The
sound levels to which most mammals are sensitive extend over
many orders of magnitude and, for this reason, it is convenient
to use a logarithmic scale when measuring sound. Both Sound
Pressure Level (SPL) and Sound
Intensity Level (SIL) are measured
in decibels (dB) and are usually expressed as ratios of a
measured and a reference level:
Sound
Pressure Level (dB) = 20 log (p/pref)
where pref is the
reference pressure
Sound
Intensity Level (dB) = 10 log (I/Iref)
where Iref is the
reference intensity
In
other words, the decibel is 10 times the log of the ratio
of two intensities, and 20 times the log of the ratio of two
pressures. The units for both SPL and SIL are dB relative
to the reference intensity (often abbreviated as dB re 1µPa
or dB//1µPa). Whenever "level" is added to the terms
sound intensity or sound pressure, it usually implies that
the measurement is in decibels. Because decibel implies a
ratio of two values (and therefore a dimensionless
measurement), SPL and SIL are equivalent when measured in
decibels.
Because
the dB scale is relative, reference levels must be
included with dB values if they are to be meaningful. The
reference levels for SPL and SIL are equivalent but are reported
in different units. The commonly used reference
pressure level in underwater acoustics is 1 µPa while
the reference
level in air
is 20 µPa (which is roughly the human hearing threshold
at 1000 Hz). The reference intensity in water
is
Iref
= p² ref / (rwater
cwater)
= 6.7 x 10-19 W/m2
where
reference pressure in water (pref)
is 1µPa rms,
and
the density of water (rwater)
is about 1000 kg/m3,
and
the speed of sound in water (cwater)
is about 1500 m/s.
Historically,
the reference intensity in air was the sound
intensity barely audible to humans,
1
E -12watts/m2
or 1 pW/m2. (A painful airborne sound to
humans is about 10 watts/m2).
When
quoting source levels, the
distance from the source for that reference level must also
be cited in
addition to the reference level. Typically the units of SIL
are dB relative to the reference intensity at 1 meter (e.g.,
20 dB re 1µPa @ 1m) - i.e. how intense the sound would be
were it measured 1 m from the source. In practice, one can
rarely measure source level at the standard 1 m reference,
so that source levels are usually estimated by measuring SPL
at some known range from the source (assumed to be a single
point), and the attenuation effects predicted and subtracted
from the measured value to estimate the level at the reference
range of 1 m.
Ideally,
it is Sound Intensity Levels that wed like to measure.
However, its easier to measure sound pressure than sound
intensity, so we measure pressure, and from that infer intensity.
Within the same medium, sound intensity or power is proportional
to the average of the squared pressure:
I
µ p2
therefore
SIL(dB)
= 10 log (I/Ir) = 10 log (p2 / p2
) = 20 log (p/1µPa) in water
or
= 20 log (p/20uPa) in air
In
other words, once we start using the decibel scale, SIL and
SPL are pretty much the same thing.