NOISE 773
where I sound intensity (W/m^2 ), where sound pressure
and particle velocity are in-phase, W sound power of the
source (W) and r distance from the source (m). The above
equation is called the inverse square law.
Scalar sound intensity level is given by
LIIr10 lg[]⁄Ief (7.2)
where L I scalar sound intensity level and I ref 10 ^12 W/m^2.
For airborne sound under typical conditions, sound pres-
sure level and scalar sound intensity level are approximately
equal, from which
LLpI ^10 lgW^20 lgr^109 (7.3)
for the spherical wave where L p and L I are expressed in dB. If
sound power has been A-weighted, L p and L I are in dBA.
When the inverse-square law applies, then sound levels
decrease with distance at the rate: 20 lg r. Thus, if sound
level is known at one location, it may be estimated at another
location. Table 4 and Figure 3 show the distance adjustment
to be added to sound level at distance r 1 from the source to
obtain the sound level at distance r 2.
MEASUREMENT AND INSTRUMENTATION
Sound level meters. The sound level meter is the basic tool
for making noise surveys. A typical sound level meter is a
hand-held battery-powered instrument consisting of a micro-
phone, amplifiers, weighting networks, a rootmean-square
rectifier, and a digital or analog sound level display. The A-
weighting network is most commonly used. This network
electronically adjusts the signal in accordance with Table 1,
so that sound level is displayed in dBA. When measuring out-
of-doors, a windscreen is used to reduce measurement error
due to wind impinging on the microphone. Integrating sound
level meters automatically calculate equivalent sound level. If
a standard sound level meter is used, equivalent sound level
may be calculated from representative measurements, using
the procedure described later.
Frequency analysis. The cause of a noise problem may
sometimes be detected by analyzing noise in frequency
bands. An octave band is a frequency range for which the
upper frequency limit is (approximately) twice the lower
TABLE 4
Spherical wave attenuation
r2/r1 ADJ
0.5 6.0
0.6 4.4
0.7 3.1
0.8 1.9
0.9 0.9
1.0 0.0
1.1 0.8
1.2 1.6
1.3 2.3
1.4 2.9
1.5 3.5
1.6 4.1
1.7 4.6
1.8 5.1
1.9 5.6
2.0 6.0
2.1 6.4
2.2 6.8
2.3 7.2
2.4 7.6
2.5 8.0
2.6 8.3
2.7 8.6
2.8 8.9
2.9 9.2
3.0 9.5
Distance adjustment based
on the inverse-square law.
L(r2) L(r1) ADJ.
Distance ratio r2/r1
Add to sound level at r1
10
5
0
–5
–10
0.5 1.0 1.5 2.0 2.5 3.0
FIGURE 3 Distance adjustment based on the inverse-square law.
Number of equal contributions
Add to level due to one source
10
8
6
4
2
0
1 2 345678910
FIGURE 2 Combining n equal contributions.
C014_003_r03.indd 773C014_003_r03.indd 773 11/18/2005 10:46:09 AM11/18/2005 10:46:09 AM