Sound Attic

Room acoustics & home studio calculators

Metres · feet · °C · °F

Room mode calculator

Type your room’s length, width and height to see where it booms and where bass goes missing: every room mode up to 300 Hz, charted and checked.

Your room

Units

in

Default 0.4 s is a round starting value, not a measurement. Put in your own from the reverb time calculator or a measurement.

Show in the list

Your room’s modes

Lowest mode
40.9 HzE1 −14¢ · axial, length
Schroeder frequency
≈ 216 Hzfrom a reverb time of 0.4 s
Modes to 300 Hz
13916 axial · 62 tangential · 61 oblique
Bonello check
Passesboth conditions met

4.2 × 3.4 × 2.4 m (13.78 × 11.15 × 7.87 ft) · 34.3 m³ (1,210 ft³) · sound at 343.3 m/s (1,126 ft/s), 20 °C (68 °F)

Modes on a frequency axis

401501631804100512561601920030fsgap20305070100150200300Hz

Widest gap below the Schroeder frequency: 50.5–65.0 Hz (14.5 Hz with no mode). Bands are third octaves; the number in each is its mode count up to the 200 Hz band. “Coincident” means the same frequency to 0.05 Hz.

Bonello check (third-octave bands to 200 Hz)

  • Counts never fall Passes No band holds fewer modes than the band below it.
  • No coincident modes Passes No two modes share a frequency.
Modes per third-octave band
Band, HzRange, HzModes
4035.5–44.71
5044.7–56.21
6356.2–70.81
8070.8–89.14
10089.1–112.25
125112.2–141.36
160141.3–177.819
200177.8–223.930

Room proportions

Your room, height : width : length = 1 : 1.42 : 1.75

Within the ITU-R BS.1116-3 proportions for a reference listening room: 1.1·w/h ≤ l/h ≤ 4.5·w/h − 4 gives 1.56 ≤ 1.75 ≤ 2.38, with l/h = 1.75 and w/h = 1.42 both under 3.

Published proportions, height : width : length (guidance only)
NameProportionsSource
Sepmeyer A1 : 1.14 : 1.39Sepmeyer 1965
Sepmeyer B1 : 1.28 : 1.54Sepmeyer 1965
Sepmeyer C1 : 1.60 : 2.33Sepmeyer 1965
Louden1 : 1.40 : 1.90Louden 1971

Every mode

139 modes up to 300 Hz
HzTypeL W HNearest note
40.9Axial1 0 0E1 −14¢
50.5Axial0 1 0G#1 −48¢
65.0Tangential1 1 0C2 −12¢
71.5Axial0 0 1D2 −45¢
81.7Axial2 0 0E2 −14¢close pair
82.4Tangential1 0 1E2 −1¢close pair
87.5Tangential0 1 1F2 +5¢
96.1Tangential2 1 0G2 −34¢close pair
96.6Oblique1 1 1G2 −25¢close pair
101.0Axial0 2 0G#2 −48¢
108.6Tangential2 0 1A2 −22¢close pair
108.9Tangential1 2 0A2 −17¢close pair
119.8Oblique2 1 1A#2 +47¢
122.6Axial3 0 0B2 −12¢
123.7Tangential0 2 1B2 +4¢
129.9Tangential2 2 0C3 −12¢close pair
130.3Oblique1 2 1C3 −7¢close pair
132.6Tangential3 1 0C3 +23¢
141.9Tangential3 0 1C#3 +41¢
143.0Axial0 0 2D3 −45¢
148.3Oblique2 2 1D3 +17¢close pair
148.8Tangential1 0 2D3 +23¢close pair
150.7Oblique3 1 1D3 +45¢close pair
151.5Axial0 3 0D#3 −46¢close pair
151.7Tangential0 1 2D#3 −44¢close pair
156.9Tangential1 3 0D#3 +15¢close pair
157.1Oblique1 1 2D#3 +17¢close pair
158.8Tangential3 2 0D#3 +36¢
163.5Axial4 0 0E3 −14¢
164.8Tangential2 0 2E3 −1¢
167.5Tangential0 3 1E3 +28¢
171.1Tangential4 1 0F3 −35¢
172.1Tangential2 3 0F3 −25¢close pair
172.3Oblique2 1 2F3 −23¢close pair
172.4Oblique1 3 1F3 −22¢close pair
174.2Oblique3 2 1F3 −4¢close pair
175.1Tangential0 2 2F3 +5¢close pair
178.4Tangential4 0 1F3 +38¢
179.8Oblique1 2 2F#3 −49¢
185.4Oblique4 1 1F#3 +4¢close pair
186.4Oblique2 3 1F#3 +13¢close pair
188.4Tangential3 0 2F#3 +32¢
192.2Tangential4 2 0G3 −34¢
193.2Oblique2 2 2G3 −25¢
194.9Tangential3 3 0G3 −10¢close pair
195.1Oblique3 1 2G3 −8¢close pair
201.9Axial0 4 0G#3 −48¢
204.4Axial5 0 0G#3 −28¢close pair
205.0Oblique4 2 1G#3 −22¢close pair
206.0Tangential1 4 0G#3 −13¢
207.6Oblique3 3 1G#3 −1¢close pair
208.3Tangential0 3 2G#3 +6¢close pair
210.5Tangential5 1 0G#3 +24¢
212.3Oblique1 3 2G#3 +38¢
213.8Oblique3 2 2A3 −50¢close pair
214.2Tangential0 4 1A3 −46¢close pair
214.6Axial0 0 3A3 −43¢close pair
216.5Tangential5 0 1A3 −28¢close pairabove fs
217.2Tangential4 0 2A3 −22¢close pairabove fs
217.9Tangential2 4 0A3 −17¢close pairabove fs
218.1Oblique1 4 1A3 −15¢close pairabove fs
218.4Tangential1 0 3A3 −12¢close pairabove fs
220.4Tangential0 1 3A3 +3¢above fs
222.3Oblique5 1 1A3 +18¢close pairabove fs
222.9Tangential4 3 0A3 +22¢close pairabove fs
223.0Oblique4 1 2A3 +24¢close pairabove fs
223.8Oblique2 3 2A3 +30¢close pairabove fs
224.2Oblique1 1 3A3 +33¢close pairabove fs
227.9Tangential5 2 0A#3 −39¢above fs
229.3Oblique2 4 1A#3 −28¢close pairabove fs
229.6Tangential2 0 3A#3 −26¢close pairabove fs
234.1Oblique4 3 1A#3 +7¢above fs
235.1Oblique2 1 3A#3 +15¢above fs
236.3Tangential3 4 0A#3 +23¢close pairabove fs
237.1Tangential0 2 3A#3 +30¢close pairabove fs
238.9Oblique5 2 1A#3 +43¢close pairabove fs
239.6Oblique4 2 2A#3 +47¢close pairabove fs
240.6Oblique1 2 3B3 −45¢above fs
241.7Oblique3 3 2B3 −37¢above fs
245.2Axial6 0 0B3 −12¢above fs
246.8Oblique3 4 1B3 −1¢close pairabove fs
247.1Tangential3 0 3B3 +1¢close pairabove fs
247.5Tangential0 4 2B3 +4¢close pairabove fs
249.4Tangential5 0 2B3 +17¢close pairabove fs
250.4Tangential6 1 0B3 +24¢close pairabove fs
250.8Oblique1 4 2B3 +27¢coincidentabove fs
250.8Oblique2 2 3B3 +27¢coincidentabove fs
252.2Oblique3 1 3B3 +37¢close pairabove fs
252.4Axial0 5 0B3 +38¢close pairabove fs
254.4Tangential5 3 0C4 −49¢close pairabove fs
254.5Oblique5 1 2C4 −48¢close pairabove fs
255.4Tangential6 0 1C4 −41¢close pairabove fs
255.7Tangential1 5 0C4 −40¢close pairabove fs
259.8Tangential4 4 0C4 −12¢close pairabove fs
260.4Oblique6 1 1C4 −8¢close pairabove fs
260.6Oblique2 4 2C4 −7¢close pairabove fs
262.4Tangential0 5 1C4 +5¢close pairabove fs
262.6Tangential0 3 3C4 +7¢close pairabove fs
264.2Oblique5 3 1C4 +17¢close pairabove fs
264.8Oblique4 3 2C4 +21¢close pairabove fs
265.2Tangential6 2 0C4 +23¢close pairabove fs
265.3Tangential2 5 0C4 +24¢close pairabove fs
265.5Oblique1 5 1C4 +26¢close pairabove fs
265.8Oblique1 3 3C4 +27¢close pairabove fs
267.0Oblique3 2 3C4 +35¢above fs
269.1Oblique5 2 2C4 +49¢close pairabove fs
269.5Oblique4 4 1C#4 −49¢close pairabove fs
269.8Tangential4 0 3C#4 −47¢close pairabove fs
274.4Oblique4 1 3C#4 −17¢close pairabove fs
274.7Oblique6 2 1C#4 −16¢close pairabove fs
274.8Oblique2 5 1C#4 −15¢close pairabove fs
275.1Oblique2 3 3C#4 −13¢close pairabove fs
276.2Oblique3 4 2C#4 −6¢above fs
280.6Tangential3 5 0C#4 +21¢above fs
283.9Tangential6 0 2C#4 +41¢above fs
286.1Axial0 0 4D4 −45¢coincidentabove fs
286.1Axial7 0 0D4 −45¢coincidentabove fs
287.3Tangential5 4 0D4 −38¢close pairabove fs
288.0Oblique4 2 3D4 −34¢close pairabove fs
288.2Tangential6 3 0D4 −32¢close pairabove fs
288.4Oblique6 1 2D4 −32¢close pairabove fs
289.0Tangential1 0 4D4 −28¢close pairabove fs
289.6Oblique3 5 1D4 −24¢close pairabove fs
289.9Oblique3 3 3D4 −23¢close pairabove fs
290.1Tangential0 5 2D4 −21¢close pairabove fs
290.5Tangential7 1 0D4 −19¢coincidentabove fs
290.5Tangential0 1 4D4 −19¢coincidentabove fs
291.8Oblique5 3 2D4 −11¢above fs
293.0Oblique1 5 2D4 −4¢close pairabove fs
293.4Oblique1 1 4D4 −2¢close pairabove fs
294.7Tangential0 4 3D4 +6¢close pairabove fs
294.9Tangential7 0 1D4 +7¢close pairabove fs
296.1Oblique5 4 1D4 +14¢close pairabove fs
296.3Tangential5 0 3D4 +16¢close pairabove fs
296.6Oblique4 4 2D4 +17¢close pairabove fs
297.0Oblique6 3 1D4 +19¢close pairabove fs
297.5Oblique1 4 3D4 +22¢close pairabove fs
297.5Tangential2 0 4D4 +23¢close pairabove fs
299.2Oblique7 1 1D4 +32¢above fs

Why a room booms at some notes

Sound bounces between the walls. At certain frequencies the reflections line up with the sound going the other way and build a standing wave, or room mode: loud in some places, almost silent in others. The calculator uses the standard formula for a rectangular room:

f = (c / 2) · √((nx / L)² + (ny / W)² + (nz / H)²)

where c is the speed of sound at your air temperature and nx, ny and nz are whole numbers. One non-zero number gives an axial mode between two opposite surfaces, usually the strongest; two give a tangential mode around four surfaces; three give an oblique mode involving all six.

Low down, modes are few and far apart, so single notes boom and others thin out. Higher up they crowd together until the room behaves evenly; the Schroeder frequency estimates where that happens. The Bonello check counts modes in third-octave bands: the counts should never fall from one band to the next, and no two modes should coincide. Here “coincide” means the same frequency to 0.05 Hz, a tolerance this calculator chooses; pairs under 1 Hz apart are ringed on the chart as well.

The formula assumes a closed box with rigid walls. Under a sloping attic roof, or with an open door, real modes shift, so treat the list as a guide and confirm by measuring.

Sources

More for the attic studio

Reverb, reflections, speakers, mics and files.

Questions

Which modes matter most?

The low axial modes, between the room’s opposite surfaces. They are usually the strongest and the most widely spaced, so each one makes its note boom or vanish depending on where you sit. Look for two modes landing close together, and for wide gaps with none.

What reverb time should I use for the Schroeder frequency?

Your room’s own, measured or estimated. The 0.4 s default is only a starting value. The estimate changes with the square root, so doubling the reverb time raises the Schroeder frequency by about 41%.

My room fails the Bonello check. Is it a bad room?

Not necessarily. Bonello’s criterion is one published way to judge how evenly modes are spread, and it says nothing about treatment, furniture or where you sit. Use it to compare possible layouts or to spot a problem frequency, then measure.

Does it work for an attic with a sloping ceiling?

Only roughly. The formula is for rectangular rooms, so a sloping roof shifts the modes in ways it cannot predict. Use the length and width of the floor and a typical ceiling height as a starting point, and confirm with a measurement.