The modulation of short wind wave breaking in the long surface wave field

Author(s):  
V.V. Bakhanov ◽  
N.A. Bogatov ◽  
A.V. Ermoshkin ◽  
O.N. Kemarskaya
2013 ◽  
Author(s):  
V. V. Bakhanov ◽  
N. A. Bogatov ◽  
A. V. Ermoshkin ◽  
A. A. Kandaurov ◽  
O. N. Kemarskaya ◽  
...  

Author(s):  
Johannes Gemmrich ◽  
Adam Monahan

AbstractIn an idealized two-layer fluid, surface waves can generate waves at the internal interface through class 3 resonant triads in which all waves are propagating in the same direction. The triads are restricted to wavenumbers above a critical value kcrit that depends on the density ratio R between the two layers, and their depths. We perform numerical simulations to analyze the evolution of a surface wave field, initially specified by a Pierson-Moskowitz type spectrum, for R = 0:97 (representing a realistic lower a bound for oceanic stratification). At high initial steepness and peak wavenumber kp ≪ kcrit, the energy increases in the spectral tail; as a parameterization of resulting wave breaking, at each time step individual waves with a steepness greater than the limiting Stokes steepness are removed. The energy change of the surface wave field is a combination of energy transfer to the interfacial waves, spectral downshift, and wave breaking dissipation. At wavenumbers ≳ 0:6kp there is a net loss of energy, with the greatest dissipation at ≈ 1:3kp. The maximum gain occurs at ≈ 0:5kp. The onset of the spectral change shows a strong threshold behaviour with respect to the the initial wave steepness. For steep initial waves the integrated energy dissipation can reach > 30% of the initial energy, and only ≈ 1% of the initial surface wave energy is transferred to the interfacial wave field. The spectral change could be expressed as an additional dissipation source term, and coupled ocean/wave models should include additional mixing associated with the interfacial waves and enhanced wave breaking turbulence.


Author(s):  
Teodor Vrećica ◽  
Nick Pizzo ◽  
Luc Lenain

AbstractOcean submesoscale currents, with spatial scales on the order of 0.1 to 10 km, are horizontally divergent flows, leading to vertical motions that are crucial for modulating the fluxes of mass, momentum and energy between the ocean and the atmosphere, with important implications for biological and chemical processes. Recently, there has been considerable interest in the role of surface waves in modifying frontal dynamics. However, there is a crucial lack of observations of these processes, which are needed to constrain and guide theoretical and numerical models. To this end, we present novel high resolution airborne remote sensing and in situ observations of wave-current interaction at a submesoscale front near the island of O’ahu, Hawaii. We find strong modulation of the surface wave field across the frontal boundary, including enhanced wave breaking, that leads to significant spatial inhomogeneities in the wave and wave breaking statistics. The non-breaking (i.e. Stokes) and breaking induced drifts are shown to be increased at the boundary by approximately 50% and an order of magnitude, respectively. The momentum flux from the wave field to the water column due to wave breaking is enhanced by an order of magnitude at the front. Using an orthogonal coordinate system that is tangent and normal to the front, we show that these sharp modulations occur over a distance of several meters in the direction normal to the front. Finally, we discuss these observations in the context of improved coupled models of air-sea interaction at a submesoscale front.


2019 ◽  
Vol 37 (6) ◽  
pp. 2025-2036 ◽  
Author(s):  
Zhendong Liu ◽  
Haixing Liu ◽  
Tianyun Su ◽  
Zhen Jia ◽  
Xinfang Li ◽  
...  

1993 ◽  
Vol 20 (1-2) ◽  
pp. 55-77 ◽  
Author(s):  
G.R. Spedding ◽  
F.K. Browand ◽  
N.E. Huang ◽  
S.R. Long

2017 ◽  
Vol 47 (8) ◽  
pp. 1921-1939 ◽  
Author(s):  
Alexander W. Fisher ◽  
Lawrence P. Sanford ◽  
Malcolm E. Scully ◽  
Steven E. Suttles

AbstractThe role of surface gravity waves in structuring the air–sea momentum flux is examined in the middle reaches of Chesapeake Bay. Observed wave spectra showed that wave direction in Chesapeake Bay is strongly correlated with basin geometry. Waves preferentially developed in the direction of maximum fetch, suggesting that dominant wave frequencies may be commonly and persistently misaligned with local wind forcing. Direct observations from an ultrasonic anemometer and vertical array of ADVs show that the magnitude and direction of stress changed across the air–sea interface, suggesting that a stress divergence occurred at or near the water surface. Using a numerical wave model in combination with direct flux measurements, the air–sea momentum flux was partitioned between the surface wave field and the mean flow. Results indicate that the surface wave field can store or release a significant fraction of the total momentum flux depending on the direction of the wind. When wind blew across dominant fetch axes, the generation of short gravity waves stored as much as 40% of the total wind stress. Accounting for the storage of momentum in the surface wave field closed the air–sea momentum budget. Agreement between the direction of Lagrangian shear and the direction of the stress vector in the mixed surface layer suggests that the observed directional difference was due to the combined effect of breaking waves producing downward sweeps of momentum in the direction of wave propagation and the straining of that vorticity field in a manner similar to Langmuir turbulence.


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