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Introduction to Acoustics

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5.2.5 Ambient Noise<br />

There are essentially two types of ocean acoustic noise:<br />

manmade and natural. Generally, shipping is the most<br />

important source of manmade noise, though noise from<br />

offshore oil rigs is becoming increasingly prevalent. See<br />

also Table 5.2 in the Marine Mammal section for specific<br />

examples of manmade noise. Typically, natural noise<br />

dominates at low frequencies (below 10 Hz) and high<br />

frequencies (above a few hundred Hz). Shipping fills in<br />

the region between ten and a few hundred Hz and this<br />

component is increasing over time [5.25, 26]. A summary<br />

of the spectrum of noise is shown in Fig. 5.15.The<br />

higher-frequency noise is usually parameterized according<br />

<strong>to</strong> the sea state (also Beaufort number) and/or wind.<br />

Table 5.1 summarizes the description of the sea state.<br />

The sound-speed profile affects the vertical and angular<br />

distribution of noise in the deep ocean. When<br />

there is a critical depth (Sect. 5.1.2), sound from sur-<br />

Table 5.1 Descrip<strong>to</strong>r of the ocean sea surface [5.24]<br />

Underwater <strong>Acoustics</strong> 5.2 Physical Mechanisms 161<br />

face sources travels long distances without interacting<br />

with the ocean bot<strong>to</strong>m, but a receiver below this critical<br />

depth should sense less surface noise because propagation<br />

involves interaction with lossy boundaries, the<br />

surface and/or bot<strong>to</strong>m. This is illustrated in Fig. 5.16a,b<br />

which shows a deep-water environment with measured<br />

ambient noise. Figure 5.16c is an example of vertical<br />

directionality of noise which also follows the propagation<br />

physics discussed above. The shallower depth is at<br />

the axis of the deep sound channel while the other is at<br />

the critical depth. The pattern is narrower at the critical<br />

depth where the sound paths tend <strong>to</strong> be horizontal since<br />

the rays are turning around at the lower boundary of the<br />

deep sound channel.<br />

In a range-independent ocean, Snell’s law predicts<br />

a horizontal noise notch at depths where the speed of<br />

sound is less than the near-surface sound speed. Returning<br />

<strong>to</strong> (5.2) and reading off the sound speeds from<br />

Fig. 5.16 at the surface (c =1530 m/s) and say, 300 m<br />

Sea criteria Beau- Wind speed 12 h wind Fully arisen sea Seafort<br />

range mean Wave Wave Fetch b,c state<br />

scale knots knots height a,b height a,b Duration b,c naut. miles scale<br />

(m/s) (m/s) ft (m) ft (m) h (km)<br />

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