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ssc-367 - Ship Structure Committee

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common probability distributions, the Gaussian (or normal)<br />

distribution and-the Rayleigh distribution. These probability<br />

distributions are used to define the distribution of wave elevations, n,<br />

and of wave heights, H, respectively.<br />

A.2.1<br />

CharacteristicFrequencies and Periods<br />

For design purposes sea spectra equations are selected to represent<br />

middle aged seas that would exist some time after a storm, yet which<br />

are still young enough to have a good dispersion of wave<br />

frequencies. The primary assumption about the design seas is that<br />

the wave elevations follow a Gaussian or normal distribution.<br />

Samples of wave records tend to support this assumption. In<br />

conjunction with the Gaussian distribution assumption, the wave<br />

elevations are assumed to have a zero mean. Digitized wave records<br />

tend to have a slight drift of the mean away from zero, usually<br />

attributed to tide or instrument drift. The Gaussian distribution<br />

assumption is equivalent to assuming that the phase angles of the<br />

constituentwaves within a wave spectrum, are uniformly distributed.<br />

The Gaussian distribution allows one to calculate statistical<br />

parameters which are used to describe the random sea. The mean<br />

elevation of the water surface is the first moment of the Gaussian<br />

probability density function. The mean-square is the second moment<br />

taken about zero, and the root-mean-square is the positive square<br />

root of the mean-square. The variance is the second moment taken<br />

about the mean value. The standard deviation is the positive square<br />

root of the variance. Since the wave elevations are assumed to have<br />

a zero mean value, the variance is equal to the mean-square, and the<br />

standard deviation is equal to the root-mean-square. In present<br />

practice, the area under a random wave energy spectrum is equated to<br />

the variance.<br />

In a similar way, the characteristic frequencies and periods of a<br />

wave spectrum are defined in terms of the shape, the area, and/or the<br />

area moments of the ~*a2 wave spectrum. Depending upon the<br />

A-6<br />

i<br />

ij<br />

-,,

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