| +3.3
| +1.2
|-
| Quad loop single element
| +4.1
| +2
|-
| 2 element yagi
| +7.1
| +5
|-
| 3 element yagi
| +10.1
| +8
|-
| 4 element yagi
| +12.1
| +10
|-
| 2 element quad
| +9.1
| +7
|-
| 3 element quad
| +12.1
| +10
|-
| 4 element quad
| +14.1
| +12
|}
 
 
Adapted from Orr WL (W6SAI) and Cowan SD (W2LX), 1986, the Radio Amateur Antenna Handbook
 
===dBo Optical Gain===
 
dBO is an unofficial term used by some amateurs working with transmission of data using light. It refers to the apparent gain of an optical system compared to a point source of light.
 
 
{{electronics}}

Latest revision as of 02:17, 22 November 2010

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 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>

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 radiator = 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>

Comparative gain of various antenna types

Antenna Type dB gain over isotropic radiator dB gain over half-wave dipole
Isoptropic radiator 0 -2.1
Ground plane +0.3 -1.8
half-wave dipole +2.1 0
5/8 wave dipole +3.3 +1.2
Quad loop single element +4.1 +2
2 element yagi +7.1 +5
3 element yagi +10.1 +8
4 element yagi +12.1 +10
2 element quad +9.1 +7
3 element quad +12.1 +10
4 element quad +14.1 +12


Adapted from Orr WL (W6SAI) and Cowan SD (W2LX), 1986, the Radio Amateur Antenna Handbook

dBo Optical Gain

dBO is an unofficial term used by some amateurs working with transmission of data using light. It refers to the apparent gain of an optical system compared to a point source of light.


Electronic Theory
Physical quantities Current * Gain * Impedance * Power * Q of a circuit * Radiated Power Measurement * Reactance* Resistivity * Resonance * Voltage
Components Baluns * Bipolar-Junction Transistors * Capacitors * Diodes * Inductors* Lasers * Microphones * Resistors * Transformers * Wire
Circuits Attenuators * Digital Signal Processing (DSP) * Dummy load * Filters * LC filters * Power Supply Design * Rectifier Circuits
Design Amplifier Design * Oscillator Design
Electromagnetic Waves Relative power (Decibels) * Harmonics * Interference and BPL
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