Nonlinear Water Waves with Applications to Wave-Current Interactions and Tsunamis
By Adrian Constantin. 2011
492 citations recorded by the source corpus.
Subfields: Earth-Surface Processes, Oceanography
View Paper: https://www.semanticscholar.org/paper/ebd71183f02ae2b7281bee89604e0084bcf617ae
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
- Adrian Constantin
- Eugen Varvaruca
- Walter A. Strauss
- R. Johnson
- David Henry
- Rossen I. Ivanov
- Yue Liu
- Erik Wahlén
In Oceanography
- Adrian Constantin
- Eugen Varvaruca
- Walter A. Strauss
- R. Johnson
- David Henry
- Erik Wahlén
- Yue Liu
- Zhaoyang Yin
Citations in the corpus
- An Exact, Steady, Purely Azimuthal Equatorial Flow with a Free Surface (2016, background): “, plane Poiseuille flow, Stokes’ unsteady problems, and many more; see Drazin and Riley 2007) and the classical inviscid nonlinear surface wave discovered byGerstner (see Gerstner 1809; Constantin 2011).”
- The dynamics of waves interacting with the Equatorial Undercurrent (2015, background): “Recently, explicit nonlinear solutions were obtained in the Lagrangian framework, these being for equatorially-trapped waves (see Constantin 2012, Henry 2013). Correspondingly, solutions for the internal waves have been described in Constantin (2014). However, both these types of solution are restri”
- Global bifurcation of steady gravity water waves with critical layers (2014, background): “This is appropriate for the ebb current, while Υ < 0 captures flood currents [10].”
- On the modelling of equatorial waves (2012, unknown): “…mass flux, given by m ¼ Z d hðxÞ ðu cÞdz: ð9Þ Note that the first two equations in (8) merely state the fact that the expression y2x þ y2z 2 ðg þ 2wÞyþ ðg 2wcÞzþ 1 r P is constant throughout the layer h(x) < z < d, in analogy with Bernoulli’s law for gravity water waves [see Constantin, 2011].”
- Some Nonlinear, Equatorially Trapped, Nonhydrostatic Internal Geophysical Waves (2014, background): “Note that r 5 r0(s) corresponds to the thermocline z 5 h0(x 2 ct, s), so that a particle located initially on the thermocline will always remain there and (7) with i 5 0 therefore holds (see Constantin 2011).”