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Reverberation

Reverberation is the persistence of sound in an enclosed volume due to multiple reflections on the enclosed surfaces after the sound source has been stopped. Reverberation is usually quantified as reverberation time, T60.

Figure 1: Reverberation due to Acoustic Reflections in Enclosed Space (Source: [1])

Reverberation vs Echo

Parameter Reverberation Echo
Intuition Similar to time constant of a physical system; the response after providing an impluse excitation Product of multiple reflections that last a very short time span (no longer than 22 ms) which arrived well after the direct sound (i.e., more than 100 ms)
Perception Perceived continuously by listener Perceived as discrete sounds
Example Response of “Hi” “Hhhhhiiiiiiiiiii…” “Hi”…“Hi”…“Hi”…

Absorption Coefficient, α

When sound wave impinges on a material, part of the energy will be reflected, another part will be transmitted through, and the last part will be absorbed as heat loss aas shown in Figure 2. Absorption coefficient is used to quantify the transmitted and absorbed part when sound wave strikes a material.

Figure 2: Incident (Ii), reflected (Ir), Absorbed (Ia), and Transmitted (It) Waves (Source: [1])

Absorption coefficient is defined as the ratio of absorbed energy over incident energy.

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Where :

  • A = equivalent absorption area
  • S = surface area
  • α = absorption coefficient

More information on α :

  • α range from 0 to 1
  • α is frequency dependent
  • material are considered absorptive if α > 0.5
  • thicker materials have better absorptive performance in low-frequency range
  • absorptive material usually low airflow resistivity

Reverberation Time, T60

Reverberation time (RT) is defined as the time taken for a sound source level to decay by 60 dB after the sound source is stopped across frequency bands. RT is frequency dependent.

Sometimes, a change of slope could be observed in a reverberation curve which usually indicates the presence of a flutter echo.

Figure 3: Example of Reverberation Time Curve with Flutter Echo (Source: [1])

Reverberation Time Design Standards

Standard Title
AS/NZS 2107:2016 Acoustics-Recommended Design Sound Levels and Reverberation Times for Building Interiors

Reverberation Time Measurement

  1. Creating a sufficiently loud noise (usually > 90 dB) either by impulse noise (e.g.: blank pistol shot/balloon burst) or random noise signal (pink/white noise)
  2. Measure the response of the enclosed space using a calibrated sound level meter (response time set to “impulse” option)
  3. Plot the response across different octave bands to obtain the time taken for 60 dB drop
  4. If the decay of 60 dB is not attainable (occurs frequently), extrapolation from T20 or T30 could be used as well, given that the decay is linear
Extrapolation Method T30 T20
Equation T60 ≈ 2(T30) T60 ≈ 3(T20)

Reverberation Time Measurement Standards

Standard Scenario
ISO 3382-1 standard for performance spaces
ISO 3382-2 standard for ordinary rooms
ISO 3382-3 standard for open-plan offices
ASTM E2235 standard for use in sound insulation

Reverberation Time Computations

Sabine Equation

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Where :

  • c20 = speed of sound at 20 °C [m/s^2]
  • V = the volume of enclosed space [m^3]
  • S = the total surface area of enclosed space [m^2]
  • α = the average absorption coefficient of room surfaces
  • = the total absorption [sabins]

Sabine equation :

  • assumed that the enclosed volumes have rather reflective surfaces with similar dimensions (“live” rooms)
  • tends to over-predict reverberation time for small rooms with high amounts of absorption
  • will perform poorly (low accuracy) when the absorption in a volume is larger
  • only valid for uniform volumes like cuboid

Eyring Equation

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Eyring equation :

  • better estimates the RT in small rooms with relatively large quantities of sound absorption (“dead” rooms)
  • approximates to Sabine equation for very “live” rooms
  • usually used for recording studios or critical listening environments

Spatial Sound Level Decay

Although reverberation time is widely used, it is not always the best for describing internal acoustics. For example:

A flat encumbered space will feature a rather low value, sometimes similar to that for a small lounge, while people inside will find the acoustics uncomfortable.

For such situations, one may use the spatial sound level decay DL2, which is the rate of sound level decay with doubling of distance. As shown in Figure 4, it is possible to distinguish the direct field region close to the source (where the influence of the room is not yet felt) and the far field region (where one is left with the reverberant field). In between stands the intermediate region, which is controlled by the acoustic treatment of the room.

Figure 4: Spatial Sound Level Decay Curve (Source: [1])


References

[1] M. Asselineau, Building Acoustics. Boca Raton, Florida: CRC Press, 2015.

[2] D. A. Bies, C. H. Hansen, and C. Q. Howard, Engineering Noise Control, 5th ed. Boca Raton, Florida: CRC Press, 2017.

[3] Wikipedia, Reverberation, Wikipedia, Jan. 10, 2022. Accessed on: Apr. 13, 2022. [Online]. Available: https://en.wikipedia.org/wiki/Reverberation