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DB(A))
The A-weighting curve is one of a family of curves
defined in IEC179 and various other standards for use in
sound level meters. Though originally intended only for the
measurement of low-level sounds (around 40-phon) it is now
commonly used for the measurement of
environmental noise and
industrial noise, when assessing potential
hearing damage and other
noise health effects at moderate to high intensity levels.
A-weighting also finds widespread use in audio equipment
measurement, though arguably it may not be the most suitable
weighting for this purpose.
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Contents
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1
Loudness measurements
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2
Environmental noise
measurement
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3
Audio reproduction and
broadcasting equipment
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4
Transfer functions of some
common weightings
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5
See also
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6
External links
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Loudness measurements
A-weighting is only really valid for relatively quiet sounds
and for pure tones as it is based on the 40-phon
Fletcher-Munson curves which represented an early
determination of the
equal-loudness contour for human hearing. The B and C curves
were intended for louder sounds (though they are less used)
while the D curve is used in assessing loud aircraft noise (IEC
537). Although the original Fletcher-Munson family of
contours have been subject to fresh experimental determinations,
notably by Robinson-Dadson, a recent survey by the ISO standards
organisation suggests that the latter may have been less
accurate than thought, and the survey comments that it is
fortunate that in the latest standard set of contours, defined
in ISO 226 (2003), the 40-phon curve comes closer to the
original Fletcher-Munson, than to the Robinson-Dadson.
Nevertheless, it will be noted that A-weighting would be a
better match to the loudness curve if it fell much more steeply
above 10 kHz, and it can be assumed that a better match was not
aimed for because steep filters were more difficult to construct
in the early days of electronics. Nowadays, no such limitation
need exist, as demonstrated by the
ITU-R 468 curve. If weightings such as these are used
without further band-limiting it is possible to obtain different
readings on different instruments if ultrasonic noise is
present. Good design therefore requires a 20 kHz low-pass filter
to be combined with the weighting curve.
Integrating
sound level meter in
dB(A)
Environmental noise measurement
A-weighted
decibels are abbreviated dB(A) or dBA. When
acoustic (calibrated microphone) measurements are being referred
to, then the units used will be
dB
SPL referenced to 20 micropascals = 0 dB SPL.
dBrn
adjusted is a synonym for dBA.
While the A-weighting curve has been widely adopted for
environmental noise measurement, and is standard in many sound
level meters, it does not really give valid results for noise
because of the way in which the human ear analyzes sound. The
A-weighting system is used commonly in
roadway noise and
aircraft noise analyses. We are considerably more sensitive
to noise in the region of 6 kHz than we are to tones of
equivalent level (see
ITU-R 468 weighting for further explanation).
A-weighting is also in common use for assessing potential
hearing damage caused by loud noise, though this seems to be
based on the widespread availability of sound level meters
incorporating A-weighting rather than on any good experimental
evidence to suggest that such use is valid. The distance of the
measuring microphone from a sound source is often "forgotten",
when SPL measurements are quoted, making the data useless. In
the case of environmental or aircraft noise distance need not be
quoted, as it is the level at the point of measurement that is
needed, but when measuring refrigerators and similar appliances
the distance should be stated; where not stated it is usually
one
metre (1 m). An extra complication here is the effect of a
reverberant room, and so noise measurement on appliances should
state "at 1 m in an
anechoic chamber". Measurements made outdoors will
approximate well to anechoic conditions.
A-weighted SPL measurements of noise level are increasingly
to be found on sales literature for domestic appliances such as
refrigerators and freezers, and computer fans. Although the
threshold of hearing is typically around 0 dB SPL, this is in
fact very quiet indeed, and appliances are more likely to have
noise levels of 30 to 40 dB SPL.
Audio reproduction and broadcasting
equipment
Human sensitivity to noise in the region of 6 kHz became
particularly apparent in the late 1960's with the introduction
of
compact cassette recorders and
Dolby-B noise reduction. A-weighted noise measurements were
found to give misleading results because they did not give
sufficient prominence to the 6 kHz region where the noise
reduction was having greatest effect, and sometimes one piece of
equipment would even measure worse than another and yet sound
better, because of differing spectral content.
ITU-R 468 noise weighting was therefore developed to more
accurately reflect the subjective loudness of all types of
noise, as opposed to tones. This curve, which came out of work
done by the
BBC
Research Department, and was standardised by the
CCIR
and later adopted by many other standards bodies (IEC,
BSI)
and,
as of 2006, is maintained by the ITU. It was widely used in
Europe, especially in broadcasting, especially when it was
adopted by
Dolby Laboratories who realised its superior validity for
their purposes. Its advantages over A-weighting seem to be less
well understood in the US, where the use of A-weighting
predominates. It is universally used by broadcasters in Britain,
Europe, and former countries of the British Empire such as
Australia and South Africa.
Though the noise level of 16-bit audio systems (such as CD
players) is commonly quoted (on the basis of calculations that
take no account of subjective effect) as −98
dBFS
(relative to
full scale), the best 468-weighted results are in the region
of −68 dB relative to alignment level (commonly defined as 18 dB
below FS), or −86 dBFS.[citation
needed]
The use of weighting curves can be regarded as "cheating"
when used to hide less-than-ideal performance in the regions
outside the weighted band, and since weighted measurements are
better than the unweighted measurements used by competitors.
(The weighting method used should therefore always be
specified along with a measurement.) They are more correct from
a psychoacoustic perspective, however, provided that the proper
curve is used.
For instance,
noise shaping achieves the same distortion benefits as
dither noise, but moves the noise to inaudible high
frequencies. This would measure differently in weighted and
unweighted tests. In this case, the extra noise is both harmless
(beneficial, actually) and inaudible, and a weighted measurement
would be appropriate.
Transfer functions of some common
weightings
The human ear varies in sensitivity in a complex way
that depends on frequency and level.
The gain curves are defined by the following s-domain
transfer functions
[1]:
A
-
kA ≈ 7.39705×109
B
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kB ≈ 5.99185×109
C
-
kC ≈ 5.91797×109
D
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kD ≈ 91104.32
The k values are constants which are used to normalize
the function to a gain of 1 (0 dB). The values listed above
normalize the functions to 0 dB at 1 kHz, as they are typically
used. (This normalization is shown in the image.)
See also
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Noise
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Signal noise
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Sound level meter
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ITU-R 468 noise weighting
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Audio quality measurement
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Noise measurement
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Noise pollution
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Noise regulation
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Headroom
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Rumble measurement
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Weighting filter
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Equal-loudness contour
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Fletcher-Munson curves
External links
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Noise measurement briefing
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Calculator for A,C,U, and AU weighting values
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A-weighting filter circuit for audio measurements
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Weighting Filter Set Circuit diagrams
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Rane pro audio reference definition of "weighting filters"
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Frequency Weighting Equations
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A-weighting in detail
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A-Weighting Equation and online calculation
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Noise