2010
DOI: 10.1016/j.cma.2009.10.016
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FORCE schemes on unstructured meshes II: Non-conservative hyperbolic systems

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Cited by 143 publications
(150 citation statements)
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“…An other possibility in approaching the matrix A i+1/2 is to use the technique proposed in [31,32,33]. In order to compute an approximation of the Roe linearization for the family of segments we should have…”
Section: Numerical Approach By Finite Volume Methodsmentioning
confidence: 99%
“…An other possibility in approaching the matrix A i+1/2 is to use the technique proposed in [31,32,33]. In order to compute an approximation of the Roe linearization for the family of segments we should have…”
Section: Numerical Approach By Finite Volume Methodsmentioning
confidence: 99%
“…The resulting PDE system is solved by a high order path-conservative WENO finite volume scheme on unstructured triangular meshes, to be applicable also in complex geometries. To assure low numerical dissipation at the free surface, which actually is crucial for the applications under consideration here, we use the new generalized Osher-type scheme of Dumbser and Toro [29], which resolves steady shear and contact waves exactly, in contrast to the simpler centered path-conservative FORCE schemes presented in [26].…”
Section: Introductionmentioning
confidence: 99%
“…The resulting PDE system is solved by a high order path-conservative WENO finite volume scheme on unstructured triangular meshes, to be applicable also in complex geometries. To assure low numerical dissipation at the free surface, which actually is crucial for the applications under consideration here, we use the new generalized Osher-type scheme of Dumbser and Toro [29], which resolves steady shear and contact waves exactly, in contrast to the simpler centered path-conservative FORCE schemes presented in [26].The model derives directly from first principles, namely the conservation of mass and momentum, hence it does not make any of the classical simplifications inherent in the commonly used shallow water models, which are based on depth-averaging, neglecting accelerations in gravity directions and on the resulting hydrostatic pressure distribution. We validate the new two-phase model against available analytical, numerical and experimental reference solutions and we also show some comparisons with the classical shallow water model for typical dambreak-type problems.…”
mentioning
confidence: 99%
“…In order to achieve high order of accuracy also in time we adopt the Lagrangian version of the local space-time discontinuous Galerkin method [9,10], first introduced for the Eulerian framework in [34,36,37,47]. The reconstructed polynomials w h (x, t n ) computed at the current time t n are evolved within one time step locally for each element T i (t) without requiring any neighbor information.…”
Section: Local Space-time Galerkin Predictor On Moving Unstructured Mmentioning
confidence: 99%
“…In [8][9][10][11]35] each lateral space-time sub-volume ∂C n i j has been mapped to a reference element ∂C E defined on a local reference system (χ 1 , χ 2 , τ ) and then parametrized with a set of bilinear (in 2D) or trilinear (in 3D) basis functions β k (χ 1 , χ 2 , τ ). The flux integral appearing in (37) has been computed on the reference element ∂C E using multidimensional Gaussian quadrature rules of suitable order of accuracy, see [76] for details. Since such a parametrization is not linear, the outward pointing normal vectorñ as well as the Jacobian of the transformation between ∂C n i j and ∂C E are not constant.…”
Section: Quadrature-free Finite Volume Scheme On Moving Meshesmentioning
confidence: 99%