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Third Generation Wind Wave Model Frequency Dependence of the White-Capping Dissipation Source Function

机译:第三代风波模型频率依赖性的白盖耗散源功能

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This paper proposes a new frequency dependence for the empirical formulas presently used to determine wave energy dissipation in ocean wave models. Using an energy focusing technique, several unidirectional transient wave trains were generated. Each of the transient wave train contained an isolated plunging or spilling breaker. By comparing the energy spectra of free-wave components before and after a breaker it was found that: 1) the energy loss as a function of frequency is almost exclusively from wave components at frequencies higher than the spectral peak frequency; 2) although the energy density of the wave components near the peak frequency are the largest, they do not significantly gain or lose energy after breaking; and 3) wave components of frequencies significantly below or near the peak frequency gain a small portion (about 12%) of energy lost by the high-frequency waves. The empirical formulas presently used to determine white-capping dissipation (Komen et al. 1994; Tolman and Chalikov 1996; Booij 1999) do not agree with the above spectral distribution of energy dissipation. Analysis of the dissipation distribution obtained by Meza et al. (2000), suggest that the dependence of the dissipation rate on the frequency should be described by, (ω/ω_p)(1-ω/ω_p) E(ω), where ω is the wave frequency, ω_p is the spectral peak frequency and E(ω) is the energy density spectrum. An energy dissipation source function with such a frequency dependence is being implemented and tested in a third generation wind wave model.
机译:本文提出了目前用于确定海浪模型中波能量耗散的经验公式的新频率依赖性。使用能量聚焦技术,产生了几个单向瞬态波动列车。每个瞬态波动火车含有隔离的嘴巴或溢出的断路器。通过比较断路器之前和之后的自由波组分的能谱,发现:1)作为频率函数的能量损失几乎完全来自高于光谱峰值频率的频率的波分量; 2)尽管峰值频率附近的波部件的能量密度是最大的,但它们在断裂后不会显着增益或失去能量; 3)频率显着低于或接近峰值频率的波部件,通过高频波损失的小部分(约12%)。目前用于确定白盖耗散的经验公式(Komen等人1994; Tolman和Chalikov 1996; Booj 1999)不同意上述能量耗散的光谱分布。 Meza等人获得的耗散分布分析。 (2000),建议耗散频率对频率的依赖性应描述(ω/ω_p)(1-ω/ω_p)e(ω),其中ω是波频,ω_p是光谱峰值频率并且e(ω)是能量密度谱。在第三代风波模型中正在实现和测试具有这种频率依赖性的能量耗散源功能。

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