2010
DOI: 10.1002/fld.2392
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Central WENO scheme for the integral form of contravariant shallow‐water equations

Abstract: A new Central Weighted Essentially Non-Oscillatory scheme for the solution of the shallow-water equations expressed in contravariant formulation is presented. One of the most efficient methodologies belonging to Central WENO family involves: reconstructions of cell-averaged values of flow variables, reconstruction of point-values of flow variables, advancing from time level t(n) to time level t(n+1) of the cell-averaged values. The extension of the above-mentioned methodology into the contravariant environment… Show more

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Cited by 17 publications
(12 citation statements)
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“…Expressions for terms s l , V l ,V l , T l and W l are given in Appendix A. Equations (5) and (6) represent the integral expressions of the FNBEs in contravariant formulation in which Christoffel symbols are absent. The procedure for the formulation of the above-mentioned contravariant integral equations is clarified in Gallerano and Cannata [2011a]. These equations are accurate to O(µ 2 ) and O(εµ 2 ) in dispersive terms and retain the conservation of potential vorticity up to O(µ 2 ), in accordance with the formulation proposed by Gallerano et al [2014].…”
Section: Hydrodynamic Modelmentioning
confidence: 93%
“…Expressions for terms s l , V l ,V l , T l and W l are given in Appendix A. Equations (5) and (6) represent the integral expressions of the FNBEs in contravariant formulation in which Christoffel symbols are absent. The procedure for the formulation of the above-mentioned contravariant integral equations is clarified in Gallerano and Cannata [2011a]. These equations are accurate to O(µ 2 ) and O(εµ 2 ) in dispersive terms and retain the conservation of potential vorticity up to O(µ 2 ), in accordance with the formulation proposed by Gallerano et al [2014].…”
Section: Hydrodynamic Modelmentioning
confidence: 93%
“…which Christoffel symbols are absent. This result has been achieved by adopting the procedure proposed by Gallerano and Cannata (2011) for the depth-averaged motion equations and extended to the three-dimensional motion equations by Cannata et al (2019). According to this procedure, the integral form of the vectorial momentum balance equation is projected onto the directions of the contravariant base vectors defined at the centre of the curvilinear control volume.…”
Section: Governing Equationsmentioning
confidence: 99%
“…In order to overcome this drawback, we propose the Boussinesq equations in contravariant formulation without the Christoffel symbols. We equate the net force to the material volume momentum rate of change in a direction defined by a parallel vector field (Gallerano & Cannata, 2011) Figure 1 a graphic sketch of the generic surface element A in the curvilinear coordinate system is shown. In this figure, a pair of covariant base vectors b (1) , b (2) and a pair of contravariant base vectors…”
Section: Hydrodynamic Modelmentioning
confidence: 99%