Gain compression in an electronic amplifier circuit is a reduction in 'differential' or 'slope' gain caused by nonlinearity of the transfer characteristic of the amplifying device. This nonlinearity may be caused by heat due to power dissipation, or by overdriving the active device beyond its linear region. It is a large signal phenomenon of circuits.
A tube radio or tube amplifier will increase in volume to a point, and then as the input signal extends beyond the linear range of the device, the effective gain is reduced, altering the shape of the waveform. This is soft limiting, which is not the same as the behavior of an audio level compressor.
Tube or transistor, gain compression means the same thing and is caused by clipping, soft or hard.
Gain is a linear operation. "Gain compression" is not linear and, as such, its effect is one of distortion, due to the nonlinearity of the transfer characteristic which also, causes a loss of 'slope' or 'differential' gain. So the output is less than expected using the small signal gain of the amplifier.
"Soft" clipping or limiting means there isn't a sharp "knee point" in the transfer characteristic. A sine wave that has been softly clipped will become more like a square wave, with more rounded edges, but will still have many extra harmonics.
A transistor's operating point may move with temperature, so higher power output may lead to compression due to collector dissipation. But it's not a change in gain; it's non-linear distortion. The output level stays relatively the same as the input level goes higher. Once the non-linear portion of the transfer characteristic of any amplifier is reached, any increase in input will not be matched by a proprtional increase in output. Thus there is compression of gain. Also, at this time because the transfer function is no longer linear, harmonic distortion will result.
"Gain compression" in RF amps is similar to soft clipping. However, in narrowband systems, the effect "looks" more like gain compression simply because the harmonics are filtered out after amplification. Many data sheets for RF amplifiers list gain compression rather than distortion figures because it's easier to measure and is more important than distortion figures in non linear RF amplifiers.
In wideband and low frequency systems, the non-linear effects are readily visible, e.g. the output is clipped. To see the same thing at one GHz, an oscilloscope with a bandwidth of at least 10 GHz is needed. Observing with a spectrum analyzer, the fundamental compressed and the harmonics picking up.
A low-noise RF amplifier if fed by a directional antenna to a consumer 900 MHz receiver should improve the transmission range. It works, but the receiver may also pick up a couple of UHF stations around 700 MHz. For example, if channel 54 is transmitting 6 MW of AM, FM, and PM, the RF front end, expecting −80 dBm, would be grossly overloaded and generate mixing products. This is a typical effect of gain compression.
A form of gain compression also takes place in loudspeaker voice coils when they heat up and increase their resistance. This causes less power to be drawn from the amplifier and a reduction in SPL.
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