2014
DOI: 10.3934/dcdss.2014.7.239
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Shallow water asymptotic models for the propagation of internal waves

Abstract: We are interested in asymptotic models for the propagation of internal waves at the interface between two shallow layers of immiscible fluid, under the rigid-lid assumption. We review and complete existing works in the literature, in order to offer a unified and comprehensive exposition. Anterior models such as the shallow water and Boussinesq systems, as well as unidirectional models of Camassa-Holm type, are shown to descend from a broad Green-Naghdi model, that we introduce and justify in the sense of consi… Show more

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Cited by 10 publications
(21 citation statements)
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“…Performing these computations, with extensive testing of their numerical accuracy (see also [2,10]), demonstrated a remarkable robustness of the nondispersive model predictions, at least for the class of initial conditions and time scales of evolution we have focussed on, at both qualitative and, with few exceptions, quantitative levels. This is borne out of a comparison between interface profiles obtained through the numerical solutions of the two-layer model (4.3) and the direct numerical simulation of their Euler counterpart by overlaying the profile on the late time snapshots from figures 14,15,18,19, as reported in figure 20. A notable example that emerges from this comparison is the prediction of "wing" structures (simple waves for the hyperbolic models) and their locations.…”
Section: Discussionmentioning
confidence: 99%
“…Performing these computations, with extensive testing of their numerical accuracy (see also [2,10]), demonstrated a remarkable robustness of the nondispersive model predictions, at least for the class of initial conditions and time scales of evolution we have focussed on, at both qualitative and, with few exceptions, quantitative levels. This is borne out of a comparison between interface profiles obtained through the numerical solutions of the two-layer model (4.3) and the direct numerical simulation of their Euler counterpart by overlaying the profile on the late time snapshots from figures 14,15,18,19, as reported in figure 20. A notable example that emerges from this comparison is the prediction of "wing" structures (simple waves for the hyperbolic models) and their locations.…”
Section: Discussionmentioning
confidence: 99%
“…In this section, we briefly recall the derivation of the full Euler system governing the evolution equations of the two-layers flow and refer to [1,5,16,17] for more details. The two-layers flow considered are assumed to be incompressible, homogeneous, immiscible perfect fluids of different densities under the sole influence of gravity.…”
Section: Full Euler Systemmentioning
confidence: 99%
“…We refer the reader to the following papers [2,9,30,6,29]. Earlier works have also set a very interesting theoretical background for the two-fluid system see [5,1,16,17,18], for more details. One of these reduced models is the Green-Naghdi system of partial differential equations (denoted GN in the following).…”
mentioning
confidence: 99%
“…where we used Lemma A.4. Of course, one could have simply kept the surface tension term unchanged at this point, as in [20]. The smallness of surface tension, expressed by bo −1 ≤ bo −1 min , is useful in the derivation of our new model, in the following subsection.…”
Section: The Green-naghdi Modelmentioning
confidence: 99%