2013
DOI: 10.1063/1.4801849
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Energy contents and vortex dynamics in Mode-C transition of wired-cylinder wake

Abstract: The 3D transition of the flow behind a circular cylinder with a near-wake wire disturbance has been investigated experimentally. The flow is oriented horizontally and the wire is positioned in the upper half of the wake. We performed flow visualization and particle image velocimetry experiments to investigate the influence of the wire on various properties of the flow, such as the dynamics of the spanwise structures. Experiments were performed in the Reynolds number range of Re = 165–300. It is shown that in M… Show more

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Cited by 9 publications
(4 citation statements)
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References 30 publications
(35 reference statements)
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“…The λ C values obtained in the present case are similar to those reported in the literature, e.g. λ C = 1.8D and 2.2D for flow past a circular cylinder with a trip-wire in the near wake by Zhang et al (1995) and Yildirim et al (2013b), respectively, and λ C ~ 1.7D for flow past a circular ring (Sheard et al, 2003).…”
Section: Wake Structure and Transition Mechanismsupporting
confidence: 89%
“…The λ C values obtained in the present case are similar to those reported in the literature, e.g. λ C = 1.8D and 2.2D for flow past a circular cylinder with a trip-wire in the near wake by Zhang et al (1995) and Yildirim et al (2013b), respectively, and λ C ~ 1.7D for flow past a circular ring (Sheard et al, 2003).…”
Section: Wake Structure and Transition Mechanismsupporting
confidence: 89%
“…The most unstable spanwise wavelength for the subharmonic mode (∼1.9h) is similar to the wavelengths for the subharmonic mode observed in the wake of other bluff bodies (e.g. Sheard et al 2009;Yildirim, Rindt & van Steenhoven 2013).…”
Section: H Jiangsupporting
confidence: 73%
“…symmetry-breaking effect of the wire compared to the natural transition modes A and B, and to show the development of the streamwise vortices as a function of time. As indicated above, the secondary streamwise vortices in mode C transition originate from the primary upper vortices only, resulting in the typical 2T-periodic nature of mode C. The energy transfer from the primary to the secondary vortices is analysed in detail elsewhere (see Yildirim, Rindt & van Steenhoven 2013). The origin of the instability for the natural transition modes A and B arises from an elliptic instability of the vortex cores for mode A and from a hyperbolic instability in the braid region for mode B (Williamson 1992(Williamson , 1996aLeweke & Williamson 1998;Thompson et al 2001).…”
mentioning
confidence: 99%