Matter and energy 4.11

Sound and Waves

Did you know?

The same noise can measure 150 dB in water and 90 dB in air. Yet it is exactly the same energy.

An old engraving shows a large horn lying on its side, connected to a cylinder turned by a crank.
Édouard-Léon Scott de Martinville’s phonautograph, 1859 model: engraving published in 1865 in a book by Franz Josef Pisko. Édouard-Léon Scott de Martinville (1817–1879), Public domain, source

The same noise can measure 150 dB in water and 90 dB in air. Yet it is exactly the same energy.

This page is about decibels, and it is the best place on the site to address a fundamental question: what exactly does this number count?

1. First, what a sound is

A sound is matter that vibrates.

When you strike a drum, the skin trembles, pushes the air touching it, that air pushes the neighbouring air, and so on all the way to the ear. Sound travels through a succession of compressions and expansions in a medium — air, water, metal.1

No matter, no sound. In space, nothing can vibrate: an exploding spaceship makes no noise there. It is one of the few errors of physics that most science-fiction films still perpetuate.

The stiffer the medium — the harder it is to compress — the faster sound travels. (It is not density that counts: at equal stiffness, a denser medium slows sound down. Steel is fast because it is very stiff, despite its weight.)2

MediumAverage speedPractical example
Air~ 340 m/sStandard propagation in everyday life
Water~ 1,500 m/sUnderwater sounds and echolocation
Steel~ 6,000 m/sYou hear the train on the rail before you hear it through the air

Sources for the table3

2. What makes a sound high or low

A guitar string that vibrates fast produces a high sound. The same string, slacker, vibrates slowly and produces a low sound. What changes is the number of back-and-forth movements per second: the frequency.

It is measured in hertz: one hertz corresponds to one vibration per second. The low E string of a guitar vibrates about 82 times per second; the high E string, about 330 times. That is four times faster, two octaves higher.4

The human ear perceives roughly 20 to 20,000 hertz. This is a range, not a boundary: it narrows with age, especially at the top, and a fifty-year-old adult rarely hears above 15,000 hertz. What you hear at a given age, you will not hear all your life.5

Beyond these limits, sound still exists — it is the ear that stops, not physics. Below 20 hertz, we speak of infrasound: elephants use it to communicate over several kilometres. Above 20,000 hertz, of ultrasound: bats use it to see in the dark.

Two different notions must not be confused. Frequency distinguishes high from low. The decibel, which the whole rest of this page deals with, distinguishes loud from soft. A very high sound can be very soft, and a very low sound can be deafening. These are two independent scales.

3. The decibel is not a unit

A metre is a metre. A kilogram is a kilogram. These are units: they measure an absolute quantity.

The decibel is not a unit. It is a ratio.6

It does not directly measure a quantity of sound: it compares the energy of a sound with a chosen reference. Reading “60 decibels” means “60 decibels above the reference”. In air, this reference is a fixed convention close to the faintest sound a normal human ear can perceive (20 µPa).7

Without the reference, the number loses all meaning.

The evidence from water

Underwater, acousticians use a different reference (1 µPa), twenty times smaller. The result: a sound of the same physical energy is measured at about 61 decibels more in water than in air.8

  • 150 dB underwater ≠ 150 dB in air.
  • A single number, two distinct conventions, two different physical realities.

But the quick explanation, the one found almost everywhere, calls for caution: “the gap comes from the change of reference”. This is true, but insufficient.

Going from 20 to 1 micropascal amounts to dividing the reference by twenty — which produces only 26 decibels of difference. Thirty-five are therefore missing.9

They come from elsewhere: water resists the passage of a wave far more than air does. Acousticians call this impedance. At identical pressure, a wave carries much less energy in water than in air, and this second effect is worth about 35.5 decibels.10

What produces the gapHow much
The change of reference (20 → 1 µPa)~26 dB
The difference in impedance between water and air~35.5 dB
Total~61.5 dB

Sources for the table11

The method matters more than the numbers. An explanation that accounts for the right result is not necessarily the right explanation: here, the reference alone gave 26 instead of 61. When correct reasoning does not add up, something is missing from it.

One warning remains, from the specialists themselves.

This figure of 61.5 circulates widely, and acousticians are wary of it. They write that it is inappropriate to suggest that subtracting 61.5 decibels “converts” an underwater level to its airborne equivalent.12

The reason: the conversion settles the question of physics, not that of perception. Hearing underwater and hearing in air are not alike; and comparing what a human hears with what a seal hears raises a problem that this calculation does not solve.13

These researchers say so plainly: it is better to apply this factor than to apply none — that has led to misleading comparisons — but its existence could confer a false sense of security. One believes one has compared; one has only converted.14

4. The scale does not advance evenly

On an ordinary graduated ruler, the distance between 10 and 20 is the same as between 20 and 30. The decibel scale, by contrast, is logarithmic: each step multiplies the value instead of adding to it.

  • +10 dB = 10 times more sound energy
  • +20 dB = 100 times more sound energy
  • +30 dB = 1,000 times more sound energy15

This is why a difference that looks small on paper can be enormous in reality. Between 85 and 115 decibels, the gap is only thirty points on paper; yet the second level carries a thousand times more energy.

5. A ratio is not a unit, and it is official

This is not a subtlety of wording: it is a matter of official nomenclature.

The International System of Units — the one that defines the metre, the kilogram and the second — does not count the decibel among its units. It classes it among the non-SI units, which serve to express logarithmic quantities.16

The reason is precisely the one given in the previous sections. A unit measures a quantity that exists independently of the observer: a metre remains a metre, whether one is measuring a table or a planet. A decibel, by contrast, says nothing until one has specified relative to what.

Many everyday numbers work this way without saying so. A percentage is a ratio. A stock market index is a ratio. An earthquake magnitude is a ratio. All are read as quantities, and none of them is one.

6. So what does this number count?

Back to the opening sentence: the same noise measures 150 dB in water and 90 dB in air.

Neither of the two numbers is wrong. Neither is rounded or approximate. Both are exact, and they describe the same physical event. What changes is the measurement convention — and a convention is neither true nor false; it is chosen.

From this follows a simple rule, which applies well beyond sound:

Before comparing two numbers, you must check that they count the same thing.

Two measurements in decibels can be compared only if they share the same reference. It is the same precaution as for the thresholds that define a city, the starting years that define a change, or the boundaries that define a fish stock. The number is solid; it is the sentence written above it that decides what it means.17

Note 1

The physical phenomenon of sound is defined to be a disturbance of matter that is transmitted from its source outward. […] These compressions (high pressure regions) and rarefactions (low pressure regions) move out as longitudinal pressure waves having the same frequency as the string—they are the disturbance that is a sound wave.

Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.1 “Sound”

See the full note ↓

Note 2

The more rigid (or less compressible) the medium, the faster the speed of sound. […] For materials that have similar rigidities, sound will travel faster through the one with the lower density […]

Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.2 “Speed of Sound, Frequency, and Wavelength”

See the full note ↓

Note 3

At 0ºC, the speed of sound is 331 m/s, whereas at 20.0ºC it is 343 m/s […] Air | 331 […] Water, fresh | 1480 […] Sea water | 1540 […] Steel | 5960

Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.2 “Speed of Sound, Frequency, and Wavelength”, Table 17.1

See the full note ↓

Note 4

In this example, consider that the low E2 string has been plucked, sounding the E2 at 82.4 Hz, but also producing all harmonics of that pitch.

Nave, Carl R., “Acoustic Guitar”, HyperPhysics, Department of Physics and Astronomy, Georgia State University, section “Fret Rule for Guitars”

See the full note ↓

Note 5

Normal human hearing encompasses frequencies from 20 to 20,000 Hz, an impressive range. […] The most common form of hearing loss comes with age and is called presbycusis—literally elder ear. Such loss is increasingly severe at higher frequencies, and interferes with music appreciation and speech recognition.

Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.6 “Hearing”

See the full note ↓

Note 6

Relative units are related to specific conditions […] Decibels are a relative unit comparing two pressures; therefore, a reference pressure must also be indicated.

Discovery of Sound in the Sea, University of Rhode Island, “Underwater dB” et “Units Page for Regulators”

See the full note ↓

Note 7

In air, the common reference is 20 μPa, because that is near the absolute threshold for a normal human listener for a sound frequency of 1,000 Hz.

National Research Council, Low-Frequency Sound and Marine Mammals: Current Knowledge and Research Needs, The National Academies Press, 1994, annexe A, p. 63

See the full note ↓

Note 8

Scientists have agreed to use 1 microPascal (µPa) as the reference pressure for underwater sound.

Discovery of Sound in the Sea, University of Rhode Island, “Underwater dB” et “Units Page for Regulators”

the difference between airborne and underwater sound can be accounted for by applying a 61.5 dB comparison factor

Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR)

See the full note ↓

Note 9

To account for the fact that most acoustic measurements performed in water are referenced to 1 µPa, while those performed in air are referenced to […] 20 µPa, 26 dB is subtracted from the original levels

Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR)

See the full note ↓

Note 10

Sounds in water and sounds in air that have the same pressures have very different intensities because the impedance of water is much greater than the impedance of air. […] The difference in impedance of air and water means that sound waves with the same pressure will have intensity levels that differ by 35.5 dB.

Discovery of Sound in the Sea (DOSITS), “What is intensity?”, University of Rhode Island

See the full note ↓

Note 11

Scientists have arbitrarily agreed to use the intensity of a sound wave with a pressure of 1 microPascal (µPa) as the reference intensity for underwater sound. […] In air, however, scientists have agreed to use the intensity of a sound wave with a higher pressure of 20 microPascals as the reference intensity.

Knowlton, Chris, “Introduction to Decibels”, Discovery of Sound in the Sea, University of Rhode Island, 20 July 2018

See the full note ↓

Note 12

inappropriate to suggest that subtracting 61.5 dB from an underwater sound pressure level "converts" that level to its airborne equivalent

Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR)

See the full note ↓

Note 13

Those issues include the perception of sound and annoyance underwater, and the problematic issue of making comparisons across species. This paper does not offer solutions to those issues

Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR)

See the full note ↓

Note 14

Whilst use of such a factor is preferable to use of none (which has led to misleading comparisons between levels in-air and water) nevertheless its existence could confer a false sense of security that the comparison is sound

Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR)

See the full note ↓

Note 15

Ratios of Intensities and Corresponding Differences in Sound Intensity Levels […] I2/I1 | β2−β1 […] 10.0 | 10.0 dB […] 100.0 | 20.0 dB […] 1000.0 | 30.0 dB

Ling, Samuel J., Sanny, Jeff and Moebs, William, University Physics, vol. 1, OpenStax, 2016, § 17.3 “Sound Intensity”

See the full note ↓

Note 16

Le tableau 8 présente une liste non exhaustive d'unités en dehors du SI, regroupées en catégories indicatives pour en faciliter la lecture. […] Le néper, le bel et le décibel servent à exprimer les valeurs de grandeurs logarithmiques spécifiques.

Table 8 presents a non-exhaustive list of non-SI units, grouped into indicative categories to make it easier to read. […] The neper, the bel and the decibel are used to express the values of specific logarithmic quantities.

Bureau international des poids et mesures, Le Système international d’unités (SI), 9e éd., 2019

See the full note ↓

Note 17

To be able to compare sound levels given in dB to one another, a standard reference intensity or reference pressure must always be used.

Knowlton, Chris, “Introduction to Decibels”, Discovery of Sound in the Sea, University of Rhode Island, 20 July 2018

See the full note ↓

Notes and sources

  1. ↑

    Passage Sound travels through a succession of compressions and expansions in a medium

    The physical phenomenon of sound is defined to be a disturbance of matter that is transmitted from its source outward. […] These compressions (high pressure regions) and rarefactions (low pressure regions) move out as longitudinal pressure waves having the same frequency as the string—they are the disturbance that is a sound wave.

    Source Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.1 “Sound”, § 17.1, 2nd paragraph and paragraph beginning “A vibrating string produces a sound wave”.

    Open access open the source · checked on 27 October 2026

  2. ↑

    Passage The stiffer the medium — the harder it is to compress — the faster sound travels […] at equal stiffness, a denser medium slows sound down

    The more rigid (or less compressible) the medium, the faster the speed of sound. […] For materials that have similar rigidities, sound will travel faster through the one with the lower density […]

    Source Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.2 “Speed of Sound, Frequency, and Wavelength”, § 17.2, paragraph on the rigidity and density of the medium.

    Open access open the source · checked on 27 October 2026

  3. ↑

    Passage ~ 340 m/s […] ~ 1,500 m/s […] ~ 6,000 m/s

    At 0ºC, the speed of sound is 331 m/s, whereas at 20.0ºC it is 343 m/s […] Air | 331 […] Water, fresh | 1480 […] Sea water | 1540 […] Steel | 5960

    Source Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.2 “Speed of Sound, Frequency, and Wavelength”, Table 17.1, § 17.2, paragraph on the effect of temperature (after Equation 17.3) and Table 17.1 “Speed of Sound in Various Media”.

    Open access open the source · checked on 27 October 2026

  4. ↑

    Passage The low E string of a guitar vibrates about 82 times per second

    In this example, consider that the low E2 string has been plucked, sounding the E2 at 82.4 Hz, but also producing all harmonics of that pitch.

    Source Nave, Carl R., “Acoustic Guitar”, HyperPhysics, Department of Physics and Astronomy, Georgia State University, section “Fret Rule for Guitars”, “Acoustic Guitar” page, section “Fret Rule for Guitars”, sentence beginning “In this example”.

    Open access open the source · checked on 27 October 2026

  5. ↑

    Passage The human ear perceives roughly 20 to 20,000 hertz […] it narrows with age, especially at the top

    Normal human hearing encompasses frequencies from 20 to 20,000 Hz, an impressive range. […] The most common form of hearing loss comes with age and is called presbycusis—literally elder ear. Such loss is increasingly severe at higher frequencies, and interferes with music appreciation and speech recognition.

    Source Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.6 “Hearing”, § 17.6, 2nd paragraph and paragraph following Figure 17.35.

    Open access open the source · checked on 27 October 2026

  6. ↑

    Passage The decibel is not a unit. It is a ratio.

    Relative units are related to specific conditions […] Decibels are a relative unit comparing two pressures; therefore, a reference pressure must also be indicated.

    Source Discovery of Sound in the Sea, University of Rhode Island, “Underwater dB” et “Units Page for Regulators”, page on units.

    Open access open the source · checked on 9 September 2026

  7. ↑

    Passage In air, this reference is a fixed convention close to the faintest sound a normal human ear can perceive (20 µPa).

    In air, the common reference is 20 μPa, because that is near the absolute threshold for a normal human listener for a sound frequency of 1,000 Hz.

    Source National Research Council, Low-Frequency Sound and Marine Mammals: Current Knowledge and Research Needs, The National Academies Press, 1994, annexe A, p. 63, appendix A “Comparison of Sound-Pressure Reference Levels in Air and Water”, p. 63.

    Open access open the source · checked on 9 September 2026

  8. ↑

    Passage Underwater, acousticians use a different reference (1 µPa), twenty times smaller.

    Scientists have agreed to use 1 microPascal (µPa) as the reference pressure for underwater sound.

    Source Discovery of Sound in the Sea, University of Rhode Island, “Underwater dB” et “Units Page for Regulators”, glossary.

    Open access open the source · checked on 9 September 2026

    Passage a sound of the same physical energy is measured at about 61 decibels more in water than in air

    the difference between airborne and underwater sound can be accounted for by applying a 61.5 dB comparison factor

    Source Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR), abstract of the article.

    Paywalled open the source · checked on 9 September 2026

  9. ↑

    Passage Going from 20 to 1 micropascal […] produces only 26 decibels of difference.

    To account for the fact that most acoustic measurements performed in water are referenced to 1 µPa, while those performed in air are referenced to […] 20 µPa, 26 dB is subtracted from the original levels

    Source Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR), body of the article.

    Paywalled open the source · checked on 9 September 2026

  10. ↑

    Passage water resists the passage of a wave far more than air does. Acousticians call this impedance […] this second effect is worth about 35.5 decibels

    Sounds in water and sounds in air that have the same pressures have very different intensities because the impedance of water is much greater than the impedance of air. […] The difference in impedance of air and water means that sound waves with the same pressure will have intensity levels that differ by 35.5 dB.

    Source Discovery of Sound in the Sea (DOSITS), “What is intensity?”, University of Rhode Island, page “What is intensity?”, paragraphs comparing the characteristic impedance of water and air.

    Open access open the source · checked on 27 October 2026

  11. ↑

    Passage the standardised reference values of 20 µPa in air and 1 µPa in water

    Scientists have arbitrarily agreed to use the intensity of a sound wave with a pressure of 1 microPascal (µPa) as the reference intensity for underwater sound. […] In air, however, scientists have agreed to use the intensity of a sound wave with a higher pressure of 20 microPascals as the reference intensity.

    Source Knowlton, Chris, “Introduction to Decibels”, Discovery of Sound in the Sea, University of Rhode Island, 20 July 2018, section “What is a dB?”.

    Open access open the source · checked on 27 October 2026

  12. ↑

    Passage inappropriate to suggest that subtracting 61.5 decibels “converts” an underwater level to its airborne equivalent

    inappropriate to suggest that subtracting 61.5 dB from an underwater sound pressure level "converts" that level to its airborne equivalent

    Source Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR), body of the article.

    Paywalled open the source · checked on 9 September 2026

  13. ↑

    Passage comparing what a human hears with what a seal hears raises a problem that this calculation does not solve

    Those issues include the perception of sound and annoyance underwater, and the problematic issue of making comparisons across species. This paper does not offer solutions to those issues

    Source Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR), abstract of the article.

    Paywalled open the source · checked on 9 September 2026

  14. ↑

    Passage it is better to apply this factor than to apply none — that has led to misleading comparisons — but its existence could confer a false sense of security

    Whilst use of such a factor is preferable to use of none (which has led to misleading comparisons between levels in-air and water) nevertheless its existence could confer a false sense of security that the comparison is sound

    Source Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (copie d’auteur sur le site de l’ISVR), abstract of the article.

    Paywalled open the source · checked on 9 September 2026

  15. ↑

    Passage +10 dB = 10 times more sound energy […] +20 dB = 100 times more sound energy […] +30 dB = 1,000 times more sound energy

    Ratios of Intensities and Corresponding Differences in Sound Intensity Levels […] I2/I1 | β2−β1 […] 10.0 | 10.0 dB […] 100.0 | 20.0 dB […] 1000.0 | 30.0 dB

    Source Ling, Samuel J., Sanny, Jeff and Moebs, William, University Physics, vol. 1, OpenStax, 2016, § 17.3 “Sound Intensity”, section 17.3 (“Sound Intensity”), Table 17.3 (the text adds: “each factor of 10 in intensity corresponds to 10 dB”).

    Open access open the source · checked on 27 October 2026

  16. ↑

    Passage The International System of Units […] does not count the decibel among its units. It classes it among the non-SI units, which serve to express logarithmic quantities.

    Le tableau 8 présente une liste non exhaustive d'unités en dehors du SI, regroupées en catégories indicatives pour en faciliter la lecture. […] Le néper, le bel et le décibel servent à exprimer les valeurs de grandeurs logarithmiques spécifiques.

    Editors’ translation Table 8 presents a non-exhaustive list of non-SI units, grouped into indicative categories to make it easier to read. […] The neper, the bel and the decibel are used to express the values of specific logarithmic quantities.

    Source Bureau international des poids et mesures, Le Système international d’unités (SI), 9e éd., 2019, section 4, table 8 “Non-SI units” (p. 33) and its note (m) (p. 34).

    Open access open the source · checked on 24 October 2026

  17. ↑

    Passage Two measurements in decibels can be compared only if they share the same reference.

    To be able to compare sound levels given in dB to one another, a standard reference intensity or reference pressure must always be used.

    Source Knowlton, Chris, “Introduction to Decibels”, Discovery of Sound in the Sea, University of Rhode Island, 20 July 2018, section “What is a dB?”.

    Open access open the source · checked on 27 October 2026

Bibliography

15
  • Bureau international des poids et mesures, Le Système international d’unités (SI), 9e éd., 2019, open access (the decibel as a logarithmic ratio, accepted for use with the SI but outside it). https://www.bipm.org/fr/publications/si-brochure
  • Discovery of Sound in the Sea (DOSITS), “What is intensity?”, University of Rhode Island, open access (the impedance of water, much greater than that of air; at equal pressure, intensity levels that differ by 35.5 dB). https://dosits.org/science/advanced-topics/what-is-intensity/
  • Discovery of Sound in the Sea, University of Rhode Island, “Underwater dB” et “Units Page for Regulators”, open access (the two reference pressures, and the fact that a decibel in water is not a decibel in air). https://dosits.org/
  • Finfer, Daniel C., Leighton, Timothy G. and White, Paul R., “Issues Relating to the Use of a 61.5 dB Conversion Factor when Comparing Airborne and Underwater Anthroprogenic Noise Levels”, Applied Acoustics, vol. 69, no. 5, 2008, p. 464-471, paywalled (the breakdown of the gap into 26 dB of reference and about 35.5 dB of impedance; the warning against the idea of “conversion”; the limits relating to perception and to comparison between species). https://doi.org/10.1016/j.apacoust.2007.05.008
  • Kinsler, Lawrence E. et al., Fundamentals of Acoustics, Wiley, 2000, in libraries (the speed of sound as a function of the stiffness and density of the medium).
  • Knowlton, Chris, “Introduction to Decibels”, Discovery of Sound in the Sea, University of Rhode Island, 20 July 2018, open access (the reference values of 1 µPa in water and 20 µPa in air; two levels in decibels can be compared only with a common reference). https://dosits.org/science/advanced-topics/introduction-to-decibels
  • Ling, Samuel J., Sanny, Jeff and Moebs, William, University Physics, vol. 1, OpenStax, 2016, § 17.3 “Sound Intensity”, open access (the table of steps: +10 dB for intensity multiplied by 10, +20 dB by 100, +30 dB by 1,000). https://openstax.org/books/university-physics-volume-1/pages/17-3-sound-intensity
  • National Research Council, Low-Frequency Sound and Marine Mammals: Current Knowledge and Research Needs, The National Academies Press, 1994, annexe A, p. 63, open access (the 20 µPa reference in air, chosen because it is close to the threshold of human hearing). https://www.nationalacademies.org/read/4557/chapter/6
  • Nave, Carl R., “Acoustic Guitar”, HyperPhysics, Department of Physics and Astronomy, Georgia State University, open access (the low E2 string of a guitar, sounding at 82.4 Hz). https://hyperphysics.gsu.edu/hbase/Music/guita.html
  • Organisation internationale de normalisation, ISO 1683, Acoustique — Valeurs de référence recommandées pour les niveaux acoustiques et vibratoires, paywalled (the standardised reference values of 20 µPa in air and 1 µPa in water).
  • Rossing, Thomas D., Moore, F. Richard and Wheeler, Paul A., The Science of Sound, Addison-Wesley, 2002, in libraries (the nature of sound, the speeds in air, water and steel, the decibel scale, the limits of human hearing).
  • Urick, Robert J., Principles of Underwater Sound, McGraw-Hill, 1983, in libraries (the conventions of underwater acoustics).
  • Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.1 “Sound”, open access (sound as a disturbance of matter travelling as compressions and rarefactions). https://openstax.org/books/college-physics-2e/pages/17-1-sound
  • Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.2 “Speed of Sound, Frequency, and Wavelength”, open access (the speed of sound as a function of the stiffness and density of the medium; the table of speeds in air, water and steel). https://openstax.org/books/college-physics-2e/pages/17-2-speed-of-sound-frequency-and-wavelength
  • Urone, Paul Peter and Hinrichs, Roger, College Physics 2e, OpenStax (Rice University), 2022, section 17.6 “Hearing”, open access (the range of 20 to 20,000 Hz; presbycusis, the loss of high frequencies with age). https://openstax.org/books/college-physics-2e/pages/17-6-hearing

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