Sound pressure

Sound pressure or acoustic pressure is the local pressure deviation from the ambient (average or equilibrium) atmospheric pressure, caused by a sound wave. In air, sound pressure can be measured using a microphone, and in water with a hydrophone. The SI unit of sound pressure is the pascal (Pa).[1]

This article is about the measurement of audible sound. For the music album, see Sound Pressure Level.

Not to be confused with Sound energy density.

Sound measurements
Characteristic	Symbols
Sound pressure	p, SPL,LPA
Particle velocity	v, SVL
Particle displacement	δ
Sound intensity	I, SIL
Sound power	P, SWL, LWA
Sound energy	W
Sound energy density	w
Sound exposure	E, SEL
Acoustic impedance	Z
Audio frequency	AF
Transmission loss	TL

Mathematical definition

Sound pressure diagram:

1. silence;
2. audible sound;
3. atmospheric pressure;
4. sound pressure

A sound wave in a transmission medium causes a deviation (sound pressure, a dynamic pressure) in the local ambient pressure, a static pressure.

Sound pressure, denoted p, is defined by

${\displaystyle p_{\mathrm {total} }=p_{\mathrm {stat} }+p}$

where

• p_total is the total pressure;
• p_stat is the static pressure.

Sound measurements

Sound intensity

Main article: Sound intensity

In a sound wave, the complementary variable to sound pressure is the particle velocity. Together, they determine the sound intensity of the wave.
Sound intensity, denoted I and measured in W·m⁻² in SI units, is defined by

${\displaystyle \mathbf {I} =p\mathbf {v} ,}$

where

• p is the sound pressure;
• v is the particle velocity.

Acoustic impedance

Main article: Acoustic impedance

Acoustic impedance, denoted Z and measured in Pa·m⁻³·s in SI units, is defined by[2]

${\displaystyle Z(s)={\frac {{\hat {p}}(s)}{{\hat {Q}}(s)}},}$

where

• ${\displaystyle {\hat {p}}(s)}$ is the Laplace transform of sound pressure;
• ${\displaystyle {\hat {Q}}(s)}$ is the Laplace transform of sound volume flow rate.

Specific acoustic impedance, denoted z and measured in Pa·m⁻¹·s in SI units, is defined by[2]

${\displaystyle z(s)={\frac {{\hat {p}}(s)}{{\hat {v}}(s)}},}$

where

• ${\displaystyle {\hat {p}}(s)}$ is the Laplace transform of sound pressure;
• ${\displaystyle {\hat {v}}(s)}$ is the Laplace transform of particle velocity.

Particle displacement

Main article: Particle displacement

The particle displacement of a progressive sine wave is given by

${\displaystyle \delta (\mathbf {r} ,\,t)=\delta _{\mathrm {m} }\cos(\mathbf {k} \cdot \mathbf {r} -\omega t+\varphi _{\delta ,0}),}$

where

• ${\displaystyle \delta _{\mathrm {m} }}$ is the amplitude of the particle displacement;
• ${\displaystyle \varphi _{\delta ,0}}$ is the phase shift of the particle displacement;
• k is the angular wavevector;
• ω is the angular frequency.

It follows that the particle velocity and the sound pressure along the direction of propagation of the sound wave x are given by

${\displaystyle v(\mathbf {r} ,\,t)={\frac {\partial \delta }{\partial t}}(\mathbf {r} ,\,t)=\omega \delta _{\mathrm {m} }\cos \!\left(\mathbf {k} \cdot \mathbf {r} -\omega t+\varphi _{\delta ,0}+{\frac {\pi }{2}}\right)=v_{\mathrm {m} }\cos(\mathbf {k} \cdot \mathbf {r} -\omega t+\varphi _{v,0}),}$

${\displaystyle p(\mathbf {r} ,\,t)=-\rho c^{2}{\frac {\partial \delta }{\partial x}}(\mathbf {r} ,\,t)=\rho c^{2}k_{x}\delta _{\mathrm {m} }\cos \!\left(\mathbf {k} \cdot \mathbf {r} -\omega t+\varphi _{\delta ,0}+{\frac {\pi }{2}}\right)=p_{\mathrm {m} }\cos(\mathbf {k} \cdot \mathbf {r} -\omega t+\varphi _{p,0}),}$

where

• v_m is the amplitude of the particle velocity;
• ${\displaystyle \varphi _{v,0}}$ is the phase shift of the particle velocity;
• p_m is the amplitude of the acoustic pressure;
• ${\displaystyle \varphi _{p,0}}$ is the phase shift of the acoustic pressure.

Taking the Laplace transforms of v and p with respect to time yields

${\displaystyle {\hat {v}}(\mathbf {r} ,\,s)=v_{\mathrm {m} }{\frac {s\cos \varphi _{v,0}-\omega \sin \varphi _{v,0}}{s^{2}+\omega ^{2}}},}$

${\displaystyle {\hat {p}}(\mathbf {r} ,\,s)=p_{\mathrm {m} }{\frac {s\cos \varphi _{p,0}-\omega \sin \varphi _{p,0}}{s^{2}+\omega ^{2}}}.}$

Since ${\displaystyle \varphi _{v,0}=\varphi _{p,0}}$, the amplitude of the specific acoustic impedance is given by

${\displaystyle z_{\mathrm {m} }(\mathbf {r} ,\,s)=|z(\mathbf {r} ,\,s)|=\left|{\frac {{\hat {p}}(\mathbf {r} ,\,s)}{{\hat {v}}(\mathbf {r} ,\,s)}}\right|={\frac {p_{\mathrm {m} }}{v_{\mathrm {m} }}}={\frac {\rho c^{2}k_{x}}{\omega }}.}$

Consequently, the amplitude of the particle displacement is related to that of the acoustic velocity and the sound pressure by

${\displaystyle \delta _{\mathrm {m} }={\frac {v_{\mathrm {m} }}{\omega }},}$

${\displaystyle \delta _{\mathrm {m} }={\frac {p_{\mathrm {m} }}{\omega z_{\mathrm {m} }(\mathbf {r} ,\,s)}}.}$

Inverse-proportional law

Further information: Inverse-square law

When measuring the sound pressure created by a sound source, it is important to measure the distance from the object as well, since the sound pressure of a spherical sound wave decreases as 1/r from the centre of the sphere (and not as 1/r², like the sound intensity):[3]

${\displaystyle p(r)\propto {\frac {1}{r}}.}$

This relationship is an inverse-proportional law.

If the sound pressure p₁ is measured at a distance r₁ from the centre of the sphere, the sound pressure p₂ at another position r₂ can be calculated:

${\displaystyle p_{2}={\frac {r_{1}}{r_{2}}}\,p_{1}.}$

The inverse-proportional law for sound pressure comes from the inverse-square law for sound intensity:

${\displaystyle I(r)\propto {\frac {1}{r^{2}}}.}$

Indeed,

${\displaystyle I(r)=p(r)v(r)=p(r)\left[p*z^{-1}\right](r)\propto p^{2}(r),}$

where

• ${\displaystyle *}$ is the convolution operator;
• z⁻¹ is the convolution inverse of the specific acoustic impedance,

hence the inverse-proportional law:

${\displaystyle p(r)\propto {\frac {1}{r}}.}$

The sound pressure may vary in direction from the centre of the sphere as well, so measurements at different angles may be necessary, depending on the situation. An obvious example of a sound source whose spherical sound wave varies in level in different directions is a bullhorn.

Sound pressure level

Sound pressure level (SPL) or acoustic pressure level is a logarithmic measure of the effective pressure of a sound relative to a reference value.
Sound pressure level, denoted L_p and measured in dB, is defined by[4]

${\displaystyle L_{p}=\ln \!\left({\frac {p}{p_{0}}}\right)\!~\mathrm {Np} =2\log _{10}\!\left({\frac {p}{p_{0}}}\right)\!~\mathrm {B} =20\log _{10}\!\left({\frac {p}{p_{0}}}\right)\!~\mathrm {dB} ,}$

where

• p is the root mean square sound pressure;[5]
• p₀ is the reference sound pressure;
• 1 Np is the neper;
• 1 B = (1/2 ln 10) Np is the bel;
• 1 dB = (1/20 ln 10) Np is the decibel.

The commonly used reference sound pressure in air is[6]

${\displaystyle p_{0}=20~\mathrm {\mu Pa} ,}$

which is often considered as the threshold of human hearing (roughly the sound of a mosquito flying 3 m away). The proper notations for sound pressure level using this reference are L_{p/(20 μPa)} or L_p (re 20 μPa), but the suffix notations dB SPL, dB(SPL), dBSPL, or dB_SPL are very common, even if they are not accepted by the SI.[7]

Most sound level measurements will be made relative to this reference, meaning 1 Pa will equal an SPL of 94 dB. In other media, such as underwater, a reference level of 1 μPa is used.[8] These references are defined in ANSI S1.1-2013.[9]

The main instrument for measuring sound levels in the environment is the sound level meter. Most sound level meters provide readings in A, C, and Z-weighted decibels and must meet international standards such as IEC 61672 - 2013.

Examples

The lower limit of audibility is defined as SPL of 0 dB, but the upper limit is not as clearly defined. While 1 atm (194 dB Peak or 191 dB SPL) is the largest pressure variation an undistorted sound wave can have in Earth's atmosphere, larger sound waves can be present in other atmospheres or other media such as under water, or through the Earth.[10]

Equal-loudness contour, showing sound-pressure-vs-frequency at different perceived loudness levels.

Ears detect changes in sound pressure. Human hearing does not have a flat spectral sensitivity (frequency response) relative to frequency versus amplitude. Humans do not perceive low- and high-frequency sounds as well as they perceive sounds between 3,000 and 4,000 Hz, as shown in the equal-loudness contour. Because the frequency response of human hearing changes with amplitude, three weightings have been established for measuring sound pressure: A, B and C. A-weighting applies to sound pressures levels up to 55 dB, B-weighting applies to sound pressures levels between 55 dB and 85 dB, and C-weighting is for measuring sound pressure levels above 85 dB.[10]

In order to distinguish the different sound measures a suffix is used: A-weighted sound pressure level is written either as dB_A or L_A. B-weighted sound pressure level is written either as dB_B or L_B, and C-weighted sound pressure level is written either as dB_C or L_C. Unweighted sound pressure level is called "linear sound pressure level" and is often written as dB_L or just L. Some sound measuring instruments use the letter "Z" as an indication of linear SPL.[10]

Distance

The distance of the measuring microphone from a sound source is often omitted when SPL measurements are quoted, making the data useless, due the inherent effect of the inverse square law, which summarily states that doubling the distance between the source and receiver results in dividing the measurable effect by four. In the case of ambient environmental measurements of "background" noise, distance need not be quoted as no single source is present, but when measuring the noise level of a specific piece of equipment the distance should always be stated. A distance of one metre (1 m) from the source is a frequently used standard distance. Because of the effects of reflected noise within a closed room, the use of an anechoic chamber allows for sound to be comparable to measurements made in a free field environment.[10]

According to the inverse proportional law, when sound level L_p1 is measured at a distance r₁, the sound level L_p2 at the distance r₂ is

${\displaystyle L_{p_{2}}=L_{p_{1}}+20\log _{10}\!\left({\frac {r_{1}}{r_{2}}}\right)\!~\mathrm {dB} .}$

Multiple sources

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

${\displaystyle L_{\Sigma }=10\log _{10}\!\left({\frac {{p_{1}}^{2}+{p_{2}}^{2}+\ldots +{p_{n}}^{2}}{{p_{0}}^{2}}}\right)\!~\mathrm {dB} =10\log _{10}\!\left[\left({\frac {p_{1}}{p_{0}}}\right)^{2}+\left({\frac {p_{2}}{p_{0}}}\right)^{2}+\ldots +\left({\frac {p_{n}}{p_{0}}}\right)^{2}\right]\!~\mathrm {dB} .}$

Inserting the formulas

${\displaystyle \left({\frac {p_{i}}{p_{0}}}\right)^{2}=10^{\frac {L_{i}}{10\,\mathrm {dB} }},\quad i=1,\,2,\,\ldots ,\,n,}$

in the formula for the sum of the sound pressure levels yields

${\displaystyle L_{\Sigma }=10\log _{10}\!\left(10^{\frac {L_{1}}{10\,\mathrm {dB} }}+10^{\frac {L_{2}}{10\,\mathrm {dB} }}+\ldots +10^{\frac {L_{n}}{10\,\mathrm {dB} }}\right)\!~\mathrm {dB} .}$

Examples of sound pressure

Examples of sound pressure in air at standard atmospheric pressure

Source of sound	Distance	Sound pressure level
		[lower-alpha 1](Pa)	(dBSPL)
1883 eruption of Krakatoa; pressure wave from the third explosion		~6.32×10^10	~310
Shock wave (distorted sound waves > 1 atm; waveform valleys are clipped at zero pressure)		1.01×10^5+	194+
Simple open-ended thermoacoustic device[11]		1.26×10^4	176
.30-06 rifle being fired	1 m to shooter's side	7.27×10^3	171
Stun grenade[12]	Ambient	1.60×10^3 ...8.00×10^3	158–172
9-inch (23 cm) party balloon inflated to rupture [13]	At ear	4.92×10^3	168
9-inch (23 cm) diameter balloon crushed to rupture [13]	At ear	1.79×10^3	159
9-inch (23 cm) diameter balloon popped with a pin [13]	At ear	1.13×10^3	155
LRAD 1000Xi Long Range Acoustic Device[14]	1 m	8.93×10^2	153
9-inch (23 cm) party balloon inflated to rupture [13]	1 m	731	151
Jet engine[10]	1 m	632	150
9-inch (23 cm) diameter balloon crushed to rupture [13]	0.95 m	448	147
9-inch (23 cm) diameter balloon popped with a pin [13]	1 m	282.5	143
Threshold of pain[15][16][17]	At ear	63.2–200	130–140
Loudest human voice[17]	1 inch	110	135
Trumpet[18]	0.5 m	63.2	130
Vuvuzela horn[19]	1 m	20.0	120
Risk of instantaneous noise-induced hearing loss	At ear	20.0	120
Jet engine	100–30 m	6.32–200	110–140
Two-stroke chainsaw[20]	1 m	6.32	110
Jack hammer	1 m	2.00	100
Traffic on a busy roadway	10 m	0.20–0.63	80–90
Hearing damage (over long-term exposure, need not be continuous)[21]	At ear	0.36	85
Passenger car	10 m	0.02–0.20	60–80
EPA-identified maximum to protect against hearing loss and other disruptive effects from noise, such as sleep disturbance, stress, learning detriment, etc.[22]	Ambient	0.06	70
TV (set at home level)	1 m	0.02	60
Normal conversation	1 m	2×10^−3–0.02	40–60
Very calm room	Ambient	2.00×10^−4 ...6.32×10^−4	20–30
Light leaf rustling, calm breathing[10]	Ambient	6.32×10^−5	10
Auditory threshold at 1 kHz[21]	At ear	2.00×10^−5	0
Anechoic chamber, Orfield Labs, A-weighted[23][24]	Ambient	6.80×10^−6	−9.4
Anechoic chamber, University of Salford, A-weighted[25]	Ambient	4.80×10^−6	−12.4
Anechoic chamber, Microsoft, A-weighted[26][27]	Ambient	1.90×10^−6	−20.35

1. All values listed are the effective sound pressure unless otherwise stated.

The relation between pressure waves and the production of X-rays in air discharges

Pressure and shock waves released by electric discharges are capable of perturbing the air in their vicinity up to 80%. [28][29] This, however, has immediate consequences on the motion and properties of secondary streamer discharges in perturbed air: Depending on the direction (relative to the ambient electric field), air perturbations change the discharge velocities, facilitate branching or trigger the spontaneous initiation of a counter discharge. [30] Recent simulations have shown that such perturbations are even capable to facilitate the production of X-rays (with energies of several tens of keV) from such streamer discharges which are produced by run-away electrons through the Bremsstrahlung process. [31]

See also

• Acoustics
• Phon (unit)
• Loudness
• Sone (unit)
• Sound level meter
• Stevens' power law
• Weber–Fechner law, especially The case of sound

References

1. "Sound Pressure is the force of sound on a surface area perpendicular to the direction of the sound". Retrieved 22 April 2015.
2. Wolfe, J. "What is acoustic impedance and why is it important?". University of New South Wales, Dept. of Physics, Music Acoustics. Retrieved 1 January 2014.
3. Longhurst, R.S. (1967). Geometrical and Physical Optics. Norwich: Longmans.
4. "Letter symbols to be used in electrical technology – Part 3: Logarithmic and related quantities, and their units", IEC 60027-3 Ed. 3.0, International Electrotechnical Commission, 19 July 2002.
5. Bies, David A., and Hansen, Colin. (2003). Engineering Noise Control.
6. Ross Roeser, Michael Valente, Audiology: Diagnosis (Thieme 2007), p. 240.
7. Thompson, A. and Taylor, B. N. sec 8.7, "Logarithmic quantities and units: level, neper, bel", Guide for the Use of the International System of Units (SI) 2008 Edition, NIST Special Publication 811, 2nd printing (November 2008), SP811 PDF
8. Morfey, Christopher L. (2001). Dictionary of Acoustics. San Diego: Academic Press. ISBN 978-0125069403.
9. "Noise Terms Glossary". Retrieved 2012-10-14.
10. Winer, Ethan (2013). "1". The Audio Expert. New York and London: Focal Press. ISBN 978-0-240-82100-9.
11. HATAZAWA, Masayasu; SUGITA, Hiroshi; OGAWA, Takahiro; SEO, Yoshitoki (2004-01-01). "Performance of a Thermoacoustic Sound Wave Generator driven with Waste Heat of Automobile Gasoline Engine". Transactions of the Japan Society of Mechanical Engineers Series B. 70 (689): 292–299. doi:10.1299/kikaib.70.292. ISSN 0387-5016.
12. "NIOSH [2014]. Health hazard evaluation report: measurement of exposure to impulsive noise at indoor and outdoor firing ranges during tactical training exercises. By Brueck SE, Kardous CA, Oza A, Murphy WJ. Cincinnati, OH: U.S. Department of Health and Human Services, Centers for Disease Control and Prevention, National Institute for Occupational Safety and Health, NIOSH HHE Report No. 2013-0124-3208" (PDF).
13. "Did You Know How Loud Balloons Can Be?". Retrieved 8 June 2018.
14. "LRAD Corporation Product Overview for LRAD 1000Xi". Retrieved 29 May 2014.
15. Nave, Carl R. (2006). "Threshold of Pain". HyperPhysics. SciLinks. Retrieved 2009-06-16.
16. Franks, John R.; Stephenson, Mark R.; Merry, Carol J., eds. (June 1996). Preventing Occupational Hearing Loss - A Practical Guide (PDF). National Institute for Occupational Safety and Health. p. 88. Retrieved 2009-07-15.
17. Realistic Maximum Sound Pressure Levels for Dynamic Microphones – Shure
18. Recording Brass & Reeds
19. Swanepoel, De Wet; Hall III, James W; Koekemoer, Dirk (February 2010). "Vuvuzela – good for your team, bad for your ears" (PDF). South African Medical Journal. 100 (4): 99–100. doi:10.7196/samj.3697. PMID 20459912.
20. "Decibel Table - SPL - Loudness Comparison Chart". sengpielaudio. Retrieved 5 Mar 2012.
21. William Hamby. "Ultimate Sound Pressure Level Decibel Table". Archived from the original on 2005-10-19.
22. "EPA Identifies Noise Levels Affecting Health and Welfare" (Press release). Environmental Protection Agency. April 2, 1974. Retrieved March 27, 2017.
23. ""THE QUIETEST PLACE ON EARTH" - GUINNESS WORLD RECORDS CERTIFICATE, 2005" (PDF). Orfield Labs.
24. Middlemiss, Neil (December 18, 2007). "The Quietest Place on Earth - Orfield Labs [audiojunkies]". Audio Junkies, Inc. Archived from the original on 2010-11-21.
25. Eustace, Dave. "Anechoic Chamber". University of Salford.
26. "Microsoft lab sets new record for the world's quietest place". 2015-10-02. Retrieved 2016-09-20. The computer company has built an anechoic chamber in which highly sensitive tests reported an average background noise reading of an unimaginably quiet -20.35 dBA (decibels A-weighted).
27. "Check out the world's quietest room". Microsoft: Inside B87. Retrieved 2016-09-20.
28. Marode, E.; Bastien, F.; Bakker, M. (1979). "A model of the streamer included spark formation based on neutral dynamics". J. Appl. Phys. 50: 140–146. doi:10.1063/1.325697.
29. Kacem, S.; et al. (2013). "Simulation of expansion of thermal shock and pressure waves induced by a streamer dynamics in positive DC corona discharges". IEEE Transactions on Plasma Science. 41: 942–947. doi:10.1109/tps.2013.2249118.
30. Köhn, C.; Chanrion, O.; Babich, L.P.; Neubert, T. (2018). "Streamer properties and associated x-rays in perturbed air". Plasma Sour. Sci. Technol. 27: 015017. doi:10.1088/1361-6595/aaa5d8.
31. Köhn, C.; Chanrion, O.; Neubert, T. (2018). "High-Energy Emissions Induced by Air Density Fluctuations of Discharges". Geophys. Res. Lett. 45: 5194–5203. doi:10.1029/2018GL077788. PMC 6049893. PMID 30034044.

General

• Beranek, Leo L., Acoustics (1993), Acoustical Society of America, ISBN 0-88318-494-X.
• Daniel R. Raichel, The Science and Applications of Acoustics (2006), Springer New York, ISBN 1441920803.

External links

• Sound Pressure and Sound Power, Effect and Cause
• Conversion of Sound Pressure to Sound Pressure Level and Vice Versa
• Table of Sound Levels, Corresponding Sound Pressure and Sound Intensity
• Ohm's Law as Acoustic Equivalent, Calculations
• Relationships of Acoustic Quantities Associated with a Plane Progressive Acoustic Sound Wave
• Sound Pressure and Sound Power, Two Commonly Confused Characteristics of Sound
• How Many Decibels Is Twice as Loud? Sound Level Change and the Respective Factor of Sound Pressure or Sound Intensity
• Decibel (Loudness) Comparison Chart