Derivation of a new two-dimensional viscous shallow water model with varying topography, bottom friction and capillary effects
By Fabien Marche. 2007
215 citations recorded by the source corpus.
Subfields: Applied Mathematics, Computational Mechanics, Oceanography
View Paper: https://www.semanticscholar.org/paper/baac818a8f84e63c5b60100fba054574b17ba9c4
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Applied Mathematics
- Zhouping Xin
- Alexis Vasseur
- Cheng Yu
- Jing Li
- Didier Bresch
- Marie-Odile Bristeau
- Emmanuel Audusse
- B. Desjardins
In Computational Mechanics
- Zhouping Xin
- Marie-Odile Bristeau
- Didier Bresch
- Alexis Vasseur
- B. Desjardins
- Jacques Sainte-Marie
- Emmanuel Audusse
- Jing Li
In Oceanography
- Cheng Yu
- Jacques Sainte-Marie
- Alexis Vasseur
- Didier Bresch
- Emmanuel Audusse
- Benoit Perthame
- Marie-Odile Bristeau
- Zhouping Xin
Citations in the corpus
- Existence of global weak solutions for 3D degenerate compressible Navier–Stokes equations (2015, result): “[25] F. Marche, Derivation of a new two-dimensional viscous shallow water model with varying topography, bottom friction and capillary effects.”
- Global Existence of Weak Solutions to the Barotropic Compressible Navier-Stokes Flows with Degenerate Viscosities (2015, background): “Recently, a friction shallow-water system, with flat bottom topography, which is derived in [5, 6, 9, 28], can be written in a two-dimensional space domain Ω as (1.”
- A multilayer Saint-Venant system with mass exchanges for shallow water flows. Derivation and numerical validation* (2009, methodology): “zb u dz, it is well known [11,16,18,20] that the shallow water system (3.”
- On the construction of approximate solutions for the 2D viscous shallow water model and for compressible Navier-Stokes models (2006, background): “Let us emphasize that the stress tensor obtained from a formal derivation of the Saint–Venant model in 2d requires to deal with 2νhD(u)+2ν∇(hdivu), see [11], which at the moment cannot be treated by the present work.”