In article , Ian Iveson
wrote:
Jim Lesurf wrote:
However the passage of time has changed both of those factors!
Although I do still wonder about some modern 'high end' designs. What
peak current and slew rates can they provide, and is it adequate for
real use with music into speakers? In particular I wonder about some
valve designs. At what current do they limit, and what happens when
they do?... Alas, if no one measures this you can't tell, or often
even guess with any reliability.
It could be that a square wave test isn't the best way of identifying
the kinds of limiting that you mention, and never was.
Well, the 1955 article that Mike just sent me a copy of does show that it
might well have been common! However since people now often don't check
I have no idea how revealing it might turn out to be nowdays. It is
easy enough to deal with this by good design. But I am less than sure
that *all* modern designs *are* 'good' in respects like this TBH.
When valve amps were the norm, true "slew rate limiting" was unheard
of, AFAIK. Not enough gain or feedback.
I appreciate that it was largely "unheard of" in the sense that many people
hadn't heard of it or knew what it was. :-)
However you don't need either high gain or overall feedback for slew
limiting to occur. So if a design isn't made in a way that ensures
it doesn't happen then the absence of feeback or high gain isn't a
guarantee. So far as I know, if the gain stages are not
preceeded by a passive LPF and you can connect arbitrary loads to the
output the slew limiting may be possible, regardless of having no feedback
back or low voltage gain.
One effect that I have seen referred to as slew rate limiting can
happen when a cathode follower with inadequate bias current fails to
keep up with the demands of a capacitive load. Like real slew rate
limiting,
Erm.. what you describe above does seems like slew rate limiting to me,
so I don't know why you say it is "like" slew rate limiting. In what
was is it *not* slew rate limiting?
it is an effect of feedback,
Again, your reason for saying that isn't clear. cf below.
and results when the triode
approaches turn-off only when the signal is both high amplitude and
high frequency...which is when the slew rate is highest.
Your approach above seems different to mine. Mine is that the stage has a
limited output current ability. So if you attach a large enough capacitance
and try to slew the voltage fast enough you get current limiting determined
slew rate limiting of the output voltage. Not sure why feedback would be
regarded as the cause of that. Perhaps you can explain if I have not
understood your point.
So far as I know the above can arise even with a single gain stage with
no feeback. The only requirement is a load capacitance that is non
zero, a current limiting mechanism in the circuit, and an input that
has too high a rate of change for the stage to then handle without
the problem arising.
The current limiting mechanism can arise in various ways. Obvious
examples being the saturation/max current the gain device can pass.
You then get essentially a current source attached to a capacitance.
However, for small amplitudes, the same CF wouldn't suffer from the same
problem even if the input slew rate were the same.
I'm not clear why you think that, I'm afraid.
I appreciate that real 'squarewaves' tend to have finite bandwidth
and so using a given generator you tend to find that the maximum slew
rate of the generator output scales with the waveform amplitude.
But if the mechanism of the problem in the stage is that it has finite
current capacity, and is connected to a load capacitance, then that
mechanism will be the same. Is your argument that with small signals
the current required for the load resistance is smaller, so more is
available for the capacitance? If so, yes, I'd agree that makes
sense.
Either way, I agree you'd need to check for this with suitably large
waveform amplitudes as smaller test signals may well not provoke
a problem which larger signals would show.
A square wave test
could miss the problem unless it was full amplitude, and then it might
be strewn with other debris. A positive pulse wouldn't show it either,
although a negative-going one would.
I'd assume the voltage amplitude required would vary with the load
capacitance and the current limit value for the part of the system which
was involved.
In practice, other tests would be used to identify most problems. The
most common use of a square wave was to check for a well-damped
transient response. For that the square wave must rise significantly
faster than the frequency of the dominant pole, and hold steady enough
so the consequent ringing can be observed. For a power amp, that
frequency was likely to be of the order of 50kHz. This test makes a
nice picture that anyone can understand directly...a steep rise,
overshoot, three declining wriggles, then flat. Lots of things do that
when you hit them, everyone sees it every day.
Yes. I think that was why later on some reviewers checking SS amps with an
output inductor assumed the ringing with a capacitative load was something
other than the passive LC resonance of the output inductor with the load
capacitance... and then though it was something to do with the stability
margin of the amp.
Stability was pretty much the big issue then, hence the need for that
particular test, but is it still? What other problems were square waves
used to illustrate then, that they could also be best used for now?
Once again, it could be that the issues of concern have changed such
that other tests are more appropriate.
For well designed amps I'd agree. However many of the 'high end' designs
these days tend to be valve types with output transformers and valve stages
that could current limit in quite complex ways. As per the results in the
1955 article I do wonder what some of the 'new' designs would do if square
wave tested into loads other that a kindly matched resistor load. :-)
If you wish to re-introduce some stringent analytical testing to
magazine reviews, then you need to pick the most directly illustrative
test for each effect you wish to portray. Re-introducing the square
wave, willy nilly, might not prove popular or particularly instructive.
Matter of horses for courses, yes. However the problem here is that in some
cases you don't know what a test will show until you do it and see.
What I would most like to see, now as then, is a clear set of graphs
showing distortion across the claimed frequency range at small, medium
and full power levels, into several representative loads (how many 3D
plots would it take to cover those 4 dimensions?), and a Bode diagram.
Some confirmation that EMC and safety standards have really been met
would be reassuring.
I'd also like measurements to determine the in-loop output impedance and
stability behaviour.
It's easy for amps to look good when they're well within their comfort
zones, so they do need to be stretched to the limits of their
performance and operating conditions, so I'm with you on that point.
These days, it should be possible to traverse those limits
systematically, rather than sample them conveniently as they seem to do.
A number of people have proposed various tests. However as with squarewaves
I always tend to end up feeling you need a variety of these on tap so you
can check for the unexpected! :-)
I presume many amps would be fine. But the importance of the tests would be
to know which ones do 'pass ok' and which get caught out in ways that might
crop up with real music into real speakers.
Slainte,
Jim
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