2020
DOI: 10.3389/fphy.2020.00032
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High Order ADER Schemes for Continuum Mechanics

Abstract: In this paper we first review the development of high order ADER finite volume and ADER discontinuous Galerkin schemes on fixed and moving meshes, since their introduction in 1999 by Toro et al. We show the modern variant of ADER based on a space-time predictor-corrector formulation in the context of ADER discontinuous Galerkin schemes with a posteriori subcell finite volume limiter on fixed and moving grids, as well as on space-time adaptive Cartesian AMR meshes. We then present and discuss the unified symmet… Show more

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Cited by 68 publications
(99 citation statements)
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“…The computational setup can be done in a fully automatic manner, without the need to generate a body-fitted structured or unstructured mesh, which can become very time consuming for complex geometries. The work presented in this paper is a natural extension of the simple diffuse interface approach introduced in [30,31,59,129] and [14]. The presented numerical algorithm with the underlying diffuse interface model is a consequent application of Godunov's shock capturing ideas to the context of moving material interfaces.…”
Section: Resultsmentioning
confidence: 99%
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“…The computational setup can be done in a fully automatic manner, without the need to generate a body-fitted structured or unstructured mesh, which can become very time consuming for complex geometries. The work presented in this paper is a natural extension of the simple diffuse interface approach introduced in [30,31,59,129] and [14]. The presented numerical algorithm with the underlying diffuse interface model is a consequent application of Godunov's shock capturing ideas to the context of moving material interfaces.…”
Section: Resultsmentioning
confidence: 99%
“…Now, the system (41), which contains only volume integrals to be calculated inside Ω i jk and no surface integrals, can be solved via a simple discrete Picard iteration for each element Ω i jk , and there is no need of any communication with neighbor elements. We recall that this procedure has been introduced for the first time in [32] for unstructured meshes, it has been extended for example to moving meshes in [7] and to degenerate space time elements in [58]; finally, its convergence has been formally proved in [14]. 10…”
Section: High Order In Time Via An Element-local Space-time Discontinmentioning
confidence: 99%
“…Furthermore, in the specific case N = 0, i.e. when the P N P M reduces to a FV scheme, the above polynomial reconstruction procedure must be made nonlinear; this can be easily done, for example, by adopting the WENO strategy specifically described in the context of P N P M type schemes (thus with the same notation adopted here) on Cartesian meshes in [25,51]. We recall that the nonlinearity introduced through ENO/WENO type procedures essentially avoids the spurious oscillations typical of high order linear schemes modeling discontin-…”
Section: High Order Spatial Reconstruction (Order M)mentioning
confidence: 99%
“…Our limiter is based on the MOOD approach [29,35,36], which has already been successfully applied in the framework of ADER finite volume schemes [21,22,85] and Discontinous Galerkin finite element schemes, see [25,47,52,75,97,124]. Specifically, the numerical solution is checked a posteriori for nonphysical values and spurious oscillations, and if it does not satisfy all admissibility detection criteria, given by both physical and numerical requirements, in a certain cell, that cell is marked as troubled.…”
Section: Introductionmentioning
confidence: 99%
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