auralmirage said:
MSH, or anyone else for that matter: Can you fill me in on the basics of harmonic distortion and why it's nice for acoustic instruments?
Mmm, OK. It goes to the nature of the sound of an instrument (or voice). The timbre of an instrument--basically what makes it sound like itself and not another instrument--is defined by a few traits, such as attack/sustain/decay, which are probably familiar terms from synthesis, but also importantly its overtones.
When you play a note on an instrument, you have the fundamental pitch of the note, A above middle C=440Hz for example, but depending on the timbre of the instrument (for example, an oboe has lots, a flute few), lots of multiples of that fundamental as well (880, 1320, 1760, etc).
The musical relationship of those overtones can be described in terms of the interval to the fundamental: the first overtone is an octave, second is octave and a fifth, third is another octave. Once you get into higher order overtones, they get both higher in pitch and more dissonant in terms of their harmonic relation to the fundamental, eventually departing from the diatonic scale entirely.
So while low-order overtones are kinda like having somebody singing above you in harmony, high-order overtones are generally thought to be less desirable, maybe like buzzing bees or nails on a chalkboard or something.
Anytime you introduce nonlinearities into a signal, that is a distortion. The question is what is the nature of the distortion? One simple type of distortion occurs in a solid-state (transistor) circuit when the gain is driven past the voltage available. The result is called hard clipping, and it creates a squarewave. The squarewave can be broken down back into the fundamental sine wave, and lots of little low to high order overtones. In the case of extreme clipping, there are lots of those little high order overtone sine waves embedded in your signal that really make it sound like crap. This is why hard-clipping solid state distortion circuits for guitar amps are commonly regarded as poo. Example: '80s vintage Peavey amps
So instead, once we accept low-order harmonic distortion as a goal for signal enhancement, we seek out circuit that can generate those overtones without clipping and creating the high-order overtones. In guitar pedals, there are lots of popular options, such as germanium diodes or transistors, or my personal favorite, LEDs
And then there are tubes . . .
Now, it all that nice for acoustic instruments? It really, really, really depends on what you are trying to do.