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AC-05Acoustic Fundamentals

Wavelength & Frequency

How long is a sound wave? Wavelength, period and wavenumber in air, water and solids.

Inputs

Hz
°C
Wavelength λ
0.3432m
λ / 4
0.0858m
Period T
1ms
Wavenumber k
18.31rad/m
Speed of sound 343.2 m/s. One wavelength is about 1.6 × a football.
Pressure along the propagation axissnapshot, two wavelengths
λ = 0.343 mλ/4λ/2λ00.10.20.30.40.50.6-101Distance (m)Pressure (norm.)
Wavelength vs frequency
audible0.343 m1101001k10k100k0.0010.010.11101001k10kFrequency (Hz)Wavelength (m)
AirWaterSteel
§ Theory of operation

The wave equation in one line

For any travelling wave, speed equals frequency times wavelength:

\lambda = c\,/\,f \qquad T = 1\,/\,f \qquad k = 2\pi\,/\,\lambda = \omega\,/\,c

In air at 20 °C (c ≈ 343 m/s), audible sound spans an astonishing range: about 17 m at 20 Hz down to 17 mm at 20 kHz, a factor of 1000. This is why acoustics behaves so differently across the spectrum.

Why wavelength matters

  • Absorbers: a porous absorber works well once its thickness approaches λ/4. Effective bass absorption therefore needs deep treatment or resonant absorbers.
  • Barriers and diffraction: obstacles small compared with λ are transparent to sound; low frequencies bend around walls and buildings.
  • Room modes appear when a room dimension equals a multiple of λ/2.
  • Microphone spacing in intensity probes and arrays must be small compared with λ to avoid spatial aliasing.
  • Near field: close to a source (within about λ/2π or the source size) pressure and velocity are not in phase and the inverse-square law does not yet apply.

Solids and liquids

Sound travels faster in stiffer media, so wavelengths are longer: a 1 kHz longitudinal wave in steel is almost 6 m long. Note that plates and beams also carry slower, dispersive bending waves whose speed rises with √f, see the panel transmission-loss calculator.