Vortex organization in the outer region of the turbulent boundary layer

By Ronald J. Adrian, C. Meinhart, Christopher D. Tomkins. Journal of Fluid Mechanics, 2000

1,756 citations recorded by the source corpus.

Subfields: Computational Mechanics, Environmental Engineering, Global and Planetary Change

View Paper: https://www.semanticscholar.org/paper/7f1a5cce0a5814f29c0827d112b2acdc9a5d5040

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Citations in the corpus

Large-Eddy Simulations on the Effects of Surface Geometry of Building Arrays on Turbulent Organized Structures (2004, result): “These characteristics of TOS are consistent with the ‘hairpin vortex packet model’ as proposed in Adrian et al. (2000) but previously described only for flat-wall boundary layers.”
Large-scale amplitude modulation of the small-scale structures in turbulent boundary layers (2009, background): “Such elongated regions of momentum deficit have been explained within vortex-based models as the regions between the legs of aligned packets of hairpin vortices (Adrian et al. 2000; Ganapathisubramani et al. 2003; Tomkins & Adrian 2003; Hambleton et al. 2006; and others). These low-speed regions are”
Some physical aspects of shock wave/boundary layer interactions (2009, neutral): “[29], Ganapathisubramani et al.”
Estimating wall-shear-stress fluctuations given an outer region input (2013, background): “…understanding of Reynolds number effects in the turbulent boundary layer, which are now well established to be closely related to the strengthening of the large scales with Re (Townsend 1976; Adrian et al. 2000; Metzger & Klewicki 2001; del Álamo et al. 2004; Marusic et al. 2010a, and others).”
The structure of the near neutral atmospheric surface layer as observed during the CASES'99 experiment (2004, methodology): “The existence of these smaller eddies is supported by the experimental work of Hommema and Adrian (2003) in the neutral PBL even though Adrian et al. (2000) disagree with Hunt and Morrison (2000) on the mechanism responsible for these substructures (they propose a bottom-up mechanism for eddy motion”
Low-Frequency Unsteadiness of Shock Wave/Turbulent Boundary Layer Interactions (2014, background): “Other notable reviews include those by Delery & Marvin (1986), Zheltovodov (1996), and Andreopoulos et al. (2000) and the recent edited books by Babinsky & Harvey (2011) and Doerffer et al. (2010).”
Direct numerical simulation of turbulence in a nominally zero-pressure-gradient flat-plate boundary layer (2009, methodology): “interesting to study any possible connections between the hairpin vortices and possible large and very-large scale motions in a ZPGFPBL such as those observed indirectly in the experiments of Adrian et al. (2000) and Hutchins & Marusic (2007).”
Characterization of coherent vortical structures in a supersonic turbulent boundary layer (2008, background): “Visual analysis of many flow samples shows the occurrence of: (i) hairpin-shaped vortices, occasionally arranged in packets (see figure 3a), as observed by Adrian et al. (2000) and Ringuette et al. (2008); (ii) vortex arches (see figure 3b); and (iii) few inverted arches (figure 3c).”
Large-scale influences in near-wall turbulence (2007, background): “For channels, analysis of large numerical domain DNS results (in particular two-dimensional spectra) have shown that the log region f uu energy can reside in very long streamwise modes for larger k y bands (certainly more than 20 channel half heights; see Jime´nez 1998; del Alamo & Jime´nez 2003).”
Uniform momentum zones in turbulent boundary layers (2014, methodology): “Any of these operations will smooth out the detection of UMZs as noted by Adrian et al. (2000).”