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Sound pressure is the local pressure deviation from the ambient (average, or equilibrium) pressure caused by a sound wave. Sound pressure can be measured using a microphone in air and a hydrophone in water. The SI unit for sound pressure is the pascal (symbol: Pa). The instantaneous sound pressure is the deviation from the local ambient pressure p_{0} caused by a sound wave at a given location and given instant in time. The effective sound pressure is the root mean square of the instantaneous sound pressure over a given interval of time (or space). In a sound wave, the complementary variable to sound pressure is the acoustic particle velocity. For small amplitudes, sound pressure and particle velocity are linearly related and their ratio is the acoustic impedance. The acoustic impedance depends on both the characteristics of the wave and the medium. The local instantaneous sound intensity is the product of the sound pressure and the acoustic particle velocity and is, therefore, a vector quantity.

The sound pressure deviation p is

- $$

where

- F = force,

- A = area.

The entire pressure p_{total} is

- $$

where

- p
_{0}= local ambient pressure,

- p = sound pressure deviation.

- $$

Sometimes variants are used such as dB (SPL), dBSPL, or dB_{SPL}. These variants are not permitted by SI.

The commonly used reference sound pressure in air is $p\_\{mathrm\{ref\}\}$ = 20 µPa (rms), which is usually considered the threshold of human hearing (roughly the sound of a mosquito flying 3 m away). When dealing with hearing, the perceived loudness of a sound correlates roughly logarithmically to its sound pressure. See also Weber-Fechner law. Most measurements of audio equipment will be made relative to this level, meaning 1 pascal will equal 94 dB of sound pressure.

In other media, such as underwater, a reference level of 1 µPa is more often used.

These references are defined in ANSI S1.1-1994.

The unit dB (SPL) is often abbreviated to just "dB", which gives some the erroneous notion that a dB is an absolute unit by itself.

The human ear is a sound pressure sensitive detector. It does not have a flat spectral response, so the sound pressure is often frequency weighted such that the measured level will match the perceived level. When weighted in this way the measurement is referred to as a sound level. The International Electrotechnical Commission (IEC) has defined several weighting schemes. A-weighting attempts to match the response of the human ear to pure tones, while C-weighting is used to measure peak sound levels. If the (unweighted) SPL is desired, many instruments allow a "flat" or unweighted measurement to be made. See also Weighting filter.

When measuring the sound created by an object, it is important to measure the distance from the object as well, since the SPL decreases in distance from a point source with 1/r (and not with 1/r^{2}, like sound intensity). It often varies in direction from the source, as well, so many measurements may be necessary, depending on the situation. An obvious example of a source that varies in level in different directions is a bullhorn.

Sound pressure p in N/m² or Pa is

- $$

where

- Z is acoustic impedance, sound impedance, or characteristic impedance, in Pa·s/m

- v is particle velocity in m/s

- J is acoustic intensity or sound intensity, in W/m
^{2}

Sound pressure p is connected to particle displacement (or particle amplitude) ξ, in m, by

- $$

Sound pressure p is

- $$

normally in units of N/m² = Pa.

where:

Symbol | SI Unit | Meaning |
---|---|---|

p | pascals | sound pressure |

f | hertz | frequency |

ρ | kg/m³ | density of air |

c | m/s | speed of sound |

v | m/s | particle velocity |

$omega$ = 2 · $pi$ · f | radians/s | angular frequency |

ξ | meters | particle displacement |

Z = c • ρ | N·s/m³ | acoustic impedance |

a | m/s² | particle acceleration |

J | W/m² | sound intensity |

E | W·s/m³ | sound energy density |

P_{ac}
| watts | sound power or acoustic power |

A | m² | Area |

The distance law for the sound pressure p is inverse-proportional to the distance r of a punctual sound source.

- $$

- $$

- $$

The assumption of 1/r² with the square is here wrong. That is only correct for sound intensity.

Note: The often used term "intensity of sound pressure" is not correct. Use "magnitude", "strength", "amplitude", or "level" instead. "Sound intensity" is sound power per unit area, while "pressure" is a measure of force per unit area. Intensity is not equivalent to pressure.

- $$

Source of sound | Sound pressure | Sound pressure level |
---|---|---|

pascal | dB re 20 μPa | |

Krakatoa explosion at 100 miles (160 km) in air | 20,000 Pa | 180 dB |

Simple open-ended thermoacoustic device | 12,000 Pa | 176 dB |

M1 Garand being fired at 1 m | 5,000 Pa | 168 dB |

Jet engine at 30 m | 630 Pa | 150 dB |

Rifle being fired at 1 m | 200 Pa | 140 dB |

Threshold of pain | 100 Pa | 130 dB |

Hearing damage (due to short-term exposure) | 20 Pa | approx. 120 dB |

Jet at 100 m | 6 – 200 Pa | 110 – 140 dB |

Jack hammer at 1 m | 2 Pa | approx. 100 dB |

Hearing damage (due to long-term exposure) | 6×10^{−1} Pa
| approx. 85 dB |

Major road at 10 m | 2×10^{−1} – 6×10^{−1} Pa
| 80 – 90 dB |

Passenger car at 10 m | 2×10^{−2} – 2×10^{−1} Pa
| 60 – 80 dB |

TV (set at home level) at 1 m | 2×10^{−2} Pa
| approx. 60 dB |

Normal talking at 1 m | 2×10^{−3} – 2×10^{−2} Pa
| 40 – 60 dB |

Very calm room | 2×10^{−4} – 6×10^{−4} Pa
| 20 – 30 dB |

Leaves rustling, calm breathing | 6×10^{−5} Pa
| 10 dB |

Auditory threshold at 1 kHz | 2×10^{−5} Pa
| 0 dB |

Sound pressure in water:

Source of sound | Sound pressure | Sound pressure level |
---|---|---|

pascal | dB re 1 μPa | |

Auditory threshold of a diver at 1 kHz | 2.2 · 10^{-3} Pa
| 67 dB |

The formula for the sum of the sound pressure levels of n incoherent radiating sources is

- $$

From the formula of the sound pressure level we find

- $$

This inserted in the formula for the sound pressure level to calculate the sum level shows

- $$

- Acoustics
- Amplitude
- Decibel, especially the Acoustics section
- Loudness
- Sone
- Sound level meter
- Sound power level
- Stevens' power law
- Weber–Fechner law, espeically The case of sound

- Beranek, Leo L, "Acoustics" (1993) Acoustical Society of America. ISBN 0-88318-494-X
- Morfey, Christopher L, "Dictionary of Acoustics" (2001) Academic Press, San Diego.

- Conversion of sound pressure to sound pressure level and vice versa
- Table of Sound Levels - Corresponding Sound Pressure and Sound Intensity
- William Hamby (2004) Ultimate Sound Pressure Level Decibel Table
- Ohm's law as acoustic equivalent - calculations
- Definition of sound pressure level
- A table of SPL values
- Relationships of acoustic quantities associated with a plane progressive acoustic sound wave - pdf
- Sound pressure and sound power - two commonly confused characteristics of sound

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Last updated on Tuesday October 07, 2008 at 21:35:56 PDT (GMT -0700)

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This article is licensed under the GNU Free Documentation License.

Last updated on Tuesday October 07, 2008 at 21:35:56 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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