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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> Technology Corporation<br />

third-octave b<strong>and</strong>s. The spectrum in Figure B.1B was begun at time 13:23:26,<br />

when <strong>the</strong> ship had been pushing ahead but reversed pitch to back away from <strong>the</strong><br />

ice. This spectrum contained <strong>the</strong> highest third octave levels at 20 <strong>and</strong> 31.5<br />

Hz, <strong>and</strong> <strong>the</strong> lowest third octave levels at <strong>the</strong> highest frequencies.<br />

Figure B.2 contains five spectra composed by sorting <strong>the</strong> individual<br />

frequency analysis cells over <strong>the</strong> 53 spectra <strong>and</strong> determining <strong>the</strong> minimum,<br />

maximum, <strong>and</strong> <strong>the</strong> 5th, 50th (median) <strong>and</strong> 95th percentile levels. In one point<br />

<strong>of</strong> view, this figure presents five points on <strong>the</strong> cumulative distribution <strong>of</strong><br />

spectrum levels for each frequency cell from 20 to 4000 Hz. Somewhat<br />

surprisingly, <strong>the</strong>re is relatively little variation between <strong>the</strong> lowest <strong>and</strong><br />

highest spectrum levels at low frequencies (about 20 dB). The sounds at those<br />

frequencies come mostly from <strong>the</strong> ship's machinery <strong>and</strong> propellers. Although<br />

<strong>the</strong> machinery operating speed is constant for all phases <strong>of</strong> <strong>the</strong> icebreaking,<br />

<strong>the</strong> power generated varies substantially. At <strong>the</strong> high frequencies, we expect<br />

considerable spread in <strong>the</strong> levels, as is shown, because <strong>of</strong> <strong>the</strong> effects <strong>of</strong><br />

cavitation. The propellers cavitate most severely during <strong>the</strong> "bollardft<br />

condition <strong>and</strong> when changing direction from going astern to goind ahead. When<br />

changing <strong>the</strong> power setting from reverse to forward, <strong>the</strong> propellers pass<br />

through a condition where <strong>the</strong>re is no cavitation at all. For comparison, <strong>the</strong><br />

idealized spectrum for Knudsen et al. (1948) Sea State 6 is shown at <strong>the</strong><br />

bottom <strong>of</strong> <strong>the</strong> figure.<br />

Table B.l presents <strong>the</strong> cumulative distribution information for each <strong>of</strong><br />

<strong>the</strong> third-octave frequency b<strong>and</strong>s. Consistent with <strong>the</strong> effect seen in <strong>the</strong><br />

statistical spectra, <strong>the</strong> span <strong>of</strong> levels at low frequencies is only 15 dB at 20<br />

Hz, 10 dB at 31.5 Hz, but at high frequencies it is 38 dB at 3150 Hz.<br />

Figure B.3 presents <strong>the</strong> variation in sound level vs. time for four third-<br />

octave b<strong>and</strong>s: 20, 50, 500, <strong>and</strong> 3150 Hz. During <strong>the</strong> 14 minutes recorded <strong>and</strong><br />

analyzed, <strong>the</strong> ship went through about five cycles <strong>of</strong> "backing <strong>and</strong> rammingft a<br />

heavy ice floe in attempting to break it up. To depict <strong>the</strong>se cycles, at <strong>the</strong><br />

bottom <strong>of</strong> each graph we have drawn a tlr<strong>and</strong>om square wave" representing <strong>the</strong><br />

times <strong>the</strong> icebreaker was going forward <strong>and</strong> in reverse. Also shown are <strong>the</strong><br />

instants <strong>of</strong> time when <strong>the</strong> ship's forward progress was seen to be stopped by<br />

<strong>the</strong> ice. The ship did not go into reverse immediately after being stopped,

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