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Sound Intensity Decibel Calculator

Physics
L = 20·log₁₀(p/p₀), p₀ = 20 µPa

10 · log₁₀

Power-like: intensity, acoustic power, dBm. A factor of ten in the quantity is 10 dB.

10·log₁₀(p²/p₀²)
= 20·log₁₀(p/p₀)

20 · log₁₀

Active

Amplitude-like: pressure, voltage, dBu, dBV. Intensity goes as pressure squared, so the 20 falls out of the 10.

Amplitude-like — pressure, voltage, dBu, dBV

Inputs

RMS, not peak. Divide a peak reading by √2 first.

Air, weighting and exposure

Feeds the speed of sound and the impedance bridge.
Feeds air density.
10 Hz – 20 kHz for the weighting curves.
0–24 h, for the dose percentage.
0–10.
Sound level
93.98 dB SPL (re 20 µPa)

20·log₁₀ — pressure is amplitude-like. The 20 is not a different convention: intensity goes as p², and 10·log₁₀(p²/p₀²) = 20·log₁₀(p/p₀).

Linear quantity
1.00 Pa
Ratio to reference
50000.00 ×
A-weighted level
77.79 dBA
Weighting offset
-16.19 dB

Sounds like: Extremely loud (motorcycle, power tools)

Comparable sound: Motorcycle (95 dB)

Perceived loudness ≈ 1.86 × the 85.00 dB baseline — a psychoacoustic rule of thumb (2^(ΔL/10)), not a physical measurement.

0 Threshold of hearing20 Rustling leaves30 Quiet room40 Whisper45 Library60 Normal conversation75 Vacuum cleaner85 Heavy traffic90 Lawnmower95 Motorcycle100 Power tools110 Concert / nightclub120 Siren at 30 m140 Jet engine at 30 m93.98 dB
What the other multiplier would have given
This is a amplitude-like quantity, so it takes 20·log₁₀ and the answer is 93.98 dB. Using the other multiplier would return 46.99 dB — exactly half. Picking the wrong one makes every decibel answer wrong by a factor of two.
The multiplier and the quantity type disagree
A amplitude-like quantity takes 20·log₁₀, which gives 93.9794 dB. The other multiplier gives 46.9897 dB — exactly half. Every decibel answer is wrong by a factor of two when this is chosen wrongly.
dBA is a convention, not the sound field
A-weighting is a perceptual convention, not a measurement of the sound field. It deliberately discards real acoustic energy at low frequency because the ear is comparatively deaf there. Never mix a dBA figure and a dB SPL figure in one arithmetic step.

Indicative permissible daily exposure

NIOSH REL — 85 dBA, 3 dB exchange
over 24 h (no practical limit at this level)
OSHA PEL — 90 dBA, 5 dB exchange
over 24 h (no practical limit at this level)
Noise dose
9.45 %
Regulatory guidance, not a safety verdict
Exposure limits are indicative regulatory guidance, not a personal risk assessment. NIOSH and OSHA differ by a factor of eight in permitted time at 100 dBA. Consult a qualified occupational-health professional and your own jurisdiction's regulations.

Frequency weighting

A — ear-like, the occupational-noise standard

0-10-20-30-40-50101001k10kSolid: A-weighting, dashed: C-weighting (dB offset vs frequency, Hz)
Octave bandA offsetC offset
31.5 Hz-39.5 dB-3.0 dB
63 Hz-26.2 dB-0.8 dB
125 Hz-16.2 dB-0.2 dB
250 Hz-8.7 dB-0.0 dB
500 Hz-3.2 dB0.0 dB
1 kHz0.0 dB-0.0 dB
2 kHz1.2 dB-0.2 dB
4 kHz1.0 dB-0.8 dB
8 kHz-1.1 dB-3.0 dB
16 kHz-6.7 dB-8.6 dB
A-weighting is a convention, not physics
A-weighting is a perceptual convention, not a measurement of the sound field. It deliberately discards real acoustic energy at low frequency because the ear is comparatively deaf there. Never mix a dBA figure and a dB SPL figure in one arithmetic step.

Step by step

Every figure below is carried at full double precision; rounding happens only where it is displayed.

Formula

L = 20 · log₁₀(p / p₀)

Substitute

L = 20 · log₁₀(1.000000 / 2e-5)

Ratio

p / p₀ = 50000.00 ×

Logarithm

log₁₀(50000.00) = 4.6989700

Result

L = 93.9794 dB SPL

Air used for the impedance bridge

Speed of sound c
343.21 m/s
Air density ρ
1.20 kg/m³
Impedance z₀ = ρc
413.27 Pa·s/m
Sound power level vs sound pressure level
Sound power level is a property of the source alone and does not change with distance; sound pressure level is a property of a point in space. Machinery datasheets quote sound power level; meters read sound pressure level.

The three references

A decibel is a ratio against a stated reference, so the reference is part of the number. Note that I₀ and W₀ share the digits 10⁻¹² but carry different units — a quiet source of errors.

SymbolValueApplies toMultiplier
I₀1 × 10⁻¹² W/m² (1 pW/m²)Sound intensity level10·log₁₀
p₀2 × 10⁻⁵ Pa (20 µPa)Sound pressure level (SPL)20·log₁₀
W₀1 × 10⁻¹² W (1 pW)Sound power level10·log₁₀

The largest sinusoidal wave one atmosphere can carry is 194.09 dB SPL. Beyond it the rarefaction half-cycle would need negative absolute pressure, so the wave becomes a shock and linear acoustics stops applying.

About This Tool

Sound Intensity Decibel Calculator – Intensity, Pressure, Power and the dB Scale

Human hearing spans about twelve orders of magnitude in intensity, from roughly 10−¹² W/m² at the threshold of hearing to around 10 W/m² at the threshold of pain. The decibelcompresses that span into a comfortable 0–130 range, and that compression is exactly what makes it so easy to misuse. This sound intensity decibel calculator converts between intensity, sound pressure, sound power and their levels, combines noise sources, propagates a level over distance, and reports A-weighted levels with indicative exposure guidance.

A decibel is a ratio, never a unit

The most important fact about the decibel is that it is not a unit at all — it is a logarithmic ratio against a stated reference. A bare “85 dB” is incomplete in the same way “85 per cent” is. dB SPL, dBA, dBu, dBV, dBm and dBFS are different scales and none of their numbers are interchangeable, so the calculator prints the reference inline with every figure.

The 10 versus 20 trap

Decibels use two different formulas depending on whether the quantity is power-like or amplitude-like, and picking the wrong one makes every answer wrong by exactly a factor of two in dB.

  • Power-likequantities — intensity, acoustic power, energy flux, dBm — take L = 10 · log₁₀(X / X₀).
  • Amplitude-likequantities — pressure, voltage, particle velocity, dBu, dBV — take L = 20 · log₁₀(X / X₀).

The 20 is not a rival convention. It falls straight out of the 10, because intensity goes as pressure squared: 10·log₁₀(p²/p₀²) = 20·log₁₀(p/p₀). One rule, applied to a squared quantity. At p = 2 Pa the correct sound pressure level is 100.00 dB; applying 10·log₁₀ by mistake returns 50.00 dB, precisely half.

Why the reference pressure is 20 µPa

The two references — I₀ = 1 pW/m² and p₀ = 20 µPa— look arbitrary but are not. Substituting them into the plane-wave relation I = p²/(ρc) requires a characteristic impedance of exactly 400 Pa·s/m, very nearly that of air: the pair was engineered so that sound pressure level and sound intensity level give the same number. Real air at 20 °C has ρc ≈ 413.3 Pa·s/m, so the two scales differ by about 0.14 dB— and the calculator shows exactly how much licence the usual interchange takes.

I₀ and W₀ share digits but not units
The reference intensity is 1 × 10−¹² W/m² and the reference sound power is 1 × 10−¹² W. Identical digits, different units, and mixing them is a silent and common error.

Why two 85 dB sources are not 170 dB

Levels do not add arithmetically. To combine incoherent noise sources you convert each back to a linear power-like quantity, sum them, and convert back: L_total = 10 · log₁₀(Σ 10^(Lᵢ/10)). Two identical 85 dB machines give 88.01 dB, because doubling the acoustic power always adds 10·log₁₀(2) = 3.01 dB whatever the starting level.

The practical lesson is that the loudest source dominates. Combining 85, 90 and 82 dB gives 91.69 dB, of which the 90 dB source supplies about 68 per cent of the linear intensity while the 82 dB source contributes just 0.49 dB. Silencing the quietest machine is nearly pointless; halving the loudest buys 3.01 dB.

Distance, and the 6 dB rule

For a point source radiating into a free field, intensity falls as 1/r², so L₂ = L₁ − 20·log₁₀(r₂/r₁). A level of 95 dB at 1 m becomes 76.94 dB at 8 m: three doublings, each costing 20·log₁₀(2) = 6.02 dB. Write 6.02, not 6, in any computed output.

Inverse-square is a free-field idealisation
A line source such as a highway spreads cylindrically and loses only 3.01 dB per doubling. Inside a room the level flattens out entirely beyond the critical distance. Closer than about one wavelength you are in the near field, where no simple 1/r law holds. Ground reflections add up to 3 dB and air absorption removes extra high-frequency energy over long ranges.

Weighted levels and exposure

A-weighting is a perceptual convention, not a measurement of the sound field. It deliberately discards real acoustic energy at low frequencies because the ear is comparatively deaf there: a 90 dB SPL rumble at 125 Hz reads about 73.9 dBA, and the 16 dB of energy did not go anywhere. It is 0 dB at 1 kHz by construction. Because occupational limits are written in dBA, the calculator shows weighted and unweighted levels side by side and never mixes them in one arithmetic step.

Exposure guidance is indicative regulatory information, not a personal risk assessment. The NIOSH REL uses an 85 dBA criterion with a 3 dB exchange rate; the OSHA PELuses 90 dBA with a 5 dB exchange rate. At 100 dBA those give 15 minutes and 2 hours — a factor of eight apart, which is why any quoted duration must name the standard behind it.

Sound power level is not sound pressure level

After the 10-versus-20 trap, the most common decibel error is confusing these two. Sound power level (L_W) is a property of the source alone and does not change with distance; sound pressure level is a property of a point in space. Datasheets quote L_W; meters read SPL. A machine radiating 0.1 W has L_W = 110.00 dB everywhere, yet produces 89.47 dB at 3 m in a free field.

Frequently Asked Questions

Is the Sound Intensity Decibel Calculator free?

Yes, Sound Intensity Decibel Calculator is totally free :)

Can I use the Sound Intensity Decibel Calculator offline?

Yes, you can install the webapp as PWA.

Is it safe to use Sound Intensity Decibel Calculator?

Yes, any data related to Sound Intensity Decibel Calculator only stored in your browser (if storage required). You can simply clear browser cache to clear all the stored data. We do not store any data on server.

How does this sound intensity and decibel calculator work?

Pick one of eight modes — intensity ⇄ decibels, pressure ⇄ decibels, combining sources, distance attenuation, the intensity/pressure bridge, or sound power at a distance — and enter the quantities in whatever units suit you. Everything is converted to SI, evaluated at full double precision, and rounded only when it is drawn on screen, so no answer is ever built from a rounded intermediate. Each result carries its reference inline, a step-by-step derivation, and the caveats that bound it.

Why is it sometimes 10·log₁₀ and sometimes 20·log₁₀?

Because the two forms are one rule applied to quantities that differ by a square. Power-like quantities — intensity, acoustic power, dBm — take L = 10·log₁₀(X/X₀). Amplitude-like quantities — pressure, voltage, dBu, dBV — take 20·log₁₀, and that 20 falls straight out of the 10 because intensity goes as pressure squared: 10·log₁₀(p²/p₀²) = 20·log₁₀(p/p₀). Choosing the wrong one makes every answer wrong by exactly a factor of two in dB. At 2 Pa the correct SPL is 100.00 dB; applying 10·log₁₀ by mistake returns 50.00 dB.

Why is the reference pressure 20 µPa rather than a round number?

It was engineered so the pressure and intensity scales read the same number. Substituting the reference pair into the plane-wave relation I = p²/(ρc) gives p₀²/I₀ = (2×10⁻⁵)²/10⁻¹² = 400 Pa·s/m, which is very nearly the characteristic impedance of air. Real air at 20 °C and 101.325 kPa has ρc = 413.27 Pa·s/m, so the two scales actually differ by 10·log₁₀(400/413.27) = −0.14 dB — small enough that acoustics quotes them interchangeably, and this calculator shows exactly how much licence that takes.

Why don't two 85 dB sources add up to 170 dB?

Because decibels are logarithms, and logarithms do not add arithmetically. You convert each level back to a linear power-like quantity, sum those, and convert back: L = 10·log₁₀(Σ 10^(Lᵢ/10)). Two identical 85 dB sources give 88.01 dB, not 170 — doubling the acoustic power always adds 10·log₁₀(2) = 3.01 dB whatever the starting level. It also means the loudest source dominates: combining 85, 90 and 82 dB gives 91.69 dB, of which the 82 dB source contributes just 0.49 dB.

Does the level really drop 6 dB every time I double the distance?

It drops 6.02 dB per doubling, and only for a point source radiating into a free field, where L₂ = L₁ − 20·log₁₀(r₂/r₁). A line source such as a highway spreads cylindrically and loses only 3.01 dB per doubling. Inside a room the level flattens out entirely beyond the critical distance, ground reflections can add up to 3 dB, and closer than about one wavelength you are in the near field where no simple 1/r law holds. Outdoor measurements over distance routinely land several dB from the free-field prediction.

Is a dBA reading the same as the physical sound level?

No, and the difference is deliberate. A-weighting is a perceptual convention that discards real acoustic energy at low frequencies because human hearing is comparatively insensitive there. A 90 dB SPL rumble at 125 Hz reads about 73.9 dBA — the 16 dB of energy did not go anywhere. A-weighting is 0 dB at 1 kHz by construction. Occupational limits are written in dBA, so the calculator reports both side by side and never mixes a weighted and an unweighted figure in one arithmetic step.