2020
DOI: 10.1016/j.jcp.2019.109167
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High order direct Arbitrary-Lagrangian-Eulerian schemes on moving Voronoi meshes with topology changes

Abstract: We present a new family of very high order accurate direct Arbitrary-Lagrangian-Eulerian (ALE) Finite Volume (FV) and Discontinuous Galerkin (DG) schemes for the solution of nonlinear hyperbolic PDE systems on moving Voronoi meshes that are regenerated at each time step and which explicitly allow topology changes in time. The Voronoi tessellations are obtained from a set of generator points that move with the local fluid velocity. We employ an AREPOtype approach [1], which rapidly rebuilds a new high quality m… Show more

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Cited by 91 publications
(72 citation statements)
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References 263 publications
(495 reference statements)
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“…Space-time predictor for sliver space-time elements When a topology change occurs, some space-time sliver elements, as those shown on the right side of Figure 8, are originated (see [90]), and the predictor procedure over them needs particular care. The problem Figure 8: Space time connectivity with topology changes and sliver element.…”
Section: Simplification In the Case Of A Fixed Cartesian Meshmentioning
confidence: 99%
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“…Space-time predictor for sliver space-time elements When a topology change occurs, some space-time sliver elements, as those shown on the right side of Figure 8, are originated (see [90]), and the predictor procedure over them needs particular care. The problem Figure 8: Space time connectivity with topology changes and sliver element.…”
Section: Simplification In the Case Of A Fixed Cartesian Meshmentioning
confidence: 99%
“…Left: at time t n the polygons P n 2 and P n 3 are neighbors and share the highlighted edge, instead at time t n+1 they do not touch each other; the opposite situation occurs for polygons P n 1 and P n 4 . This change of topology causes the appearance of degenerate elements of different types (refer to [90] for all the details). In particular, so-called space-time sliver elements (right) need to be taken into account when considering the space-time framework, so the predictor and the corrector step have to be a adapted to their special features.…”
Section: Simplification In the Case Of A Fixed Cartesian Meshmentioning
confidence: 99%
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“…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%
“…[17,5,13,11,7,10,9,12,15,16,14,49,65]. However, much less is known so far on the construction of arbitrary high order accurate exactly divergence-preserving schemes on general polygonal and polyhedral meshes [67,41,26], or on general space-trees with arbitrary refinement factor r, see e.g. [38].…”
Section: Hyperbolic Curl Cleaning With An Extended Generalized Lagranmentioning
confidence: 99%