It is shown that some recent data on the crest‐to‐trough heights of sea waves are fitted just as well as by the one‐parameter Rayleigh distribution as by the two‐parameter Weibull distribution, provided that the rms amplitude ā is taken as 0.925(2 m 0 ) 1/2 , where m 0 is the lowest moment of the frequency spectrum. Reasons why the ratio ā/(2 m 0 ) 1/2 should differ from unity are discussed. It is shown that the effect of finite wave steepness would be to increase the ratio by a factor [1 + ( ak )2] approximately, contrary to observation. The effect of finite band width is estimated from a model assuming low background noise superposed linearly on a delta function spectrum. For narrow band widths one obtains the formula ā 2 /2 m 0 = 1 − 0.734ν 2 , where ν is the rms spread of the noise about the mean frequency. Values of ν 2 corresponding to Pierson‐Moskowicz spectra give results in close agreement with observation.
No takes yet. Share an insight, caveat, or question.
M. S. Longuet‐Higgins (1980) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: