2018
DOI: 10.1061/(asce)hy.1943-7900.0001511
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PIV-PLIF Characterization of Nonconfined Saline Density Currents under Different Flow Conditions

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Cited by 18 publications
(6 citation statements)
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“…Typical profiles of shear layers are obtained: the streamwise velocity shows an error function-like distribution linking the top and bottom borders of the mixing layer, and the TKE presents a Gaussian-like distribution peaking at the mixing layer's centre, where shearing is at a maximum (Townsend 1980;Vreman, Geurts & Kuerten 1997;Balaras, Piomelli & Wallace 2001;Yang et al 2004;Krug et al 2013). In particular, the profiles obtained forx f −x > 3.4H compare well with experimental and numerical data reported in the body of lock-exchange currents (Garcia 1994;Gray, Alexander & Leeder 2006;Cantero, Balachandar & Parker 2009;Eggenhuisen & McCaffrey 2012) and unconfined currents (Pérez-Díaz et al 2018b;Wilson, Friedrich & Stevens 2018a). The velocity gradient remains constant across the mixing layer, except inside the head where it grows towards the centre of the mixing region.…”
Section: Reynolds Stress U Vsupporting
confidence: 79%
“…Typical profiles of shear layers are obtained: the streamwise velocity shows an error function-like distribution linking the top and bottom borders of the mixing layer, and the TKE presents a Gaussian-like distribution peaking at the mixing layer's centre, where shearing is at a maximum (Townsend 1980;Vreman, Geurts & Kuerten 1997;Balaras, Piomelli & Wallace 2001;Yang et al 2004;Krug et al 2013). In particular, the profiles obtained forx f −x > 3.4H compare well with experimental and numerical data reported in the body of lock-exchange currents (Garcia 1994;Gray, Alexander & Leeder 2006;Cantero, Balachandar & Parker 2009;Eggenhuisen & McCaffrey 2012) and unconfined currents (Pérez-Díaz et al 2018b;Wilson, Friedrich & Stevens 2018a). The velocity gradient remains constant across the mixing layer, except inside the head where it grows towards the centre of the mixing region.…”
Section: Reynolds Stress U Vsupporting
confidence: 79%
“…Release of a dense fluid into a lighter ambient fluid from a non-continues source (e.g., the lock-exchange technique) or a continuous source (e.g., a dense jet) has been studied in several experimental investigations [6][7][8][9][10][11][12][13][14][15][16][17][18] . Experimental investigations also assessed the interactions between turbidity currents of different densities and velocities with an obstacle of varying geometrical features including height and width 19-27 .…”
Section: Turbidity Currents Are Frequently Observed In Natural and Mamentioning
confidence: 99%
“…One camera took the image at time t and the other camera at t + ∆t. The velocity composition was carried out by an inter-correlation algorithm [42], which divides the two successive images of the recorded particles at time t and t + ∆t into small interrogation areas. The position of the correlation peak between the two images corresponds to the most probable displacement of the particles for each of these interrogation areas [42].…”
Section: Setup Of the Physical Modellingmentioning
confidence: 99%
“…The velocity composition was carried out by an inter-correlation algorithm [42], which divides the two successive images of the recorded particles at time t and t + ∆t into small interrogation areas. The position of the correlation peak between the two images corresponds to the most probable displacement of the particles for each of these interrogation areas [42]. The effects of geometric distortion, resulting from small angles in camera alignment, were automatically corrected during image processing and post-processing using LaVision DaVis software.…”
Section: Setup Of the Physical Modellingmentioning
confidence: 99%