Please use this identifier to cite or link to this item: https://doi.org/10.1002/fld.1899
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dc.titleA numerical technique for laminar swirling flow at the interface between porous and homogenous fluid domains
dc.contributor.authorYu, P.
dc.contributor.authorLee, T.S.
dc.contributor.authorZeng, Y.
dc.contributor.authorMeguid, S.A.
dc.contributor.authorLow, H.T.
dc.date.accessioned2014-06-16T09:33:42Z
dc.date.available2014-06-16T09:33:42Z
dc.date.issued2009-05-30
dc.identifier.citationYu, P., Lee, T.S., Zeng, Y., Meguid, S.A., Low, H.T. (2009-05-30). A numerical technique for laminar swirling flow at the interface between porous and homogenous fluid domains. International Journal for Numerical Methods in Fluids 60 (3) : 337-353. ScholarBank@NUS Repository. https://doi.org/10.1002/fld.1899
dc.identifier.issn02712091
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/54685
dc.description.abstractThere have been a few recent numerical implementations of the stress-jump condition at the interface of conjugate flows, which couple the governing equations for flows in the porous and homogenous fluid domains. These previous demonstration cases were for two-dimensional, planar flows with simple geometries, for example, flow over a porous layer or flow through a porous plug. The present study implements the interfacial stress-jump condition for a non-planar flow with three velocity components, which is more realistic in terms of practical flow applications. The steady, laminar, Newtonian flow in a stirred micro-bioreactor with a porous scaffold inside was investigated. It is shown how to implement the interfacial jump condition on the radial, axial, and swirling velocity components. To avoid a full threedimensional simulation, the flow is assumed to be independent of the azimuthal direction, which makes it an axisymmetric flow with a swirling velocity. The present interface treatment is suitable for non-flat surfaces, which is achieved by applying the finite volume method based on body-fitted and multi-block grids. The numerical simulations show that a vortex breakdown bubble, attached to the free surface, occurs above a certain Reynolds number. The presence of the porous scaffold delays the onset of vortex breakdown and confines it to a region above the scaffold. Copyright © 2008 John Wiley & Sons, Ltd.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1002/fld.1899
dc.sourceScopus
dc.subjectBlock-structured grids
dc.subjectPorous medium
dc.subjectPorous-fluid interface
dc.subjectStress jump
dc.subjectSwirling flow
dc.subjectTissue-engineering scaffold
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.contributor.departmentTEMASEK LABORATORIES
dc.description.doi10.1002/fld.1899
dc.description.sourcetitleInternational Journal for Numerical Methods in Fluids
dc.description.volume60
dc.description.issue3
dc.description.page337-353
dc.description.codenIJNFD
dc.identifier.isiut000265996700006
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