2018
DOI: 10.1017/jfm.2018.126
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Time evolution of uniform momentum zones in a turbulent boundary layer

Abstract: Time-resolved planar particle image velocimetry was used to analyse the structuring of a turbulent boundary layer into uniform momentum zones (UMZs). The instantaneous peak-detection method employed by Adrian et al. (J. Fluid Mech., vol. 422, 2000, pp. 1–54) and de Silva et al. (J. Fluid Mech., vol. 786, 2016, pp. 309–331) is extended to account for temporal coherence of UMZs. The resulting number of zones detected appears to follow a normal distribution at any given instant. However, the extreme cases in whic… Show more

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Cited by 49 publications
(128 citation statements)
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References 58 publications
(94 reference statements)
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“…Studies of coherent structures in high-Reynolds-number flows have revealed the presence of spatial regions with relatively uniform streamwise velocity (Meinhart & Adrian 1995). These structures are known as uniform momentum zones (UMZs) and have been identified both at the laboratory scale (Adrian et al 2000;de Silva et al 2016;Saxton-Fox & McKeon 2017;Laskari et al 2018) and in the atmosphere (Morris et al 2007;Heisel et al 2018). Individual UMZs are separated by relatively thin regions where a large percentage of the overall shear and vorticity are concentrated (Priyadarshana et al 2007;Eisma et al 2015;de Silva et al 2017).…”
Section: Introductionmentioning
confidence: 99%
“…Studies of coherent structures in high-Reynolds-number flows have revealed the presence of spatial regions with relatively uniform streamwise velocity (Meinhart & Adrian 1995). These structures are known as uniform momentum zones (UMZs) and have been identified both at the laboratory scale (Adrian et al 2000;de Silva et al 2016;Saxton-Fox & McKeon 2017;Laskari et al 2018) and in the atmosphere (Morris et al 2007;Heisel et al 2018). Individual UMZs are separated by relatively thin regions where a large percentage of the overall shear and vorticity are concentrated (Priyadarshana et al 2007;Eisma et al 2015;de Silva et al 2017).…”
Section: Introductionmentioning
confidence: 99%
“…The largest UMZs remain coherent in the streamwise direction for distances approaching the boundary-layer (BL) thickness or channel half-height h for times estimated to be O(h/U ∞ ), where U ∞ is the free-stream or mean channel-centreline velocity (Laskari et al 2018). Both laboratory experiments (de Silva et al 2016) and analyses of the mean momentum equation (Klewicki 2013a,b) indicate that the number of UMZs grows logarithmically with the friction Reynolds number Re τ ≡ u τ h/ν, where u τ is the wall friction velocity and ν is the kinematic viscosity of the fluid, and that the typical change in streamwise velocity across individual fissures is a few multiples of u τ .…”
Section: Introductionmentioning
confidence: 99%
“…The values of mean flow velocity bold-italicutrue¯f=()utrue¯f,vtrue¯f, turbulence intensities σ f = ( σ fu , σ fv ), the mean period of event occurrences trueT¯, and the probability distribution of the event duration T used in simulations are taken from the flow data of wall‐bounded turbulence studies ( Dennis & Nickels, ; Laskari et al, ; Noguchi & Nezu, ). The values of sediment particle settling velocity w s = (0, − w s ) depend on the properties of simulated suspended sediment particles.…”
Section: Methodsmentioning
confidence: 99%
“…Probability density functions of the residence time of large‐scale Q2 events measured by Laskari et al (). In this work, the residence time is treated as the duration for ejection and sweep events.…”
Section: Methodsmentioning
confidence: 99%
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