Consideration of the structure of wind-generated waves when the duration and fetch of the wind are large suggests that the smaller-scale components of the wave field may be in a condition of statistical equilibrium determined by the requirements for attachment of the crests of the waves. A dimensional analysis, based upon the idea of an equilibrium range in the wave spectrum, shows that for large values of the frequency ω, the spectrum Φ(ω) is of the form Φ (ω) ~ α g²ω⁻⁵ where α is an absolute constant. The instantaneous spatial spectrum Ψ ( k ) is proportional to k −4 for large wave numbers k , which is consistent with the observed occurrence of sharp crests in a well-developed sea, and the loss of energy from the wave system to turbulence and heat is proportional to ρ w u³_* , where ρ w is the water density and u the friction velocity of the wind at the surface. This prediction of the form of Φ(ω) for large ω with α = 7·4×10 −3 , agrees well with measurements made by Burling (1955).
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O. M. Phillips (1958) studied this question.
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