High–Reynolds Number Wall Turbulence

By Alexander J Smits, B. McKeon, Ivan Marusic. 2011

1,023 citations recorded by the source corpus.

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

View Paper: https://www.semanticscholar.org/paper/596161f91295afbe85b9035fb3b148e503d86371

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Citations in the corpus

Space-Time Correlations and Dynamic Coupling in Turbulent Flows (2017, methodology): “Applications of Taylor’s frozen-flow hypothesis to the time-to-space conversion in experimental measurements have been discussed in recent review articles (Lohse & Xia 2010, Smits et al. 2011, Wallace 2014).”
Towards Reconciling the Large-Scale Structure of Turbulent Boundary Layers in the Atmosphere and Laboratory (2012, background): “A thorough reading on coherent structures in laboratory flows can be found in the reviews of Robinson (1991), Panton (2001), Klewicki (2010), Marusic et al. (2010b) and Smits et al. (2011).”
Direct numerical simulation of turbulent channel flow up to $\mathit{Re}_{{\it\tau}}\approx 5200$ (2014, background): “The von Kármán constant κ that appears in the log-law, is also an important parameter for calibrating turbulence models (Durbin & Pettersson Reif 2010; Marusic et al. 2010b; Smits et al. 2011; Spalart & Allmaras 1992).”
The engine behind (wall) turbulence: perspectives on scale interactions (2017, background): “…review of scaling and coherent structure in wall turbulence Recent comprehensive treatises on the state of the art in our understanding of scaling, coherent structure and theoretical advances in wall turbulence have been given by Adrian (2007), Klewicki (2010) and Smits et al. (2011), among others.”
On coherent structure in wall turbulence (2013, background): “As mentioned above, models for the origin, dynamics and evolution of coherent structure are generally sparse in the literature, with the notable exception of the near-wall, self-sustaining cycle elucidated by Waleffe and co-workers, e.g. Waleffe (1997). Significant progress has also been made in ter”
Cascades in Wall-Bounded Turbulence (2012, background): “…objects variously described as global modes by del Álamo & Jiménez (2003) and del Álamo et al. (2004), or as very-large-scale motions (VLSMs) or superstructures by Adrian (2007) and Smits et al. (2011), whereas the objects depicted in Figure 4 are the largescale motions (LSMs) of those authors.”
Generalized logarithmic law for high-order moments in turbulent boundary layers (2013, result): “The prior data are consistent with a value (the Townsend–Perry constant) of A1 ≈ 1.25 (Marusic & Kunkel 2003; Smits et al. 2011; Hultmark et al. 2012; Marusic 2012; Marusic et al. 2013), whereas B1 is dependent upon flow conditions and geometry, and is thus not expected to be universal.”
On the logarithmic region in wall turbulence (2013, methodology): “However, as seen in figure 1, the turbulence intensity 716 R3-4 profiles tend to depart from the logarithmic profile more abruptly than for the mean flow (Marusic & Kunkel 2003; Smits et al. 2011).”
The Physics of Sediment Transport Initiation, Cessation, and Entrainment Across Aeolian and Fluvial Environments (2020, background): “…on the Initiation of Aeolian Rolling and Saltation Transport The size of turbulent flow eddies, and thus the duration of turbulent fluctuation events, is limited by the system dimensions, more specifically, the boundary layer thickness δ [see review by Smits et al., 2011, and references therein].”