Please use this identifier to cite or link to this item: https://doi.org/10.1063/1.1789771
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dc.titleDevelopment of boundary-layer flow in the presence of forced wavelength Görtler vortices
dc.contributor.authorMitsudharmadi, H.
dc.contributor.authorWinoto, S.H.
dc.contributor.authorShah, D.A.
dc.date.accessioned2014-10-07T09:02:37Z
dc.date.available2014-10-07T09:02:37Z
dc.date.issued2004-11
dc.identifier.citationMitsudharmadi, H., Winoto, S.H., Shah, D.A. (2004-11). Development of boundary-layer flow in the presence of forced wavelength Görtler vortices. Physics of Fluids 16 (11) : 3983-3996. ScholarBank@NUS Repository. https://doi.org/10.1063/1.1789771
dc.identifier.issn10706631
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/84984
dc.description.abstractHot-wire measurements in the boundary layer developing on a concave surface of 2.0 m radius of curvature in the presence of forced wavelength Görtler vortices have been conducted for a free-stream velocity of 3.0 m/s. The wavelengths of vortices were preset by vertical perturbation wires of 0.2 mm diameter located 10 mm upstream of the concave surface leading edge. The velocity contours in the cross-sectional planes at several streamwise locations show the growth and breakdown of the vortices that are similar to those found in the transitional flow field. It shows the occurrence of the second instability mode that is indicated by the formation of small horseshoe eddies generated between the two neighboring vortices traveling in the streamwise direction to form mushroom-like structures as a consequence of the nonlinear growth of the Görtler vortices. The breakdown of these structures before the boundary-layer flow becomes turbulent is also shown to qualitatively predict the start of the transition in the flow. The Görtler number where the start of the transition was predicted is found to be within the range of transitional Görtler numbers previously reported for naturally developed Görtler vortices. The average of the spanwise wavelength after being normalized by v/u τ, is comparable with the generally quoted value of 100 for turbulent boundary layers. © 2004 American Institute of Physics.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1063/1.1789771
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.description.doi10.1063/1.1789771
dc.description.sourcetitlePhysics of Fluids
dc.description.volume16
dc.description.issue11
dc.description.page3983-3996
dc.description.codenPHFLE
dc.identifier.isiut000224456800017
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