2002
DOI: 10.1006/jcph.2001.6892
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A Technique of Treating Negative Weights in WENO Schemes

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Cited by 341 publications
(308 citation statements)
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“…The external force term f represents the gravitational force only, neglecting surface tension forces and Coriolis. The advection term is discretized with the fifth-order WENO (weighted essentially non-oscillatory) scheme (Shi et al, 2002) or the second-order TVD (total variation diminishing) Superbee scheme (Darwish and Moukalled, 2003) in separate numerical tests. The diffusion term on the right-hand side of Eq.…”
Section: Governing Equationsmentioning
confidence: 99%
See 1 more Smart Citation
“…The external force term f represents the gravitational force only, neglecting surface tension forces and Coriolis. The advection term is discretized with the fifth-order WENO (weighted essentially non-oscillatory) scheme (Shi et al, 2002) or the second-order TVD (total variation diminishing) Superbee scheme (Darwish and Moukalled, 2003) in separate numerical tests. The diffusion term on the right-hand side of Eq.…”
Section: Governing Equationsmentioning
confidence: 99%
“…The multi-material level-set method herein follows Merriman et al (1994) with the addition of high-order numerical schemes (Shu and Osher, 1989;Shi et al, 2002). The "level set" of the ith fluid is designated as φ i :…”
Section: Estimation Of Parameters For Time-dependent Coussot Modelmentioning
confidence: 99%
“…Explicit formulas for WENO coefficients on uniform meshes appear in, e.g., [7,8]. A framework for deriving WENO coefficients for non-uniform meshes is established in [7]; explicit formulas appear for uniform meshes.…”
Section: Introductionmentioning
confidence: 99%
“…WENO coefficients on arbitrary triangular meshes are derived for second-order schemes in [14] and for third-and fourth-order schemes in [15]. Computations in two dimensions with WENO discretizations are performed in [8] on triangular and rectangular meshes.…”
Section: Introductionmentioning
confidence: 99%
“…Other first and second order schemes have been applied to the SWE using the idea of balancing the source term and the flux gradients, for example the wave propagation algorithm by LeVeque [46], the kinetic scheme by Xu [62], and Perthame and Simeoni [48], central-upwind schemes proposed by Kurganov and Levy [39], and a family of flux-splitting numerical solvers proposed in [51]. It is worth pointing out that the contributions mentioned above, devoted to the numerical solution of hyperbolic problems with stiff source terms, do not address in general the question of convergence of the method, in particular when the system is singular.…”
Section: Introductionmentioning
confidence: 99%