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dc.contributor.authorJaiswal, Bharat Raj
dc.contributor.authorGupta, B. R.
dc.date.accessioned2015-02-13T07:22:16Z
dc.date.available2015-02-13T07:22:16Z
dc.date.issued2014
dc.identifier.citationApplied and Computational Mechanics. 2014, vol. 8, no. 2, p. 157-176.en
dc.identifier.issn1803-680X (Print)
dc.identifier.issn2336-1182 (Online)
dc.identifier.urihttp://www.kme.zcu.cz/acm/acm/article/view/268/300
dc.identifier.urihttp://hdl.handle.net/11025/11955
dc.description.abstractAn analysis is carried out to study the flow characteristics of creeping motion of an inner non-Newtonian Reiner-Rivlin liquid spheroid r = 1+ ∑k=2∞αkGk(cos θ), here αk is very small shape factor and Gk is Gegenbauer function of first kind of order k, at the instant it passes the centre of a rigid spherical container filled with a Newtonian fluid. The shape of the liquid spheroid is assumed to depart a bit at its surface from the shape a sphere. The analytical expression for stream function solution for the flow in spherical container is obtained by using Stokes equation. While for the flow inside the Reiner-Rivlin liquid spheroid, the expression for stream function is obtained by expressing it in a power series of S, characterizing the cross-viscosity of Reiner-Rivlin fluid. Both the flow fields are then determined explicitly by matching the boundary conditions at the interface of Newtonian fluid and non-Newtonian fluid and also the condition of impenetrability and no-slip on the outer surface to the first order in the small parameter ε, characterizing the deformation of the liquid sphere. As an application, we consider an oblate liquid spheroid r = 1+2εG2(cos θ) and the drag and wall effects on the body are evaluated. Their variations with regard to separation parameter, viscosity ratio λ, cross-viscosity, i.e., S and deformation parameter are studied and demonstrated graphically. Several well-noted cases of interest are derived from the present analysis. Attempts are made to compare between Newtonian and Reiner-Rivlin fluids which yield that the cross-viscosity μc is to decrease the wall effects K and to increase the drag DN when deformation is comparatively small. It is  observed that drag not only varies with λ, but as η increases, the rate of change in behavior of drag force increases also.en
dc.format20 s.cs
dc.format.mimetypeapplication/pdf
dc.language.isoenen
dc.publisherUniversity of West Bohemiaen
dc.relation.ispartofseriesApplied and Computational Mechanicsen
dc.rights© 2014 University of West Bohemia. All rights reserved.en
dc.subjectReiner-Rivlinova kapalinacs
dc.subjectGegenbauerova funkcecs
dc.subjectproudová funkcecs
dc.subjectsféroidcs
dc.subjecttažná sílacs
dc.subjectfaktor korekce stěnycs
dc.subjectsférický kontejnercs
dc.titleWall effects on Reiner-Rivlin liquid spheroiden
dc.typečlánekcs
dc.typearticleen
dc.rights.accessopenAccessen
dc.type.versionpublishedVersionen
dc.subject.translatedReiner-Rivlin fluiden
dc.subject.translatedGegenbauer functionen
dc.subject.translatedstream functionsen
dc.subject.translatedspheroiden
dc.subject.translateddrag forceen
dc.subject.translatedwall correction factoren
dc.subject.translatedspherical containeren
dc.type.statusPeer-revieweden
Appears in Collections:Volume 8, number 2 (2014)
Volume 8, number 2 (2014)

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