Probability distributions of surface gravity waves during spectral changes
By Hervé Socquet-Juglard, K. Dysthe, Karsten Trulsen, Harald E. Krogstad, Jingdong Liu. Journal of Fluid Mechanics, 2005
275 citations recorded by the source corpus.
Subfields: Earth-Surface Processes, Geophysics, Oceanography
View Paper: https://www.semanticscholar.org/paper/8488a902cb65dd78c7f39ccb8e1ab0862bcafe49
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Earth-Surface Processes
- Francesco Fedele
- M. Onorato
- Hitoshi Tamura
- Takuji Waseda
- T. Kinoshita
- Karsten Trulsen
- M. Tayfun
- Luigi Cavaleri
In Geophysics
In Oceanography
- Francesco Fedele
- M. Onorato
- Karsten Trulsen
- Peter A. E. M. Janssen
- Hitoshi Tamura
- Takuji Waseda
- T. Kinoshita
- M. Tayfun
Citations in the corpus
- On nonlinear wave groups and crest statistics (2009, background): “The numerical simulations of relatively wideband waves based on the Dysthe equation (Socquet-Juglard et al. 2005) and the fairly recent analyses of oceanic measurements gathered during a number of hurricanes in the Gulf of Mexico and North Sea storms (Forristall 2000, 2007; Tayfun & Fedele 2007b;…”
- Evolution of weakly nonlinear random directional waves: laboratory experiments and numerical simulations (2010, methodology): “The numerical and experimental p.d.f.s are compared to the Gaussian distribution and the Tayfun second-order distribution (see Tayfun 1980 and (8) in Socquet-Juglard et al. 2005 for details).”
- Statistical properties of mechanically generated surface gravity waves: a laboratory experiment in a three-dimensional wave basin (2009, background): “…second-order distribution (see Socquet-Juglard et al. 2005): p(η) = 1 − 7σ 2k2p/8√ 2π(1 + 3G + 2G2) exp ( − G 2 2σ 2k2p ) , (3.3) where G = √ 1 + 2k2pση − 1, (3.4) which has been derived in Socquet-Juglard et al. (2005) as an approximation of the Tayfun second-order distribution (see Tayfun 1980).”
- Evolution of a Random Directional Wave and Freak Wave Occurrence (2009, background): “This result is consistent with the report by Soquet-Juglard et al. (2005) and more recently by Gramstad and Trulsen (2007).”
- On Oceanic Rogue Waves (2015, methodology): “ximum over large areas (‘˛L 0) x(PT) ST =x m+2mx 2 + g e (1+4mx m) 16x m ; (21) where now xsatisfies 16M 3 m 2P R(x ) = 1. This is the 3-D analogue of the 2-D Piterbarg-Tayfun (PT) model formulated by Socquet-Juglard et al. (2005), and hereafter referred to as 3D-PT (see also Piterbarg (1995) and For”