QUOTE(briantrumpet @ May 11 2008, 09:44 AM)

QUOTE(joolsters @ May 11 2008, 09:23 AM)

The fundamental of the harmonic series. You know how on the Euphonium you get different partials depending on the tension on your lips and how it goes from something like
C --> G --> C --> E --> G --> (very flat) Bb --> C --> D --> E --> (very flat) F# etc.
The first "C" would be the 1st harmonic, and it is actually possible to another partial below that, the fundamental / pedal tone / whatever people call it.
This is a nice clear description ... but, apologies for being pedantic, the pedal C is actually the 1st harmonic, because the ratio between the pedal C (1st harmonic) and the next one (the 2nd harmonic - the first one in your list) is 1:2. So the list of notes with their harmonic numbers is:
C(1) - C(2) - G(3) - C(4) - E(5) - G(6) - Bb(7) - C(8) etc.[...]
There are competing nomenclatures in this area. For a physicist, harmonics are components of repeating waveforms, and are indeed in the ratios of the natural numbers. They are determined by Fourier analysis, which is not particularly complicated but does need the integral calculus, so I shan't describe it. IIRC, a physicist would describe the various notes available on a brass instrument as the eigenvectors of an eigensystem; I prefer to call them overtones, though I suppose that few others do. A major objection to calling them "harmonics" is that the frequencies of the resonances are only approximately in the ratio of the natural numbers. If you put a mouthpiece on a parallel tube and blow it like a brass instrument, you will find resonances roughly in the ratios of the odd numbers 1:3:5:...[1] Brass instrument designers are obliged to have parallel tubing in the middle of their instruments, so as to be able to add extra length with valves, but then make the instrument approximate to the behaviour of the ideal conical shape, which gives frequency ratios 1:2:3:..., by adding a tapered mouthpipe and a rapidly expanding bell. This works amazingly well, but not perfectly, because the tapered portions combine with only one length of parallel tubing to give resonant frequencies in harmonic ratios.[2]
This is demonstrable on four valve instruments, such as double horns and tubas. Typically, on these, the longest configuration is nearly twice the length of the shortest. If you play the two series with these fingerings, aiming each note in the middle of the resonance, not attempting to lip it towards "correct" tuning, and measure the frequencies, you will find that at least one of them is not harmonic: either the short instrument has a compressed series or the long one an expanded one, or both. I tune my double horns so that the two sides (F and Bb) are in tune in the upper register, and can hear very clearly that the bottom notes of the shortest configuration are naturally sharp. They are easy to lower with lip and hand, of course.
Cornett resonances also depart from harmonic frequencies. Despite having a conical bore, my mute cornett has an expanded series of resonances, in this case, I suspect, because the ratio of throat area to bell area is small (about 32, compared with 3600 for my horn), so that the acoustic properties vary towards those of a parallel tube. The first octave and the twelfth are both usable with fingerings in which most of the holes are covered, because the pitches remain controllable by lip, but the double octave puts the note into a register where the resonance is very sharp, and no small adjustments are possible.
[1] The clarinet, with its near parallel bore and its reed similarly stopping one end, overblows at the twelfth, because that is the frequency of the second resonance.
[2] ISTR that Benade claims (either in his book, "Fundamentals of Musical Acoustics" or his article "Physics of Brasses" in Scientific American) that there is no resonant frequency at that of the pedal note. What happens here is that the second, third and fourth harmonics of the lip or reed motion (this is a repeated wave form, so it
does have harmonic components) lock into the higher resonances of the tube. The lowest resonances tend to be about a third lower than the harmonic frequency, so the pitch of these notes can be lowered easily with the lip.