2014
DOI: 10.1017/jfm.2014.236
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Experimental investigation of flow behind a cube for moderate Reynolds numbers

Abstract: The wake behind a cube with a face normal to the flow was investigated experimentally in a water tunnel using laser induced fluorescence (LIF) visualisation and particle image velocimetry (PIV) techniques. Measurements were carried out for moderate Reynolds numbers between 100 and 400 and in this range a sequence of two flow bifurcations was confirmed. Values for both onsets were determined in the framework of Landau's instability model. The measured longitudinal vorticity was separated into three components c… Show more

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Cited by 34 publications
(39 citation statements)
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“…The experimentally found Strouhal numbers are almost independent of the Reynolds number. Similar results were reported recently by Klotz et al (2014) for a cube placed in a low-Reynolds water tunnel (with cross-section 100 mm × 100 mm, located at PMMH, ESPCI). Unlike the experiments by Calvert, which were carried out in a wind tunnel representing to a large extent an unconfined configuration, our experiments were realized in a water channel with non-negligible blockage factor.…”
Section: Resultssupporting
confidence: 91%
“…The experimentally found Strouhal numbers are almost independent of the Reynolds number. Similar results were reported recently by Klotz et al (2014) for a cube placed in a low-Reynolds water tunnel (with cross-section 100 mm × 100 mm, located at PMMH, ESPCI). Unlike the experiments by Calvert, which were carried out in a wind tunnel representing to a large extent an unconfined configuration, our experiments were realized in a water channel with non-negligible blockage factor.…”
Section: Resultssupporting
confidence: 91%
“…4a, b,c,d). We note that the transition to hairpin shedding in JICF in low-velocity-ratio regime is analogous to the transition reported for the wake behind three-dimensional bluff bodies, such as sphere (Johnson & Patel 1999;Gumowski et al 2008), disk (Bobinski et al 2014) and cube (Klotz et al 2014), with similar structure of shed hairpins and with a gentle kinking of two trails of counter-rotating vortices prior to self-sustained shedding of hairpins (see at x/D jet > 8 in Fig. 4c,d).…”
Section: Resultssupporting
confidence: 77%
“…The test section has rectangular cross-section of 15.0 cm width and 10.0 cm height, and length of the channel is 150.0 cm. The crossflow is induced by gravity, using a constant-level tank located above the test section to provide a constant pressure gradient (see also Fig.1 in Klotz et al (2014)). Before entering the test section, the crossflow is conditioned by two honeycomb screens and a 4:1 contraction nozzle.…”
Section: Experimental Set-upmentioning
confidence: 99%
“…The wake and its instabilities behind different 3D static bodies, e.g., sphere, disks, cube, bullets, etc. were considered in the numerical as well as in the experimental studies [1][2][3][4][5][6]. The flow instabilities of a viscous fluid past a rotating sphere may be considered as a simplified case of a more general family of flows around immersed rotating bodies [7,8].…”
Section: Introductionmentioning
confidence: 99%