Global Feedback - A huge benefit for audio

You can't blame AR; serious science and understanding of the scientific method is only a couple of centuries old.

Well, the early development of the hypothetico-deductive-probabilistico-approximative Formal Axiomatic Method and its pillar, the Symbolic Logic was initiated back in the seventeenth century by some mathematicians imbued with the lofty romantic-idealistic-deterministic vision of establishing an analogy between numbers and Nature through many-layered abstractions. It`s a pretty much all-round method, its application is limited only by our imagination.
 
There is no such thing as infinite feedback or zero output impedance in practical feedback amplifiers. The figures are easily measurable and easily calculatable.
Practical feedback amplifiers can have a positive or a negative output impedance. But not zero ?

If someone is making these claims, clearly they do not understand feedback.
An argument to explain why an amplifier could have not have zero impedance (it does not need to have infinite negative feedback for that) would be more interesting than your favorite leitmotiv.
 
The definition of feedback is: a part of the output from a system reaching the input and adding to or subtracting from it. This is elementary control theory.
A degenerating resistor connected to the emitter has the output current component flowing into it and creating a voltage difference which subtracts from the signal voltage which is usually applied between ground and base. This is negative feedback.
This is an excellent univocal definition which, slightly modified, could be extended to differential inputs.
 
This thread is attracting flies like you know what.
 

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A typical GNFB amp will have 60-80dB. The Zero GNFB is by definition 0dB.
Would the optimum set equal to both, and design a very linear amp then add say 30-40dB. Would that be a middle ground for all the protagonists here?

It depend what goal of the amplifier specification.
If the goal is best linearity, then choose high loop gain at 20 Hz to 20 kHz.
If the goal is sound pleasing, you must define what make sound pleasing or not pleasing. Many people have their own idea about pleasing sound.

The problem is many people do not understand the correlation between sound pleasing with measurement.

The other problem is people who do not understand engineering talk about engineering, blame the measurement and blame the technique.
 
Sound has a "highest purpose" arithmetically determined, just like human does have. Therefore it can have characteristics that are positive on a scale of purposefulness. In these modern days music is not always about harmony. Nothing wrong about it. The normalization process may be applied to difference between individuals. To create amplifier that does the job - "amplifying" - not only a single recipe should suit. There could be different approaches. Instead of global feedback, one could perhaps use certain patterns of numbers and create local "spins" around amplifying devices, by defining desired order of pattern. Negative multiplied with negative is positive number. Not fully true, if the process is within boundaries of negative amounts always being in return. "But supply voltage is free from negative form..unless it is off". Sure, go that way. And record is free from soul too.
 
This is on a humorous note.

About 30 years ago, someone described feedback as:
When you deficate and eat it or part of it.

This person now is almost retired and possesses a Higher Technician Diploma. I still remember the transformer phasor diagram on his study table.
 
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Originally Posted by jan.didden
This can be and has been technically demonstrated as fact. See the various writings of Self, Cordell, and earlier Baxandall.


I guess you mean the conversion of second-order distortion to higher-order distortion by negative feedback; the total distortion goes down, but the harmonic content also changes. That was already shown in L. I. Farren's 1938 paper, https://linearaudio.nl/sites/linearaudio.net/files/Farren feedback1938.pdf , and he referred to an even older article by Richard Feldtkeller in Telegraphen- und Fernsprechtechnik, vol. 25, page 217.

First I'd like to say that the paper you linked is great, and it's surprising to me that this was published in 1938. Global feedback in audio power amplifiers wasn't seen much until the 1950s. and did not become de riguer until the late 1960s. The fact of the matter is that it's difficult to apply global feedback to a transformer coupled amplifier, although the Williamson and Ultralinear topologies became somewhat popular (tubes were losing their popularity and were considered old fashioned) and showed that it could be done.

Second, I'd like to point out that you're both right. Global feedback does change the harmonic profile and it does skew it towards higher order harmonics. But the design theory (which I realize isn't always achieved) is that if there's enough loop gain in the passband, and the higher order harmonics are below the threshold of audibility (even mediocre modern amplifiers achieve -80 dB which is pretty good), then the distortion is negligible. I've seen specs that claimed the higher order harmonics were -110 to -120 dB which is almost certainly negligible.

Do amplifiers achieve their published specifications? There's a lot of reasons why they might not while in service, but that's another rabbit hole.
 
Derivation of the foundation formula for Negative Feedback, the economical magic, which makes cheap amplifiers behave like prohibitively expensive ones.

Suppose an amplifier has a transfer function:
V = G.i

Where V = output voltage, G is a constant and i is the input voltage.

We will apply feedback to the amplifier to change its transfer function into a line with a lower gradient.

Let us say the amount of feedback is f where f < 1 but not negative.

Applying the transfer function, we get:
V = G.(i - fV)
=> V = Gi - GfV
=> V(1 + Gf) = Gi

Rewriting:
Gi = V(1 + Gf)

The new gain is:
V/i = G/(1 + Gf)

If G is very large, 1 + Gf >> 1, implying we can eliminate 1.

Therefore:
V/i = 1/f

This result concludes that when G is large but not necessarily stable and constant, a better behaving amplifier can be made by applying a feedback fraction of f.