1999
DOI: 10.1017/s0022112099005911
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The turbulent boundary layer over transverse square cavities

Abstract: Laser-induced uorescence (LIF) and laser Doppler velocimetry (LDV) are used to explore the structure of a turbulent boundary layer over a wall made up of two-dimensional square cavities placed transversely to the flow direction. There is strong evidence of occurrence of outflows of fluid from the cavities as well as inflows into the cavities. These events occur in a pseudo-random manner and are closely associated with the passage of near-wall quasi-streamwise vortices. These vortices and the associated l… Show more

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Cited by 133 publications
(79 citation statements)
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References 28 publications
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“…Interestingly, the spatial extents of pww in the streawise and spanwise directions appear unaffected by protrusion F as the inhomogeneous correlation matches its homogeneous counterpart except for slight differences for small spatial separations (Note that the inhomogeneous correlations appear much noisier than their homogeneous counterparts because the number of samples averaged to generate inhomogeneous correlations is significantly reduced under this assumption). The relative insensitivity of the larger-scale features of p wl and pe to roughness feature F is consistent with the observations of Djenidi et al (1999) who reported that the outflows from square cavities did not appreciably affect the spatial characteristics of low-speed streaks in the near-wall region. They attributed this insensitivity to the substantial scale difference between the outflows generated by the roughness cavities and the large-scale streaks.…”
Section: Impact Of Surface Protrusions On Spatial Correlations In Rousupporting
confidence: 90%
See 1 more Smart Citation
“…Interestingly, the spatial extents of pww in the streawise and spanwise directions appear unaffected by protrusion F as the inhomogeneous correlation matches its homogeneous counterpart except for slight differences for small spatial separations (Note that the inhomogeneous correlations appear much noisier than their homogeneous counterparts because the number of samples averaged to generate inhomogeneous correlations is significantly reduced under this assumption). The relative insensitivity of the larger-scale features of p wl and pe to roughness feature F is consistent with the observations of Djenidi et al (1999) who reported that the outflows from square cavities did not appreciably affect the spatial characteristics of low-speed streaks in the near-wall region. They attributed this insensitivity to the substantial scale difference between the outflows generated by the roughness cavities and the large-scale streaks.…”
Section: Impact Of Surface Protrusions On Spatial Correlations In Rousupporting
confidence: 90%
“…Although the overall shape of Puv was unaffected compared to smooth-wall flow, its streamwise extent was also decreased by the short strip of roughness. Djenidi et al (1999) studied the near-wall structure of a turbulent boundary layer over d-type transverse square cavities using laser-induced fluorescence (LIF) in a streamwise-spanwise plane positioned 6y. above the roughness crests at Reo = 1100.…”
Section: Roughness Effects In the Near-wall Regionmentioning
confidence: 99%
“…These occurred at irregular time intervals and were associated with some additional air entrainment. The ejections appeared to be sequential from upstream to downstream as illustrated by Djenidi et al (1999) and Chanson et al (2002). On average, the flat stepped data indicated a nearly constant cavity ejection rate independently of downstream distance for a given flow rate (Fig.…”
Section: Cavity Flow Processesmentioning
confidence: 86%
“…For a flow of given bulk Reynolds number, R, over two-dimensional roughness elements, the transition between d-and k-type roughness depends solely on the streamwise spacing of the elements. Many researchers have chosen to focus on square bar roughness to investigate the effect of spacing on turbulence structure and mean flow characteristics, both experimentally (Coleman, Nikora, McLean, & Schlicke, 2007;Djenidi, Antonia, Amielh, & Anselmet, 2008;Djenidi, Elavarasan, & Antonia, 1999;Krogstad, Andersson, Bakken, & Ashrafian, 2005;Okamoto, Seo, Nakaso, & Kawai, 1993;Roussinova & Balachandar, 2011) and numerically (Cui, Patel, & Lin, 2003;Ikeda & Durbin, 2007;Stoesser & Nikora, 2008;Stoesser & Rodi, 2004). Simpson (1973), Tani (1987), Jiminez (2004) and Coleman et al (2007) all proposed that the transition from d-to k-type roughness occurs at around l/k = 5, where l is the crest-to-crest bar spacing and k is the roughness height.…”
Section: Introductionmentioning
confidence: 99%