Chapter 01 / Acoustics

Acoustics聲學

A brass note is an arithmetic series pretending to be a single sound. Set the eight partials below, press play, and watch the waveform admit what it really is: one fundamental plus its whole integer family, summed in real time.

Macro detail of a brass instrument bell, flared rim filling the frame
PLATE 01 — BELL, MACRO

Partial mixer — 8 sliders

1.00
0.55
0.32
0.18
0.10
0.06
0.04
0.03
233 Hz
Audio starts only after you press play. The picture is computed, not measured, so it stays honest either way.
B♭3 ≈ 233 Hz A4 = 440 Hz 8 partials Sine + gain

Why integer multiples? Because a standing wave only survives if it closes on itself. The air column in a brass instrument is forced to fit a whole number of half-wavelengths between the lip reed and the bell, so the allowed modes are f, 2f, 3f and onward. Nothing in the physics permits 2.7f. The harmonic series is not a choice the instrument makes; it is the residue left after everything impossible has cancelled itself out.

Why does a flugelhorn sound different from a trumpet at the same pitch? The bore. A trumpet is mostly cylindrical and keeps shoving energy into the upper partials; a flugelhorn is conical for most of its length, flares earlier, and rolls its spectrum off faster. The second and third harmonics dominate, the eighth is barely present. That is the whole recipe for the mellow tone — the sliders above, tilted hard to the left.

What does the rider at the back of a hall actually hear? Mostly the low partials, because the upper ones beam forward out of the bell and air absorption eats them first. Off axis, the note arrives darker than it left the instrument: fewer harmonics, slower attack, more of the room in the balance. A flugelhorn is less affected because it started dark. Distance changes the mix, never the arithmetic.