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dc.contributor.authorKaoullas, G.en
dc.contributor.authorGeorgiou, Georgios C.en
dc.creatorKaoullas, G.en
dc.creatorGeorgiou, Georgios C.en
dc.date.accessioned2019-12-02T10:35:53Z
dc.date.available2019-12-02T10:35:53Z
dc.date.issued2013
dc.identifier.urihttp://gnosis.library.ucy.ac.cy/handle/7/57009
dc.description.abstractThe Newtonian Poiseuille flow is considered for various geometries, under the assumption that wall slip occurs above a critical value of the wall shear stress known as, the slip yield stress. In the axisymmetric and planar cases, there are two flow regimes defined by a critical value of the pressure gradient above which slip occurs. Two critical pressure gradients characterise the annular and rectangular Poiseuille flows. Below the first critical value no-slip occurs while above the second-one, slip occurs at all walls. In the intermediate regime for the annular problem, slip occurs only at the inner-wall, while for the rectangular problem, there are two intermediate regimes for which there are no analytical solutions. In the first regime slip occurs only in the middle sections of the wider walls and in the second-one partial slip also occurs along the narrower walls. Analytical solutions of all flow problems (with the exception of the two intermediate regimes of the rectangular Poiseuille case) are derived and discussed. © 2013 Elsevier B.V.en
dc.sourceJournal of Non-Newtonian Fluid Mechanicsen
dc.source.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84876400893&doi=10.1016%2fj.jnnfm.2013.02.005&partnerID=40&md5=d2b2828d8f1bbd0fdff2332cf7c5b0e6
dc.subjectYield stressen
dc.subjectCritical valueen
dc.subjectMathematical techniquesen
dc.subjectWall shear stressen
dc.subjectPoiseuille flowen
dc.subjectSlip yield stressen
dc.subjectNavier slipen
dc.subjectNewtonian fluiden
dc.subjectIntermediate regimesen
dc.subjectNewtonian fluidsen
dc.subjectPressure gradienten
dc.subjectMiddle sectionen
dc.subjectTwo flow regimesen
dc.titleNewtonian Poiseuille flows with slip and non-zero slip yield stressen
dc.typeinfo:eu-repo/semantics/article
dc.identifier.doi10.1016/j.jnnfm.2013.02.005
dc.description.volume197
dc.description.startingpage24
dc.description.endingpage30
dc.author.facultyΣχολή Θετικών και Εφαρμοσμένων Επιστημών / Faculty of Pure and Applied Sciences
dc.author.departmentΤμήμα Μαθηματικών και Στατιστικής / Department of Mathematics and Statistics
dc.type.uhtypeArticleen
dc.description.notes<p>Cited By :12</p>en
dc.source.abbreviationJ.Non-Newton.Fluid Mech.en
dc.contributor.orcidKaoullas, G. [0000-0003-0498-7896]
dc.contributor.orcidGeorgiou, Georgios C. [0000-0002-7451-224X]
dc.gnosis.orcid0000-0003-0498-7896
dc.gnosis.orcid0000-0002-7451-224X


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