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dc.contributor.authorTyvand, Peder A.
dc.contributor.authorNøland, Jonas Kristiansen
dc.date.accessioned2021-10-20T09:16:05Z
dc.date.available2021-10-20T09:16:05Z
dc.date.created2020-03-19T00:43:00Z
dc.date.issued2020
dc.identifier.citationTransport in Porous Media. 2020, 132 (3), 535-559.en_US
dc.identifier.issn0169-3913
dc.identifier.urihttps://hdl.handle.net/11250/2824048
dc.description.abstractThe analytical theory on Darcy–Bénard convection is dominated by normal-mode approaches, which essentially reduce the spatial order from four to two. This paper goes beyond the normal-mode paradigm of convection onset in a porous rectangle. A handpicked case where all four corners of the rectangle are non-analytical is therefore investigated. The marginal state is oscillatory with one-way horizontal wave propagation. The time-periodic convection pattern has no spatial periodicity and requires heavy numerical computation by the finite element method. The critical Rayleigh number at convection onset is computed, with its associated frequency of oscillation. Snapshots of the 2D eigenfunctions for the flow field and temperature field are plotted. Detailed local gradient analyses near two corners indicate that they hide logarithmic singularities, where the displayed eigenfunctions may represent outer solutions in matched asymptotic expansions. The results are validated with respect to the asymptotic limit of Nield (Water Resour Res 11:553–560, 1968).en_US
dc.language.isoengen_US
dc.relation.urihttps://link.springer.com/article/10.1007/s11242-020-01403-2
dc.titleOscillatory Convection Onset in a Porous Rectangle with Non-analytical Cornersen_US
dc.typeJournal articleen_US
dc.typePeer revieweden_US
dc.description.versionpublishedVersionen_US
dc.source.pagenumber535-559en_US
dc.source.volume132en_US
dc.source.journalTransport in Porous Mediaen_US
dc.source.issue3en_US
dc.identifier.doi10.1007/s11242-020-01403-2
dc.identifier.cristin1802322
cristin.ispublishedtrue
cristin.fulltextpostprint
cristin.qualitycode2


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