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Pipe Organ Frequency Calculator

Convert between organ pipe physical length and pitch for both open and stopped pipes. Includes end-correction physics, harmonic content, nearest-note identification, and a rank context table (32′ / 16′ / 8′ / 4′ / 2′ / 1′).

Input

Pipe type
cm
mm
°C
Common ranks

Result

Result
Fundamental f₁
Nearest note
Physical length
Effective length L_eff
Sound speed c
First 6 harmonics
Formulas
Open pipe (both ends open): f_n = n · c / (2 · L_eff), L_eff = L + 1.2·r, all harmonics
Stopped pipe (one closed): f_n = (2n−1) · c / (4 · L_eff), L_eff = L + 0.6·r, odd harmonics only
Sound speed: c ≈ 331.4 + 0.6·T(°C) m/s

Rank context (same diameter, transposed by foot pitch)

RankRequired lengthResulting pitch

"Foot pitch" is the conventional organ-builder label. An 8′ rank's low C plays at unison pitch (C2 ≈ 65.4 Hz); a 16′ rank's low C plays one octave lower, a 4′ rank one octave higher, etc.

About Organ Pipe Acoustics

Organ pipes are tuned acoustic resonators — the same physics as flutes and clarinets, scaled up by 100×. Two main families dominate: open flue pipes (open at both ends, like the Diapason / Principal) and stopped flue pipes (one closed end, like the Bourdon / Gedackt). Reed pipes use a separate physics (a vibrating tongue drives the air column) and aren't covered by this tool.

Open pipes

Both ends are pressure nodes — the standing wave fits an integer number of half-wavelengths between the ends. Fundamental: f₁ = c / (2·L_eff). All integer harmonics are present (1f, 2f, 3f, …), giving the classic bright "open flute" timbre.

Stopped pipes

One open end (pressure node), one closed end (pressure antinode). The standing wave fits an odd number of quarter-wavelengths between them. Fundamental: f₁ = c / (4·L_eff) — exactly an octave below the equivalent open pipe of the same length. Only ODD harmonics exist (1f, 3f, 5f, …), giving the characteristic hollow, "stopped flute" timbre. This is why a 16′ stopped rank takes only 8 feet of pipe — a major space savings for the bass register.

End correction

Air doesn't stop exactly at an open end — it "bulges" outward slightly. The effective acoustic length is longer than the physical length by ~0.6·r per open end (Levine-Schwinger, unflanged). An 8′ open pipe at 2.44 m with 100 mm diameter has L_eff = 2.44 + 1.2·0.05 = 2.50 m, lowering the predicted pitch by about 4%. Without end correction, a 2.44 m open pipe predicts 70.3 Hz; with correction, 68.6 Hz — close to but not exactly C2 (65.4 Hz). Real organ pipes are tuned by sliding tuning sleeves or cutting slots; the calculator's prediction is a starting point.

Rank conventions (foot pitch)

Organ builders label ranks by the physical length of the C below middle C. An 8′ rank has its low C at approximately 8 feet (its C2 plays at the keyboard's C2 pitch — "unison"). Other rank conventions:

  • 32′: two octaves below 8′ (lowest pedal stops, only in large organs)
  • 16′: one octave below 8′ (typical pedal voice)
  • 8′: unison (most ranks)
  • 4′: one octave above 8′
  • 2′: two octaves above 8′
  • 1′: three octaves above 8′
  • 5⅓′, 2⅔′, 1⅗′: mutation stops at non-octave intervals (a fifth, twelfth, seventeenth)

Frequently Asked Questions

Why is a stopped 16′ rank only 8 feet long?
Because a stopped pipe's fundamental is at c / (4·L_eff) instead of c / (2·L_eff) — exactly half the frequency of an open pipe of the same length. So a stopped pipe sounds one octave lower than the open pipe twice its size. An 8-foot stopped pipe plays the same low C as a 16-foot open pipe. The trade-off: stopped ranks only produce odd harmonics, giving a hollower timbre. Space-saving for cathedral organs that need huge 32′ pedal stops.
Why does temperature affect tuning so dramatically?
Pipe pitch is proportional to sound speed, which scales as √T (Kelvin). A church warms from 15 °C in winter to 25 °C in summer: c goes from 340 to 346 m/s, a 1.8% change = 31 cents (~⅓ semitone). The organ goes flat as it cools. Modern installations include heating control to stabilize this; period organs were tuned to play at concert temperature.
Does pipe diameter affect pitch?
Yes, through end correction (~1.2·r for open pipes). A wider pipe has more end correction, lowering the pitch. A 2.44 m pipe at 100 mm diameter plays about 68 Hz; the same length at 50 mm diameter plays about 69.3 Hz. For precision tuning, builders adjust both length and diameter. Diameter also strongly affects timbre and dynamic range — narrow pipes are quieter and stringy (Salicional), wide pipes are louder and flutey (Open Diapason).
What's the difference between Töpfer scaling and arbitrary diameter?
Töpfer's normal scale defines pipe diameter as a function of pitch: roughly, halving the frequency increases diameter by ~√2 (so each octave down, diameter grows by 41%, not doubles). This produces consistent timbre and dynamic balance across the rank. This tool lets you set any diameter independently — useful for academic exploration, but real ranks follow some scaling progression.
Why are mutation stops at non-octave intervals (5⅓′, 2⅔′, 1⅗′)?
Mutation stops add specific harmonics to enrich the tone of unison stops. A 2⅔′ rank plays a fifth above the unison (note: not the octave's fifth — the third harmonic of the 8′ rank). When played with an 8′ Principal, the 2⅔′ Twelfth adds the 3rd harmonic, brightening the sound. A 1⅗′ Tierce adds the 5th harmonic. Combining several mutation stops with the unison (the "plenum") synthesizes complex timbres reminiscent of brass or strings.
Do real organs use this exact formula?
As a starting point, yes — but final tuning is empirical. Organ builders cut pipes slightly long, then tune by adjusting a sleeve at the top (open pipes) or a stopper at the closed end (stopped pipes). Voicing (mouth shape, languid alignment, wind pressure) introduces small pitch shifts of ±20 cents that the formula doesn't predict. The formula gives the 95-99% correct length; the last percent is done by ear in the loft.