This part of IS0 9613 specifies an engineering method for calculating the attenuation of sound during propagation outdoors in order to predict the levels of environmental noise at a distance from a variety of sources. The method predicts the equivalent continuous A-weighted sound pressure level (as described in
parts 1 to 3 of IS0 1996) under meteorological conditions favourable to propagation from sources of known sound emission.
These conditions are for downwind propagation, as specified in 5.4.3.3 of IS0 1996-21987 or, equivalently,
propagation under a well-developed moderate groundbased temperature inversion, such as commonly occurs
at night. Inversion conditions over water surfaces are not covered and may result in higher sound pressure
levels than predicted from this part of IS0 9613.
The method also predicts a long-term average A-weighted sound pressure level as specified in IS0 1996-1 and IS0 1996-2. The long-term average A-weighted sound pressure level encompasses levels for a wide variety of meteorological conditions.
The method specified in this part of IS0 9613 consists specifically of octave-band algorithms (with nominal midband frequencies from 63 Hz to 8 kHz) for calculating the attenuation of sound which originates from a point sound source, or an assembly of point sources. The source (or sources) may be moving or stationary. Specific terms are provided in the algorithms for the following physical effects:
- geometrical divergence;
- atmospheric absorption;
- ground effect;
- reflection from surfaces;
- screening by obstacles.
Additional information concerning propagation through housing, foliage and industrial sites is given in annex A.
This method is applicable in practice to a great variety of noise sources and environments. It is applicable, directly or indirectly, to most situations concerning road or rail traffic, industrial noise sources, construction
activities, and many other ground-based noise sources. It does not apply to sound from aircraft in flight, or to blast waves from mining, military or similar operations.
To apply the method of this part of IS0 9613, several parameters need to be known with respect to the geometry
of the source and of the environment, the ground surface characteristics, and the source strength in terms of octave-band sound power levels
for directions relevant to the propagation.
NOTE 1 If only A-weighted sound power levels of the sources are known, the attenuation terms for 500 Hz may be used to estimate the resulting attenuation.
The accuracy of the method and the limitations to its use in practice are described in clause 9.
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