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| The reference sound pressure p0 = 20 µPa = 2 × 10-5 Pa is equal to the sound pressure level Lp = 0 dB as auditory threshold. |
Readings of a pure 1 kHz tone should be identical, whether weighted or not.
| Enter a value in the left or right box, then press the TAB bar or make a mouse click at an empty space at the side, to get the solution. The calculator works in both directions of the ↔ sign. |
There is also the reference power P0 = 1 milliwatt = 0,001 watt ≡ 0 dBm.
| Sound Field Quantities
Sound pressure, sound or particle velocity, particle displacement or particle ampliude, (voltage, current, electric resistance). Inverse Distance Law 1/r |
Sound Energy Quantities Sound intensity, sound energy density, sound energy, acoustic power. (electrical power). Inverse Square Law 1/r² |
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Since sound measuring instruments (meters) respond to sound pressure the "decibel" is generally associated with sound pressure level. Sound pressure levels quantify in decibels the strength (not intensity!) of given sound sources. Sound pressure levels vary substantially with distance from source, and also diminish as a result of intervening obstacles and barriers, air absorption, wind and other factors. Sound Pressure Level (SPL): 20×log (p/p0) = 10×log (p/p0)2, where p0 = 2×10−5 N/m2. p = root mean square sound pressure (N/m2 = Pa). The usual reference level p0 is 20×10−6 Pa. Note that the noise from motors is documented in sound power (acoustic power) level. "Threshold of audibility'' or the minimum pressure fluctuation detected by the ear is less than 10−9 of atmospheric pressure or about 2×10−5 Pa(pascal) at 2000 Hz. "Threshold of pain'' corresponds to a pressure 106 times greater, but still less than 1/1000 of atmospheric pressure. The standard airpressure is 101325 Pa = 101.325 kPa or 1013.25 hectopascal. Because of the wide range, sound pressure measurements are made on a logarithmic decibel scale. Sound power levels are connected to the sound source and are independent of distance. Sound powers are indicated in decibel. Lw = 10×log (P / P0) where: P0 = reference power (W). The usual reference level is P0 = 10−12 W, calculated from p0 = 20 micropascals, which is the lowest sound persons of excellent hearing can discern. Sound power is measured as the total sound power emitted by a source in all directions in watts (joules / second). Sound power levels do not vary with distance from source. |
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Questions: 1. How many decibels is the sound pressure p = 1 Pa? 2. How many decibels is the acoustic intensity I = 1 W/m2? 3. How many decibels is the acoustic power P = 1 W? 4. How many decibels is the particle velocity v = 1 m/s? 5. How many decibels is the sound energy W = 1 J? 6. How many decibels is the sound energy density E = 1 J/m3? The calculators above can help to give the answers. |
| Note: The radiated sound power (sound intensity) is the cause - and the sound pressure is the effect. The effect is of particular interest to the sound engineer. The effect of temperature and the sound power. |
| Acousticians and sound protectors (noise fighters) need the sound intensity (acoustic intensity). As a sound designer you don't need that; look out more for the sound pressure at your ears and at the microphones. |
Sound pressure and sound power
| Table of Sound Levels, Sound Pressure, and Sound Intensity Conversion of Sound Units (Levels) Damping of Sound Level with Distance |
Frequently used false statements in the context of
sound values and the distance of the sound source
| Wrong expression | Correct version |
| Sound pressure falls inversely proportional to the square of the distance 1/r2 from the sound source. wrong |
Sound pressure falls inversely proportional to the distance 1/r from the sound source. That is the 1/r law or distance law. |
| Sound pressure level decreases as the distance increases per doubling of distance from the source by (−)3 dB. wrong |
Sound pressure level decreases by (−)6 dB per doubling of distance from the source to 1/2 (50 %) of the sound pressure initial value. |
| Sound intensity (energy) falls inversely proportional to the distance 1/r from the sound source. wrong |
Sound intensity (energy) falls inversely proportional to the square of the distance 1/r2 from the sound source. |
| Sound intensity level decreases inversely as the square of the distance increases per doubling of sound source with (−)3 dB per doubling. wrong |
Sound intensity level decreases by (−)6 dB per doubling of distance from the source to 1/4 (25 %) of the sound intensity initial value. |
| Neither the sound power nor the sound power level decreases in doubling the distance. Why is this so? The psychoacoustic subjective sensations of loudness do not belong to those predictable and measurable sound quantities; see: Correlation between volume level in phone and loudness in sone People feel and judge sound events after: - exposure duration - spectral composition - temporal structure - sound level - information content - subjective mental attitude |
| "Sound level" is the sound pressure level in decibel (SPL), or sometimes the sound intensity level in dB (SIL). The reference sound pressure is p0 = 20 µPa = 2 × 10−5 Pa − the reference sound intensity is I = 10−12 W/m2.
Notice, that the calculation I ≈ p2 is effective for progressive plane waves. It can be seen that "sound intensity" (acoustic intensity) may never be equated with "sound pressure". The sound pressure is thealternating sound pressure as RMS value. The sound pressure amplitude is the peak value of the sound pressure. The sound volume is determined by the sound pressure p and expressed as sound pressure level Lp in dB.
Note: The sound intensity is a sound energy quantity. Membranes (diaphragms) of microphones and our eardrums are moved by alternating sound pressure, that is a sound field quantity. |
Sound Level Comparison Chart and the Factor
| Table of sound level dependence and the change of the respective factor to subjective volume (loudness), objective sound pressure (voltage), and sound intensity (acoustic power) How many decibels (dB) level change is double, half, or four times as loud? How many dB to appear twice as loud (twofold)? Here are all the different factors. Factor means "how many times" or "how much" ... Doubling of loudness. |
| Level Change |
Volume Loudness |
Voltage Sound pressure |
Acoustic Power Sound Intensity |
| +40 dB | 16 | 100 | 10000 |
| +30 dB | 8 | 31.6 | 1000 |
| +20 dB | 4 | 10 | 100 |
| +10 dB | 2.0 = double | 3.16 = √10 | 10 |
| +6 dB | 1.52 fold | 2.0 = double | 4.0 |
| +3 dB | 1.23 fold | 1.414 fold = √2 | 2.0 = double |
| - - - - ±0 dB - - - - | - - - - 1.0 - - - - - - - | - - - - 1.0 - - - - - - - | - - - - - 1.0 - - - - - |
| −3 dB | 0.816 fold | 0.707 fold | 0.5 = half |
| −6 dB | 0.660 fold | 0.5 = half | 0.25 |
| −10 dB | 0.5 = half | 0.316 | 0.01 |
| −20 dB | 0.25 | 0.100 | 0.01 |
| −30 dB | 0.125 | 0.0316 | 0.001 |
| −40 dB | 0.0625 | 0.0100 | 0.0001 |
| Log. quantity | Psycho quantity | Field quantity | Energy quantity |
| dB change | Loudness multipl. | Amplitude multiplier | Power multiplier |
| For a 10 dB increase of the sound level we require ten times more power from the amplifier. This increase of the sound level means for the sound pressure a lifting of the factor 3.16. Loudness and volume are highly subjective. That belongs to the domain of psychoacoustics. |
The standard atmosphere is 101325 Pa = 101.325 kPa or 1013.25 hectopascal.
Audio voltage and level
| Enter a value in the left or right box, then press the TAB bar or make a mouse click at an empty space at the side, to get the solution. The calculator works in both directions of the ↔ sign. |
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