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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 />

reaches <strong>the</strong> cruising altitude. This is usually not true for smaller aircraft<br />

<strong>and</strong> helicopters which generally fly at lower altitudes. Thus <strong>the</strong> effective<br />

area <strong>of</strong> significant sound level near an airport is determined largely by <strong>the</strong><br />

type <strong>of</strong> aircraft used. The model described in Section 4.3 was used as a guide<br />

in estimating <strong>the</strong> effective areas to be considered for aircraft sources. For<br />

aircraft travelling at low altitude <strong>the</strong> procedure used for moving sources is<br />

applied .<br />

If a source is moving so as to change its average location within a<br />

period <strong>of</strong> two hours, <strong>the</strong> effective speed <strong>of</strong> advance must be considered since<br />

<strong>the</strong> value <strong>of</strong> Pe is increa ed. This occurs because <strong>the</strong> source has effectively<br />

occupied more than a 1 km 5 area in <strong>the</strong> two hour period, which is equivalent to<br />

ha ing more than 1 source. It can be shown that <strong>the</strong> number <strong>of</strong> independent 1<br />

km<br />

3 areas occupied by <strong>the</strong> source in a two-hour period is equal to (1+1.77S)<br />

where S is <strong>the</strong> average speed <strong>of</strong> advance in km/hr. If <strong>the</strong> source is travelling<br />

along a straight path, S is equal to <strong>the</strong> actual speed. The Pe for a single<br />

moving source <strong>the</strong>n becomes<br />

The basic formulation <strong>of</strong> <strong>the</strong> St<strong>and</strong>ardized Noise Contribution Model can be<br />

summarized by <strong>the</strong> following equation:<br />

SNC(S1) = Ls(S1) - TLr + 10 Log{(Tf)(Pe)(Ns)} (dB re 1 pPa at 300 m)<br />

where<br />

SNC(S1) = The st<strong>and</strong>ardized noise contribution <strong>of</strong> source Type 1 at a<br />

specific site (1/3 octave b<strong>and</strong> spectrum)<br />

L,(SI) = Source Level <strong>of</strong> <strong>the</strong> Type 1 source (dB re 1 wPa, 1 m) (1/3<br />

octave b<strong>and</strong> spectrum)<br />

TLr = Transmission Loss in <strong>the</strong> area at a range <strong>of</strong> 300 m (dB)<br />

(1/3 octave b<strong>and</strong> spectrum)<br />

Tf = (Time Fraction) Source-on duration/Reference period<br />

Pe = (Probability <strong>of</strong> Encounter) The probability that a<br />

specific type <strong>of</strong> source will be found in a 1 km2 area<br />

surrounding <strong>the</strong> receiver location<br />

N(S1) = Number <strong>of</strong> Type 1 sources in a specific area.<br />

The SNC spectra <strong>of</strong> <strong>the</strong> significant sources in a specific area can be added<br />

toge<strong>the</strong>r using a 1/3 octave power summation process to determine a composite<br />

st<strong>and</strong>ardized noise level.<br />

The formulation <strong>of</strong> <strong>the</strong> SNC Model in Eq. (20) does not distinguish<br />

between fixed sources that fluctuate in level <strong>and</strong> moving sources that

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