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dc.contributor.authorPrebeg, Marin
dc.date.accessioned2019-11-14T11:51:58Z
dc.date.available2019-11-14T11:51:58Z
dc.date.created2018-12-10T13:41:02Z
dc.date.issued2018
dc.identifier.citationSpringer Proceedings in Mathematics & statistics. 2018, 237 479-490.nb_NO
dc.identifier.issn2194-1017
dc.identifier.urihttp://hdl.handle.net/11250/2628526
dc.description.abstractWe consider Large Time Step (LTS) methods, i.e., the explicit finite volume methods not limited by the Courant–Friedrichs–Lewy (CFL) condition. The original LTS method (LeVeque in SIAM J Numer Anal 22, 1985) was constructed as an extension of the Godunov scheme, and successive versions have been developed in the framework of Roe’s approximate Riemann solver. Recently, Prebeg et al. (in ESAIM: M2AN, in press, 2017) developed the LTS extension of the HLL and HLLC schemes. We perform the modified equation analysis and demonstrate that for the appropriate choice of the wave velocity estimates, the LTS-HLL scheme yields entropy-satisfying solutions. We apply the LTS-HLL(C) schemes to the one-dimensional Euler equations and consider the Sod shock tube, double rarefaction, and Woodward–Colella blast-wave problem.nb_NO
dc.language.isoengnb_NO
dc.publisherSpringer Verlagnb_NO
dc.titleNumerical viscosity in large time step hll-type schemesnb_NO
dc.typeJournal articlenb_NO
dc.typePeer reviewednb_NO
dc.description.versionacceptedVersionnb_NO
dc.source.pagenumber479-490nb_NO
dc.source.volume237nb_NO
dc.source.journalSpringer Proceedings in Mathematics & statisticsnb_NO
dc.identifier.doi10.1007/978-3-319-91548-7_36
dc.identifier.cristin1641143
dc.description.localcodeThis is a post-peer-review, pre-copyedit version of an article published in [Springer Proceedings in Mathematics & statistics ]. The final authenticated version is available online at: https://doi.org/10.1007/978-3-319-91548-7_36nb_NO
cristin.unitcode194,64,25,0
cristin.unitnameInstitutt for energi- og prosessteknikk
cristin.ispublishedtrue
cristin.fulltextpreprint
cristin.qualitycode1


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