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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 />

<strong>of</strong> man-associated activities such as vessels <strong>and</strong> aircraft are presented in<br />

Section 3.3 on a 1/3 octave b<strong>and</strong> basis.<br />

3.2.1 Meteorological sources (wind, rain, sleet)<br />

An early major summary <strong>of</strong> ocean ambient noise, published by Knudsen et<br />

al. (1944), has become a common baseline for comparison <strong>of</strong> ambient noise<br />

conditions in both <strong>the</strong> deep water <strong>and</strong> shallow water environment. However, <strong>the</strong><br />

st<strong>and</strong>ard "Knudsen curves", which provide a means for estimating background<br />

noise levels to be expected for particular wind or sea state conditions, apply<br />

most reliably to deep ocean conditions, <strong>and</strong> <strong>the</strong>n most effectively for frequencies<br />

between 500 Hz <strong>and</strong> 50 kHz. Shallow water ambient noise levels, <strong>the</strong> focus<br />

<strong>of</strong> this study, tend to agree with <strong>the</strong> Knudsen curves for frequencies above<br />

1000 Hz but can vary considerably from site-to-site in continental shelf <strong>and</strong><br />

near-shore areas. Wenz (1962) <strong>and</strong> Urick (1983) provide useful ambient noise<br />

summaries for <strong>the</strong> shallow water environment (as well as deep water). Figure<br />

3.1 includes average shallow water spectra for typical wind <strong>and</strong> rain<br />

conditions obtained from <strong>the</strong>ir summaries.<br />

- Wind<br />

On a 1 &octave basis, wind-related ambient noise in shallow water (Fig.<br />

3.1) tends to peak at about 1 kHz. Levels in 1/3 octave b<strong>and</strong>s generally<br />

decrease at a rate <strong>of</strong> 3-4 dB per octave at progressively higher frequencies<br />

<strong>and</strong> at about 6 dB per octave at progressively lower frequencies. Sound levels<br />

increase at a rate <strong>of</strong> 5-6 dB per doubling <strong>of</strong> wind speed. Maximum 1/3-octave<br />

b<strong>and</strong> levels <strong>of</strong> about 95 dB referenced to 1 pPa are frequently observed at<br />

about 1 kHz for sustained winds <strong>of</strong> 17-21 m/sec (34-40 knots) <strong>and</strong> about 82 dB<br />

also at 1 kHz when <strong>the</strong> winds are in <strong>the</strong> 3.4 - 5.4 m/s or 7-10 knot range.<br />

Since ambient noise related to wind is caused primarily by wave action <strong>and</strong><br />

spray (<strong>and</strong> possibly to some extent to acoustic <strong>and</strong> pressure fluctuation<br />

coupling effects from air to water), <strong>the</strong> wind related noise component is<br />

strongly dependent on wind duration <strong>and</strong> fetch as well as water depth, bottom<br />

topography <strong>and</strong> proximity to topographic features such as isl<strong>and</strong>s <strong>and</strong> shore. A<br />

sea state scale which is related to sea surface conditions as a function <strong>of</strong><br />

wind conditions is commonly used in categorizing wind-related ambient noise<br />

Table 3.1). The curves for wind-related ambient noise shown in Fig. 3.1 are<br />

reasonable averages, although relatively large departures from <strong>the</strong>se curves<br />

can be experienced depending on site location <strong>and</strong> o<strong>the</strong>r factors such as bottom<br />

topography- <strong>and</strong> proximity to isl<strong>and</strong> or l<strong>and</strong> features. Statistical estimates <strong>of</strong><br />

ambient noise conditions along <strong>the</strong> coast <strong>of</strong> <strong>the</strong>-Alaskan Beaufort Sea (Miles et<br />

al. 1987) predict that <strong>the</strong> 95th percentile <strong>and</strong> 5th percentile levels <strong>of</strong><br />

ambient noise (due primarily to wind) are 10 to 20 dB above <strong>and</strong> -below <strong>the</strong><br />

median level respectively. The median levels in <strong>the</strong> Beaufort Sea, as shown by<br />

-<strong>the</strong>* <strong>and</strong> o symbols in Fig. 3.1 <strong>and</strong> by Greene ( 1987), are close to <strong>the</strong> Sea<br />

State 2 curve.<br />

- Rain<br />

Water droplets impacting <strong>the</strong> ocean surface can be a major high frequency<br />

source <strong>of</strong> ambient noise in <strong>the</strong> ocean, depending on precipitation rate. As<br />

described by Wenz (1962) <strong>and</strong> Urick (1983) <strong>and</strong> based on <strong>the</strong>ir review <strong>of</strong>

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