On Determining the Onset and Strength of Breaking for Deep Water Waves. Part II: Influence of Wind Forcing and Surface Shear

Abstract Part I of this study describes the authors' findings on a robust threshold variable that determines the onset of breaking for unforced, irrotational deep water waves and proposes a means of predicting the strength of breaking if the breaking threshold is exceeded. Those results were based on a numerical study of the unforced evolution of fully nonlinear, two-dimensional inviscid wave trains and highlight the fundamental role played by the nonlinear wave group dynamics. In Part II the scope of these calculations is extended to investigate the additional influence of wind forcing and background shear on the evolution to breaking. Using the methodology described in Part I, the present study focuses on the influence of wind forcing and vertical shear on long-term evolution toward breaking or recurrence of the maximum of the local energy density within a wave group. It investigates the behavior of a dimensionless local growth rate parameter that reflects the mean energy flux to the energy maximum in t...

[1]  M. Longuet-Higgins,et al.  Periodicity in Whitecaps , 1972, Nature.

[2]  W. Plant A relationship between wind stress and wave slope , 1982 .

[3]  M. Banner,et al.  Modeling Wave-Enhanced Turbulence in the Ocean Surface Layer , 1994 .

[4]  Leo H. Holthuijsen,et al.  Statistics of Breaking Waves Observed as Whitecaps in the Open Sea , 1986 .

[5]  Paolo Boccotti,et al.  A field experiment on the mechanics of irregular gravity waves , 1993 .

[6]  P. Saffman,et al.  Effect of a surface shear layer on gravity and gravity–capillary waves of permanent form , 1990, Journal of Fluid Mechanics.

[7]  H. Mitsuyasu,et al.  The Effect of Swell on the Growth of Wind Waves , 1991 .

[8]  M. Donelan,et al.  Effects of Velocity Shear on the Stability of Surface Deep Water Wave Trains , 1988 .

[9]  Mark A. Donelan,et al.  Expected Structure of Extreme Waves in a Gaussian Sea. Part I: Theory and SWADE Buoy Measurements , 1993 .

[10]  O. M. Phillips,et al.  Wave breaking in the presence of wind drift and swell , 1974, Journal of Fluid Mechanics.

[11]  Takuji Waseda,et al.  Laboratory observations of wave group evolution, including breaking effects , 1999, Journal of Fluid Mechanics.

[12]  J. S. Chu,et al.  Measurements of the interaction of wave groups with shorter wind-generated waves , 1992, Journal of Fluid Mechanics.

[13]  Jinbao Song,et al.  On Determining the Onset and Strength of Breaking for Deep Water Waves. Part I: Unforced Irrotational Wave Groups , 2002 .

[14]  Xin Tian,et al.  On the determination of the onset of breaking for modulating surface gravity water waves , 1998, Journal of Fluid Mechanics.

[15]  Stephen E. Belcher,et al.  Effects of Long Waves on Wind-Generated Waves , 2000 .

[16]  T. Waseda,et al.  Experimental study of the stability of deep-water wave trains including wind effects , 1999, Journal of Fluid Mechanics.

[17]  B. Fornberg A Numerical Method for Conformal Mappings , 1980 .

[18]  John W. Dold,et al.  Water-Wave Modulation , 1986 .

[19]  M. Donelan,et al.  Dynamics and Modelling of Ocean Waves , 1994 .

[20]  W. Pierson,et al.  A proposed spectral form for fully developed wind seas based on the similarity theory of S , 1964 .

[21]  M. Longuet-Higgins Statistical properties of wave groups in a random sea state , 1984, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[22]  D. H. Peregrine,et al.  Steep, steady surface waves on water of finite depth with constant vorticity , 1988, Journal of Fluid Mechanics.

[23]  O. M. Phillips,et al.  On the incipient breaking of small scale waves , 1974, Journal of Fluid Mechanics.

[24]  N. Huang,et al.  Experimental study of the influence of wind on Benjamin–Feir sideband instability , 1986, Journal of Fluid Mechanics.

[25]  O. Phillips The dynamics of the upper ocean , 1966 .