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contributor authorHsu, Chin-Tsau
contributor authorWu, Hong-Ye
contributor authorHsu, En-Yun
contributor authorStreet, Robert L.
date accessioned2017-06-09T14:46:16Z
date available2017-06-09T14:46:16Z
date copyright1982/09/01
date issued1982
identifier issn0022-3670
identifier otherams-26395.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4163284
description abstractComplete expressions for wind momentum and energy transfer to wind-generated waves are derived based on a boundary-layer integral method. The airflow and wave measurements as made by Wu et al. (1977, 1979) are used to provide a first-order estimate of the momentum and energy budget. The momentum and energy transfer to waves are found to be dominated by the wave-induced pressure and mainly received by the dominant wave, which agree with the wind energy input mechanism of a nonlinear wind-waves model proposed by Lake and Yuen (1978) and Yuen and Lake (1979). It is found that the waves support about 61% of the total wind momentum, but receive only about 29% of the tow wind energy across the interface. This low fraction of energy to the waves is found to be the consequence of a high ratio of mean surface current velocity to wave celerity which results in a considerable leakage of energy delivered by the wave-supported momentum to the current. The measured energy transfer to waves by the wave-induced pressure is found to be in good agreement with that observed by others in the laboratory and in the field. The comparison of wave-growth parameter based on the wave-induced pressure to the field observations of Snyder et al. (1981) and to the predictions of Al-Zanaidi and Hui (1981) shows a strong dependence of the wave-growth parameter on the wave slope. Based on the side-band instability theory of Benjamin and Feir (1967) and the nonlinear wave-modulation theory of Yuen and Lake (1980), the down-shifting of dominant wave frequency f0 along the fetch x1 is found to be described by f0u*/g = 0.91(x1g/u2*)?5/16, where u* is the wind friction velocity and g the gravitational acceleration. As a result, the dominant wave slope k0? changes with the fetch as k0? = 0.58 ? (x1g/u2*)??; this implies an evolution of the wind wave from a bounded, nonlinear system at short fetch to a free linear system at large fetch (a fully developed sea state). The decrease in the saturation range constant (Phillips, 1958, 1977) with increasing fetch is found to be closely related to this evolution.
publisherAmerican Meteorological Society
titleMomentum and Energy Transfer in Wind Generation of Waves
typeJournal Paper
journal volume12
journal issue9
journal titleJournal of Physical Oceanography
identifier doi10.1175/1520-0485(1982)012<0929:MAETIW>2.0.CO;2
journal fristpage929
journal lastpage951
treeJournal of Physical Oceanography:;1982:;Volume( 012 ):;issue: 009
contenttypeFulltext


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