Mean velocity and turbulence measurements of flow around a 6:1 prolate spheroid

dc.contributor.authorBarber, Kevin Michaelen
dc.contributor.committeechairSimpson, Roger L.en
dc.contributor.committeememberWalker, Dana A.en
dc.contributor.committeememberDevenport, William J.en
dc.contributor.departmentAerospace Engineeringen
dc.date.accessioned2014-03-14T21:31:04Zen
dc.date.adate2009-03-12en
dc.date.available2014-03-14T21:31:04Zen
dc.date.issued1990-05-05en
dc.date.rdate2009-03-12en
dc.date.sdate2009-03-12en
dc.description.abstractInvestigations of the three-dimensional flow around a 6:1 prolate spheroid model 1.37 m long were conducted in the separation and near wake regions along the leeward side. Mean velocity flow field measurements, at α = 10∘ and 15∘ , and at Re = 1.3 x 10⁶ (U<sub>re</sub>= 15.2 mls) and 4.0x 10⁶ (Ure=45.7 m/s), were obtained at four axial locations along the afterbody. Boundary layer profiles and Reynolds shear stress measurements were obtained at two axial locations, with a = 100 and Re=4.0 X 10⁶. Results of the flow field measurements indicate vortical flow along the surface of the body, growing in strength with increasing Reynolds number and increasing angle of attack. Skewing of the three-dimensional boundary layer is seen in the boundary layer profiles, with the surface shear stress direction lagging the local free-stream velocity direction. Growth of the boundary layer is evident circumferentially and axially along the body. Results of the turbulence measurements show that the distribution of Reynolds stress quantities is different from that of a two-dimensional flow over a flat plate, due to the three-dimensional flow and separation that is present. Estimates of x and z eddy viscosities show that the eddy viscosity is not isotropic. Estimates of the mixing length compared to values for a two-dimensional flow model indicate that the model predicts high values for the mixing length. Comparisons made with results obtained at DFVLR in West Germany show good agreement for the mean velocity and Reynolds normal stress values; however, the agreement of the Reynolds shear stresses is not as good.en
dc.description.degreeMaster of Scienceen
dc.format.extentxxvii, 228 leavesen
dc.format.mediumBTDen
dc.format.mimetypeapplication/pdfen
dc.identifier.otheretd-03122009-040424en
dc.identifier.sourceurlhttp://scholar.lib.vt.edu/theses/available/etd-03122009-040424/en
dc.identifier.urihttp://hdl.handle.net/10919/41446en
dc.language.isoenen
dc.publisherVirginia Techen
dc.relation.haspartLD5655.V855_1990.B372.pdfen
dc.relation.isformatofOCLC# 22606637en
dc.rightsIn Copyrighten
dc.rights.urihttp://rightsstatements.org/vocab/InC/1.0/en
dc.subject.lccLD5655.V855 1990.B372en
dc.subject.lcshAir flow -- Researchen
dc.subject.lcshBoundary layer -- Researchen
dc.subject.lcshTurbulence -- Researchen
dc.titleMean velocity and turbulence measurements of flow around a 6:1 prolate spheroiden
dc.typeThesisen
dc.type.dcmitypeTexten
thesis.degree.disciplineAerospace Engineeringen
thesis.degree.grantorVirginia Polytechnic Institute and State Universityen
thesis.degree.levelmastersen
thesis.degree.nameMaster of Scienceen
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