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Analysis and Ranking of the Acoustic Disturbance Potential of ...

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Report No. 6945<br />

BBN Systems <strong>and</strong> Technologies Corporation<br />

3. NOISE SOURCE CHARACTERISTICS AND TYPES<br />

This section contains a discussion <strong>of</strong> <strong>the</strong> various sources <strong>of</strong> sound in <strong>the</strong><br />

Alaskan coastal environment. Procedures for describing <strong>the</strong> properties <strong>of</strong><br />

sound are presented. Representative examples are given which show <strong>the</strong><br />

characteristics <strong>of</strong> ambient noise <strong>and</strong> man-made sound sources.<br />

3.1 Noise Source Descriptors<br />

Noise has been described as unwanted sound. This subjective definition<br />

is appropriate since sound that may be disturbing to some listeners may contain<br />

useful information for o<strong>the</strong>rs - a rock music concert being one example.<br />

The procedures outlined here for describing sound energy are <strong>the</strong>refore<br />

intended to provide physical measures which can be used to classify sound<br />

sources without requiring consideration <strong>of</strong> <strong>the</strong>ir potential effects on<br />

listeners. The issues <strong>of</strong> annoyance <strong>and</strong> disturbance are addressed separately<br />

in Section 5. Two major categories <strong>of</strong> descriptive parameters are considered -<br />

sound level spectra <strong>and</strong> temporal statistics.<br />

3.1.1 Sound level spectra<br />

The mammalian heacing process is capable <strong>of</strong> working over a very wide<br />

range <strong>of</strong> sound intensities <strong>and</strong> frequencies. Studies <strong>of</strong> <strong>the</strong> hearing processes<br />

<strong>of</strong> humans <strong>and</strong> <strong>of</strong> a limited number <strong>of</strong> o<strong>the</strong>r species, including some marine<br />

mammals, have showrthat this wide range capability is obtained by having a<br />

logarithmic hearing sensitivity characteristic; i.e., <strong>the</strong> sensation <strong>of</strong><br />

loudness has been found to increase as <strong>the</strong> logarithm <strong>of</strong> <strong>the</strong> sound pressure.<br />

Also, humans <strong>and</strong> several o<strong>the</strong>r species have a proportional b<strong>and</strong>width hearing<br />

selectivity; i.e., <strong>the</strong> selectivity <strong>of</strong> <strong>the</strong> hearing process becomes broader in<br />

<strong>the</strong> high frequency portion <strong>of</strong> <strong>the</strong> hearing range.<br />

The logarithmic hearing sensitivity characteristic has resulted in <strong>the</strong><br />

decibel scale <strong>of</strong> measuring sound intensity with a reference level (for<br />

airborne sound) set at <strong>the</strong> average threshold <strong>of</strong> (young) human hearing. Since<br />

sound intensity is proportional to <strong>the</strong> sound pressure squared, this results in<br />

<strong>the</strong> following definition <strong>of</strong> sound pressure level:<br />

SPL = 10<br />

dB<br />

or<br />

SPL = 20 L0g(P/Pref)<br />

dB<br />

where, for airborne sounds,<br />

'ref<br />

= 20 pPascal (20 pNewton/meter 2<br />

) <strong>and</strong><br />

Log = LoglO<br />

For underwater sound 1 pPa is used as <strong>the</strong> reference pressure to obtain a more<br />

convenient physical scale. Underwater sound levels using this reference will<br />

be specified using Lr or Ls ra<strong>the</strong>r than SPL to avoid confusion.

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