On a unified breaking onset threshold for gravity waves in deep and intermediate depth water

被引:85
作者
Barthelemy, X. [1 ,2 ]
Banner, M. L. [1 ]
Peirson, W. L. [2 ]
Fedele, F. [3 ]
Allis, M. [4 ]
Dias, F. [5 ]
机构
[1] UNSW Sydney, Sch Math & Stat, Sydney, NSW 2052, Australia
[2] UNSW Sydney, Sch Civil & Environm Engn, Water Res Lab, 110 King St, Manly Vale, NSW 2093, Australia
[3] Georgia Inst Technol, Sch Civil & Environm Engn, Atlanta, GA 30332 USA
[4] Natl Inst Water & Atmospher Res, Hamilton 3216, New Zealand
[5] Univ Coll Dublin, Sch Math & Stat, Dublin, Ireland
基金
欧洲研究理事会; 澳大利亚研究理事会; 爱尔兰科学基金会;
关键词
surface gravity waves; wave breaking; waves/free-surface flows; 3-DIMENSIONAL OVERTURNING WAVES; ORDER SPECTRAL METHOD; PART; NUMERICAL-SIMULATION; SINGULAR-INTEGRALS; ENERGY; STRENGTH; VELOCITY; MODELS; FIELD;
D O I
10.1017/jfm.2018.93
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
We revisit the classical but as yet unresolved problem of predicting the breaking onset of 2D and 3D irrotational gravity water waves. Based on a fully nonlinear 3D boundary element model, our numerical simulations investigate geometric, kinematic and energetic differences between maximally tall non-breaking waves and marginally breaking waves in focusing wave groups. Our study focuses initially on unidirectional domains with flat bottom topography and conditions ranging from deep to intermediate depth (depth to wavelength ratio from 1 to 0.2). Maximally tall non-breaking (maximally recurrent) waves are clearly separated from marginally breaking waves by their normalised energy fluxes localised near the crest tip region. The initial breaking instability occurs within a very compact region centred on the wave crest. On the surface, this reduces to the local ratio of the energy flux velocity (here the fluid velocity) to the crest point velocity for the tallest wave in the evolving group. This provides a robust threshold parameter for breaking onset for 2D wave packets propagating in uniform water depths from deep to intermediate. Further targeted study of representative cases of the most severe laterally focused 3D wave packets in deep and intermediate depth water shows that the threshold remains robust. These numerical findings for 2D and 3D cases are closely supported by our companion observational results. Warning of imminent breaking onset is detectable up to a fifth of a carrier wave period prior to a breaking event.
引用
收藏
页码:463 / 488
页数:26
相关论文
共 65 条
[1]  
Allis M. J, 2013, THESIS
[2]  
[Anonymous], 1977, The Dynamics of the Upper Ocean
[3]   GENERALIZED VORTEX METHODS FOR FREE-SURFACE FLOW PROBLEMS [J].
BAKER, GR ;
MEIRON, DI ;
ORSZAG, SA .
JOURNAL OF FLUID MECHANICS, 1982, 123 (OCT) :477-501
[4]   Linking Reduced Breaking Crest Speeds to Unsteady Nonlinear Water Wave Group Behavior [J].
Banner, M. L. ;
Barthelemy, X. ;
Fedele, F. ;
Allis, M. ;
Benetazzo, A. ;
Dias, F. ;
Peirson, W. L. .
PHYSICAL REVIEW LETTERS, 2014, 112 (11)
[5]   Wave breaking onset and strength for two-dimensional deep-water wave groups [J].
Banner, Michael L. ;
Peirson, William L. .
JOURNAL OF FLUID MECHANICS, 2007, 585 :93-115
[6]   On the determination of the onset of breaking for modulating surface gravity water waves [J].
Banner, ML ;
Tian, X .
JOURNAL OF FLUID MECHANICS, 1998, 367 :107-137
[7]  
BARTHELEMY X., 2015, ARXIV150806001
[8]   On the efficient numerical simulation of directionally spread surface water waves [J].
Bateman, WJD ;
Swan, C ;
Taylor, PH .
JOURNAL OF COMPUTATIONAL PHYSICS, 2001, 174 (01) :277-305
[9]   Wave breaking and the surface velocity field for three-dimensional water waves [J].
Bridges, Thomas J. .
NONLINEARITY, 2009, 22 (05) :947-953
[10]   Simulation of Wave Breaking in One-Dimensional Spectral Environment [J].
Chalikov, Dmitry ;
Babanin, Alexander V. .
JOURNAL OF PHYSICAL OCEANOGRAPHY, 2012, 42 (11) :1745-1761