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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 />

recording system <strong>and</strong> techniques had evolved over six years <strong>of</strong> making such<br />

recordings from small boats.<br />

The analysis was performed using a Hewlett-Packard Vectra computer system<br />

(compatible with <strong>the</strong> IBM PC-AT). The technique was based on <strong>the</strong> weighted,<br />

overlapped segment averaging technique <strong>of</strong> Carter <strong>and</strong> Nuttall (1980). <strong>the</strong><br />

signals were played back through a Krohn-Hite model 3342 filter to prevent<br />

aliasing. A 12-bit Metrabyte model DASH 16 analog-to-digital converter was<br />

used to digitize sections <strong>of</strong> signal each 16.5 s in duration. The sample rate<br />

was 8192 samples/second. The 16.5 s sections were analyzed separately <strong>and</strong> <strong>the</strong><br />

results saved for comparison <strong>and</strong> statistical analyses. They were taken every<br />

16 s. The results were sound pressure spectra with calibrated levels from 10<br />

to 4000 Hz.<br />

Each 16.5 s section was fur<strong>the</strong>r divided into one-second segments for<br />

Fourier analysis using a fast Fourier transform routine. Segments were<br />

overlapped by 50% to permit extracting information from samples at <strong>the</strong> ends <strong>of</strong><br />

each segment attenuated by "windowing" (Harris 1978); we used <strong>the</strong> Blackman-<br />

Harris minimum three-term window. The magnitudes squared (<strong>the</strong> ttpowers") in<br />

each transform cell, or bin, were computed. The results <strong>of</strong> analyzing each<br />

segment were averaged to obtain our estimates <strong>of</strong> <strong>the</strong> sound power spectrum for<br />

a 16.5 s section <strong>of</strong> sound.<br />

The effective b<strong>and</strong>width <strong>of</strong> each spectrum analysis cell was 1.7 Hz,<br />

although <strong>the</strong> cells were spaced 1 Hz apart. The powers in <strong>the</strong> cells were added<br />

to obtain <strong>the</strong> sound power in selected frequency b<strong>and</strong>s, in particular, <strong>the</strong><br />

st<strong>and</strong>ard third-octave b<strong>and</strong>s widely used in acoustical sound <strong>and</strong> noise<br />

measurements. All levels, both spectrum levels <strong>and</strong> b<strong>and</strong> levels, were saved<br />

for statistical analysis, printing, <strong>and</strong> plotting.<br />

There were two statistical analysis techniques. In one, each <strong>of</strong> <strong>the</strong><br />

analysis cells (frequency bins) in <strong>the</strong> 53 resulting spectra were sorted from<br />

smallest to largest. Then, <strong>the</strong> minimum, fifth percentile, fiftieth percentile<br />

(median), ninety-fifth percentile <strong>and</strong> maximum levels for that bin were<br />

identified <strong>and</strong> saved until five statistical spectra were generated,<br />

corresponding to those levels. The five statistical spectra were plotted.

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