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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 />

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Sound Speed, m/sac<br />

Figure 4.2. Range <strong>of</strong> Sound Speed Pr<strong>of</strong>iles for Study Areas.<br />

transmission loss characteristics using published information on bottom<br />

characteristics <strong>and</strong> sound speed pr<strong>of</strong>iles.<br />

The source <strong>and</strong> receiver depths used in <strong>the</strong> modeling work were 5 m <strong>and</strong><br />

10 m respectively to represent <strong>the</strong> average depth <strong>of</strong> ship <strong>and</strong> boat propellers<br />

<strong>and</strong> a representative depth <strong>of</strong> marine mammal habitat. It was necessary to<br />

perform both frequency <strong>and</strong> depth averaging <strong>of</strong> <strong>the</strong> model output to obtain<br />

transmission loss characteristics that were not over.1~ influenced by single<br />

frequency interference patterns. For most <strong>of</strong> <strong>the</strong> analysis <strong>the</strong> model output<br />

for three frequencies was averaged, corresponding to <strong>the</strong> upper, middle, <strong>and</strong><br />

lower frequencies <strong>of</strong> a 1/3 octave b<strong>and</strong>. In this way, results for <strong>the</strong> 100,<br />

315, <strong>and</strong> 1000 Hz 1/3 octave b<strong>and</strong>s were obtained. In addition, <strong>the</strong> received<br />

levels were depth-averaged from 5 to 15 m.<br />

An example <strong>of</strong> <strong>the</strong> output <strong>of</strong> <strong>the</strong> IFD Model is shown in Fig. 4.3. Here<br />

propagation in a region <strong>of</strong> <strong>the</strong> Norton Basin Planning Area with a depth <strong>of</strong> 33 m<br />

was considered. Figure 4.3A presents <strong>the</strong> predicted transmission loss at 3<br />

frequencies for <strong>the</strong> strong surface layer pr<strong>of</strong>ile shown in Fig. 4.2. Using<br />

information obtained from <strong>the</strong> literature (Mackenzie 1973), <strong>the</strong> model<br />

incorporated a bottom composition <strong>of</strong> silt-s<strong>and</strong> with a thickness <strong>of</strong> 2 m <strong>and</strong> a<br />

sub-bottom layer <strong>of</strong> basalt. The transmission loss for <strong>the</strong> same region under<br />

neutral gradient conditions is shown in Fig. 4.3B. The transmission loss<br />

characteristics can be seen to be similar out to a range <strong>of</strong> 3 km. Beyond this<br />

range <strong>the</strong> loss can be seen to be significantly less for <strong>the</strong> neutral gradient<br />

condition, with <strong>the</strong> greatest difference occurring at 1 kHz. These results<br />

indicate that <strong>the</strong> range <strong>of</strong> influence <strong>of</strong> <strong>the</strong> loudest industrial noise sources<br />

can be changed considerably by seasonal effects on <strong>the</strong> sound speed pr<strong>of</strong>ile.<br />

Transmission loss data reported by Mackenzie (1961) for transmission at 200 Hz<br />

using a shallow source <strong>and</strong> receiver are also shown in Fig. 4.3B. Unfortunately<br />

no data are available at o<strong>the</strong>r frequencies for <strong>the</strong>se conditions in this area.

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