OK - my books are out on loan (again), so I'll take the lazy way out. Google "node antinode brass" and the second hit will give:
http://www.colorado.edu/physics/phys483 ... /n1106.htm" target="_blank" target="_blank" target="_blank
where you will find (my apologies for using the trumpet as the example...):
Flared Bell
Let's talk about a trumpet as a example. If there was not a flared bell the trumpet would have odd integer overtones. The flared bell (and to a lesser extent the mouthpiece) cause the overtones to be harmonic (almost). This is due to many years of artisans tinkering with various shapes and sizes for the bell. The original first natural mode is shifted upward and is not related in a harmonic way with the other normal modes which take on a frequency of 2f, 3f, 4f, ... with the fundamental missing. The missing fundamental can be played by careful control of the lips and heavily relying on the overtones, and is called the "pedal tone".
The natural modes of flared bells in combination with cylindrical and conical cavities are discussed in "The Physics of Musical Instruments", Fletcher and Rossing (1998), if you are interested in the actual solutions to the wave equation in these more complicated geometries.
Look at the diagram there under the heading "conical bore" - and then note that the flared bell effectively LENGTHENS the tube as the frequency goes up (I think I have that right - please do check with our friends Fletcher and Rossing - or find the Benade article in Scientific American on the Physics of Brasses).
To summarize: the tuba is best viewed as being OPEN on one end and CLOSED on the other, with a node at one end and an anti-node on the other. Ordinarily, this might lead to the conclusion that you can only get odd harmonics - but the flared bell changes the effective length of the tube so that you get 2f, 3f, 4f, ... (but note the absence of 1f!!!!!) There is a "first partial" but it's not in the 2f, 3f, 4f... harmonic series. If you object that "I can *hear* the fundamental, then consider the psychological implications of hearing a tone where 2f, 3f, 4f, 5f, ... are all present (but not f). Your brain (and perhaps your ears) inserts the 'f which *must* be there' (see also: Difference Tones).
Back to the point: computing node/anti-node locations using a very simple model of oscillations of a string WILL NOT WORK. Perhaps you have noticed that TUBAS ARE NOT STRINGS.
And anyway, String Theory is out of date - the current version is Membrane Theory, and (against all odds) the drummers are the new Kings of Physics.