Perturbing vortex packets in a turbulent boundary layer

A zero pressure gradient turbulent boundary layer of $\textit {Re}_{\tau }=2500$ was perturbed by a single spanwise array of finite cylinders mounted on the bounding surface and extending through the logarithmic region. The cylinder height was $H/\delta =0.2$ ( $H^{+}=500$ ), where $\delta $ is the...

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Veröffentlicht in:Journal of fluid mechanics 2014-06, Vol.748, p.368-398
Hauptverfasser: Zheng, Shaokai, Longmire, Ellen K.
Format: Artikel
Sprache:eng
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Zusammenfassung:A zero pressure gradient turbulent boundary layer of $\textit {Re}_{\tau }=2500$ was perturbed by a single spanwise array of finite cylinders mounted on the bounding surface and extending through the logarithmic region. The cylinder height was $H/\delta =0.2$ ( $H^{+}=500$ ), where $\delta $ is the boundary layer thickness, with an aspect ratio ( $AR$ ) (height/diameter) of four. Streamwise–spanwise ( $x\text {--}y$ ) planes of the flow were examined by particle image velocimetry (PIV) up to $7\delta $ downstream at a wall-normal location of $z^{+}=300$ for cylinder array spacings ranging from $0.2\delta $ to $0.8\delta $ . Average streamwise velocity fields showed a splitting, then merging pattern of cylinder wakes which occurred further downstream as the cylinder spacing increased. Based on measurements at the furthest downstream location, both the spanwise variation of average streamwise velocity and the Fourier content in the instantaneous fields suggested that the case with $0.6\delta $ cylinder spacing, which matched the dominant spanwise scale in the unperturbed flow, yielded the most persistent downstream flow organization. A flying PIV method was implemented to track specific packet structures over a range $-2
ISSN:0022-1120
1469-7645
DOI:10.1017/jfm.2014.185