In article , Peter Scott
wrote:
"Jim Lesurf" wrote in message
...
[snip]
But I come back the point about the hf. Surely if the clipping is
caused by effects in the output transistors, that drive them into
non-linearity, it is in effect after the amp stages?
If you are observing components at the amplifier's output terminals when
driving a normal passive linear load then the signals you see are all
getting their non-zero power from the amplifier to that point. Consider in
this context two questions:
1) How can any part of the amplifier be "after" the amplifier? (This sounds
like we are heading towards a Zen Koan if we aren't careful. ;- )
2) The load is not generating the power observed, so if it isn't being
provided by the amp, what would be meant by saying it comes from "after the
amp stages"?
Otherwise how could components be generated that lie outside the range
of the amp.
This depends what definition you are using for the "range of the amp".
When operating as a unit, the overall amplifier circuit will have a given
frequency response into the load. However individual gain devices in the
amp may well have gain 1 over a wider range. Also, when you push devices
into nonlinear behaviour by clipping/saturating/switching them, this may
create changes in level which occur in shorter timescales (and hence at
higher frequencies) than the range over which the amp has a gain 1 in
normal, unclipped use. Is this what you have in mind?
However in my experience most SS amps have devices with gain up to
frequencies well above 20kHz (typically to MHz region or higher). Hence I
doubt this is a problem as such for audio. The audible problems will tend
to be at much lower frequencies.
Or is it that fourier doesn't come into it.
Fourier Tranformation and Fourier Theory simply provides a method for
looking at the same information in terms of either the time waveform (time
domain) or frequency spectrum (frequency domain). You can use this as you
prefer, provided the tranformation is performed correctly over an
appropriate waveform interval, etc. So it can come into it or not depending
on what you are trying to explain/understand, etc.
The fact that you need this range of frequencies to synthesise the wave
doesn't mean that the amp has to produce them.
If they appear in the clipped waveform, then they have power. Thus they
will have come from somewhere. If they are at the ouput terminals of the
amp, and the load is essentially passive and linear, the question becomes,
where else are they coming from?
The 'sharpness' of the clipping will depend on the behaviour of the
amp/devices. Hence you can't assume perfectly sharp clipping (which would
potentially produce components up to an arbitrarily high frequency).
All that is needed is a slew rate that is at least equal to the steepest
slope on the wave.
The slew rate isn't really the issue, I think. It is the sharpness of the
'corners' produced as the signal enters/leaves clipping. i.e. the
derivatives of the shape if considering the time domain waveform.
'Perfect' or idealised clipping would involve a discontinuous change in the
slope of the waveform at the instants when clipping starts/ends. Such
discontinuities would imply an infinite bandwidth for the output. In
reality, this doesn't happen, though. All real devices have finite
bandwidths and finite response times.
Slainte,
Jim
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