Please use this identifier to cite or link to this item: https://doi.org/10.1007/s00348-003-0733-7
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dc.titleA flow field study of an elliptic jet in cross flow using DPIV technique
dc.contributor.authorNew, T.H.
dc.contributor.authorLim, T.T.
dc.contributor.authorLuo, S.C.
dc.date.accessioned2014-06-16T09:28:11Z
dc.date.available2014-06-16T09:28:11Z
dc.date.issued2004-04
dc.identifier.citationNew, T.H., Lim, T.T., Luo, S.C. (2004-04). A flow field study of an elliptic jet in cross flow using DPIV technique. Experiments in Fluids 36 (4) : 604-618. ScholarBank@NUS Repository. https://doi.org/10.1007/s00348-003-0733-7
dc.identifier.issn07234864
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/54157
dc.description.abstractThe digital particle image velocimetry (DPIV) technique has been used to investigate the flow fields of an elliptic jet in cross flow (EJICF). Two different jet orientations are considered; one with the major axis of the ellipse aligned with the cross flow (henceforth referred to as a low aspect ratio (AR) jet), and the other with the major axis normal to the cross flow (henceforth referred to as a high aspect ratio jet). Results show that the vortex-pairing phenomenon is prevalent in the low aspect ratio jet when the velocity ratio (VR)≥3, and is absent in the high aspect ratio jet regardless of the velocity ratio. The presence of vortex pairing leads to a substantial increase in the leading-edge peak vorticity compared to the lee-side vorticity, which suggests that vortex pairing may play an important role in the entrainment of ambient fluid into the jet body, at least in the near-field region. In the absence of vortex pairing, both the leading-edge and the lee-side peak vorticity increase monotonically with velocity ratio regardless of the aspect ratio. Moreover, time-averaged velocity fields for both AR=0.5 and AR=2 jets reveal the existence of an "unstable focus" (UF) downstream of the jet, at least for VR≥2. The strength and the location of this focus is a function of both the velocity ratio and aspect ratio. In addition, time-averaged vorticity fields show a consistently higher peak-averaged vorticity in the low aspect ratio jet than in the high aspect ratio jet. This behavior could be due to a higher curvature of the vortex filament facing the cross flow in the low aspect ratio jet, which through mutual interaction may lead to higher vortex stretching, and therefore higher peak-averaged vorticity.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1007/s00348-003-0733-7
dc.sourceScopus
dc.typeArticle
dc.contributor.departmentMECHANICAL ENGINEERING
dc.contributor.departmentTEMASEK LABORATORIES
dc.description.doi10.1007/s00348-003-0733-7
dc.description.sourcetitleExperiments in Fluids
dc.description.volume36
dc.description.issue4
dc.description.page604-618
dc.description.codenEXFLD
dc.identifier.isiut000220937300010
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