I ran across this thread (which is still in its infancy), and thought that people like Chung might be interested. I would have to read this very carefully in order to grasp any of it, but others here might find it easier reading. http://www.audioasylum.com/forums/se...ges/20121.html

OK, in slightly more layman's terms, based on what I've understood of what's going on so far: Someone came up with something called an "ideal distortion spectrum". This spectrum has the property of the 3rd harmonic cancelling out the 2nd, the 5th cancelling out the 4th, and so on. By 'cancelling', I believe this talks about a psychoacoustic cancellation, so that even though the final waveform looks pretty distorted on a scope, the human ear isn't able to hear any difference between the distorted waveform and the original pure sinewave tone. Apparently, this was tested at up to 8% distortion at about 400 Hz (I think), which I'm sure most people would agree should be audible. To put it differently, it appears that it's possible to set up a distortion spectrum that to the human ear sounds like the original pure tone. It also appears that SET amps have a spectrum that is very similar to this "ideal distortion spectrum". So, there might be a scientific reason to what subjectivists have said for a long time, that SETs sound more like the "real thing". So, on the face of things SET amps have higher distortion numbers, but what's possibly more important here is the distribution of that distortion across the different harmonics, not just the total number. Anyway, the bottomline is, the blanket statement that "tubes have more distortion and SETs have the most among the different tube amp types" is probably too simplistic. This is quite likely another case of not knowing exactly what to measure, driven mostly by our insufficient knowledge of psychoacoustics. I know there are people who believe that we know pretty much all the important things about how human hearing works, but it's possible that some subtle details are still missing. It may turn out that it's the distribution of the distortion across the different harmonics (in other words, the spectrum) that's more important than just the average distortion percentage. As these studies have shown, a band-limited square wave actually came out 'cleaner' after being passed through this distortion spectrum when compared to the original. And that's about the limit of my understanding of that discussion

Saurav: You might want to start with this: http://www.lammindustries.com/intervie/audiorus.html Larry

Suarav: I looked at that thread you posted, and I don't know what the man was talking about Assuming that your understanding of what he wrote is correct. Help me answer a couple of questions: 1. The harmonics of a sinewave increases at different rates, depending on the order of the harmonic, as a function of the amplitude of the sinewave. To illustrate: you double the input level, the second harmonic component goes up 4 times, and the 3rd goes up 8 time, the 4th 16 times, and so on. The ratio of the harmonic terms changes dramatically as the input level changes. How can this "cancellation" or "masking" work over any reasonable range of input signal? Remember music has a large dynamic range; it is not a constant level square wave. 2. You can think of music as composed of a lot of sinuosids with time-varying amplitude and frequencies. When you have multiple sinusoids at the input of the amp, you will have harmonic distortion, as well as intermodulation distortion. The intermodulation products are not harmonically related to the original signal. How can this "cancellation" or "masking" work to suppress the perception of intermodulation products? There are a lot more questions that one can raise about this theory, but it really does not sound that interesting a theory to me at all. Besides, do you want an amplifier that can create an output that sounds "better" than the original?

BTW, here's the other thread, and I had some of it wrong http://www.audioasylum.com/scripts/t...tubediy&m=9690 To quote:

Suarav: This is taking too much time, but here is what I meant: The amplifier, whether a SET or a solid state, is described by a transfer function. In other words, output voltage is a function of the input voltage. Most amplifiers are quasi-linear, and the output can be expressed as a polynomial function of the input voltage. This model does not fit amplifiers that have cross-over distortion, or other strongly frequency-dependent distortion, but those are exceptions rather than the norm. So we can express Vout=a1*Vin + a2*Vin**2 + a3*Vin**3 + higher order terms. By the way, a2, a4 and so on contribute to the even harmonics, and a3, a5, etc. the odd harmonics. If you put Vin= Asinwt, and do the expansion, you will find terms of sin2wt, sin3wt, and so on in Vout. These are the harmonic distortion terms. You will find that if the input level (Asinwt) doubles, the 2nd harmonic term will increase by a factor of 4 (due to a2Vin**2) and so on. So the harmonic distortion terms are strong functions of the input level. You can also set Vin=Asinw1t+Bsinw2t to find the intermodulation terms, and convince yourself that those are not harmonically related to the input. If only a "golden" set of harmonic distortion terms sound "good", I don't see any way a SET amplifier or any amplifier being able to maintain the ratios of those harmonic terms, over the usual dynamic range of the input.

Suarav: I apologize if I sounded rude. I'm in a hurry to a presentation. The power series expansion is a pretty fundamental concept in understanding distortion, and I would be happy to clarify things later.

No problems. Let me think about what you said, I don't remember my Taylor's (or whatever) expansions any more I do think that the constant multipliers would be such that the higher power terms would be smaller in magnitude than the fundamental. However, you're talking about maintaining linearity across a range of input values (I think), which is a different thing from driving the amp too hard and into a non-linear region. Also, I don't know why an amp's transfer function would expand in terms of powers of the input, instead of frequency multiples. For instance, trivially, the power series expansion doesn't hold at DC. In any case, I'm sure this wouldn't hold across a wide dynamic range. And that's normal for any amplifier, THD goes up as signal level goes up. Nevertheless, even if the device could stay within a reasonable tolerance level of this distortion over a reasonable dynamic input range, that's still interesting, to me. To use your term, if a specific "golden" distortion sounds 'perfect', then something close to that would sound 'almost perfect', with the sound getting subjectively worse as one deviates further from that 'golden' (set of) number(s). So, it's not an all-or-nothing situation.

sin^2(x)=1/2*(1-cos2x) sin^3(x)=1/4*(3sinx-sin3x) So the 2nd order term gives rise to sinusiods at twice the input frequency, hence 2nd harmonic distortion. The 3rd order term leads to sinusiods at 3 times the input frequency, or 3rd harmonic distortion. In general, if the input is A sinx + B siny, there will be terms at frequencies mx+ny, where m and n are positive and negative integers. It's hard to design an amplifier that generates -22dB 2nd harmonic distortion over a range of input levels. Again, intermodulation will hurt you in a very bad way, since the products are not harmonically related to the inputs.