Matches in SemOpenAlex for { <https://semopenalex.org/work/W2023853370> ?p ?o ?g. }
- W2023853370 endingPage "270" @default.
- W2023853370 startingPage "247" @default.
- W2023853370 abstract "In the present work, a high order realizable scheme for the Eulerian simulation of disperse phase flows on unstructured grids is developed and tested. In the Eulerian modeling framework two approaches are studied: the monokinetic (MK) [1] and the Gaussian closures [2, 3]. The former leads to a pressureless gas dynamics system (PGD). It accurately reproduces the physics of such flows at low Stokes number, but is challenging for numerics since the resulting system is weakly hyperbolic. The latter deals with higher Stokes numbers by accounting for particle trajectory crossings (PTC) [4]. Compared to the MK closure, the resulting system of equation is hyperbolic but has a more complex structure; realizability conditions are satisfied at the continuous level, which imply a precise framework for numerical methods. To achieve the goals of accuracy, robustness and realizability, the Discontinuous Galerkin method (DG) is a promising numerical approach [5, 6, 7, 8]. Based on the recent work of Zhang et al. [6], the DG method used is associated to a convex projection strategy, which respects the realizability constraints without affecting the accuracy. The main contribution of this work is to apply one of the latest developments in the field of numerical methods (DG) to physical models, taking into account the free transport and drag terms of the disperse phase flow, which are the building blocks for the Eulerian modeling based on moment methods. DG results are eventually compared qualitatively and quantitatively to the Lagrangian results and to the reference simulations provided by a second order structured MUSCL/HLL finite volume scheme [9, 3]. Through these comparisons, the DG method is shown to be competitive for the description of such flows." @default.
- W2023853370 created "2016-06-24" @default.
- W2023853370 creator A5028947795 @default.
- W2023853370 creator A5035669382 @default.
- W2023853370 creator A5046573369 @default.
- W2023853370 creator A5055196143 @default.
- W2023853370 date "2014-09-01" @default.
- W2023853370 modified "2023-10-09" @default.
- W2023853370 title "On the Development of High Order Realizable Schemes for the Eulerian Simulation of Disperse Phase Flows: A Convex-State Preserving Discontinuous Galerkin Method" @default.
- W2023853370 cites W1555627060 @default.
- W2023853370 cites W193373252 @default.
- W2023853370 cites W1966241802 @default.
- W2023853370 cites W1971818437 @default.
- W2023853370 cites W1977665684 @default.
- W2023853370 cites W1983162060 @default.
- W2023853370 cites W1983178362 @default.
- W2023853370 cites W1990187415 @default.
- W2023853370 cites W1991573831 @default.
- W2023853370 cites W1993298250 @default.
- W2023853370 cites W1994955324 @default.
- W2023853370 cites W2002892388 @default.
- W2023853370 cites W2005027835 @default.
- W2023853370 cites W2008956940 @default.
- W2023853370 cites W2011702259 @default.
- W2023853370 cites W2021517416 @default.
- W2023853370 cites W2041342863 @default.
- W2023853370 cites W2043057066 @default.
- W2023853370 cites W2049098006 @default.
- W2023853370 cites W2055380691 @default.
- W2023853370 cites W2056994727 @default.
- W2023853370 cites W2063735786 @default.
- W2023853370 cites W2065812865 @default.
- W2023853370 cites W2076565801 @default.
- W2023853370 cites W2082335044 @default.
- W2023853370 cites W2085961649 @default.
- W2023853370 cites W2090020940 @default.
- W2023853370 cites W2091178963 @default.
- W2023853370 cites W2112548197 @default.
- W2023853370 cites W2143008187 @default.
- W2023853370 cites W2162728998 @default.
- W2023853370 cites W2963311102 @default.
- W2023853370 cites W4210886888 @default.
- W2023853370 cites W4378673242 @default.
- W2023853370 doi "https://doi.org/10.1260/1757-482x.6.3.247" @default.
- W2023853370 hasPublicationYear "2014" @default.
- W2023853370 type Work @default.
- W2023853370 sameAs 2023853370 @default.
- W2023853370 citedByCount "12" @default.
- W2023853370 countsByYear W20238533702015 @default.
- W2023853370 countsByYear W20238533702016 @default.
- W2023853370 countsByYear W20238533702017 @default.
- W2023853370 countsByYear W20238533702019 @default.
- W2023853370 countsByYear W20238533702020 @default.
- W2023853370 countsByYear W20238533702023 @default.
- W2023853370 crossrefType "journal-article" @default.
- W2023853370 hasAuthorship W2023853370A5028947795 @default.
- W2023853370 hasAuthorship W2023853370A5035669382 @default.
- W2023853370 hasAuthorship W2023853370A5046573369 @default.
- W2023853370 hasAuthorship W2023853370A5055196143 @default.
- W2023853370 hasBestOaLocation W20238533701 @default.
- W2023853370 hasConcept C11413529 @default.
- W2023853370 hasConcept C121332964 @default.
- W2023853370 hasConcept C126255220 @default.
- W2023853370 hasConcept C134306372 @default.
- W2023853370 hasConcept C135628077 @default.
- W2023853370 hasConcept C2776378722 @default.
- W2023853370 hasConcept C2778770139 @default.
- W2023853370 hasConcept C28826006 @default.
- W2023853370 hasConcept C33923547 @default.
- W2023853370 hasConcept C41008148 @default.
- W2023853370 hasConcept C43058520 @default.
- W2023853370 hasConcept C53469067 @default.
- W2023853370 hasConcept C73000952 @default.
- W2023853370 hasConcept C92244383 @default.
- W2023853370 hasConcept C97355855 @default.
- W2023853370 hasConceptScore W2023853370C11413529 @default.
- W2023853370 hasConceptScore W2023853370C121332964 @default.
- W2023853370 hasConceptScore W2023853370C126255220 @default.
- W2023853370 hasConceptScore W2023853370C134306372 @default.
- W2023853370 hasConceptScore W2023853370C135628077 @default.
- W2023853370 hasConceptScore W2023853370C2776378722 @default.
- W2023853370 hasConceptScore W2023853370C2778770139 @default.
- W2023853370 hasConceptScore W2023853370C28826006 @default.
- W2023853370 hasConceptScore W2023853370C33923547 @default.
- W2023853370 hasConceptScore W2023853370C41008148 @default.
- W2023853370 hasConceptScore W2023853370C43058520 @default.
- W2023853370 hasConceptScore W2023853370C53469067 @default.
- W2023853370 hasConceptScore W2023853370C73000952 @default.
- W2023853370 hasConceptScore W2023853370C92244383 @default.
- W2023853370 hasConceptScore W2023853370C97355855 @default.
- W2023853370 hasIssue "3" @default.
- W2023853370 hasLocation W20238533701 @default.
- W2023853370 hasLocation W20238533702 @default.
- W2023853370 hasLocation W20238533703 @default.
- W2023853370 hasLocation W20238533704 @default.
- W2023853370 hasLocation W20238533705 @default.
- W2023853370 hasOpenAccess W2023853370 @default.
- W2023853370 hasPrimaryLocation W20238533701 @default.