Story points: 3
Scope
The core mechanic that sets how easily a NAF overblows: the aspect ratio of the air jet (flue height = jet thickness) to the True-Sound-Hole gap (jet travel length) crossing the splitting edge.
Why
The "friend overblew one flute but not the other" difference is a jet-stability problem. A thin, fast jet (shallow flue) reaching the edge quickly (short TSH gap) spikes into the octave with a tiny velocity increase; more jet travel/give absorbs higher velocities.
Implementation plan
- Add
docs/acoustics/jet-aspect-ratio.md:
- Define jet length W (flue exit → splitting edge) and jet thickness (flue height); stability depends on W/thickness and the phase-lock between jet transit time and the bore's acoustic cycle.
- Short W + thin jet → low overblow-threshold velocity (twitchy). Longer W and/or thicker jet → higher threshold (forgiving).
- Laminar vs turbulent: too-short/rough flue → turbulent, weak fundamental; perfectly laminar but too thin → high Reynolds sensitivity, jumps octave on a small breath increase.
Acceptance
- Jet aspect-ratio model + overblow-threshold relationship documented.
- Laminar/turbulent stability notes included.
- Cites source.
Links
Story points: 3
Scope
The core mechanic that sets how easily a NAF overblows: the aspect ratio of the air jet (flue height = jet thickness) to the True-Sound-Hole gap (jet travel length) crossing the splitting edge.
Why
The "friend overblew one flute but not the other" difference is a jet-stability problem. A thin, fast jet (shallow flue) reaching the edge quickly (short TSH gap) spikes into the octave with a tiny velocity increase; more jet travel/give absorbs higher velocities.
Implementation plan
docs/acoustics/jet-aspect-ratio.md:Acceptance
Links
NAF Playability.md,Flute Acoustics.md(2026-07-02).