2015
DOI: 10.1016/j.ijheatfluidflow.2014.09.009
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Properties of the streamwise velocity fluctuations in the inertial layer of turbulent boundary layers and their connection to self-similar mean dynamics

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Cited by 14 publications
(8 citation statements)
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“…Referencing the Newtonian fluid flow cases (δ + ≅ 1800 experiment, δ + = 2004 DNS), it is apparent that these profiles complete their distinct change in slope near U/U cl = 0.68 at the present δ + . As observed by Zhou & Klewicki (2015) in boundary layers over 1450 δ + 19600 this knee in the curve slowly moves to lower U/U cl with increasing δ + , and the onset of the Reynolds number invariant (approximately linear) region closely corresponds to the start of the inertial domain found from consideration of the MMB. For the DNS, this position is denoted by the solid vertical line in figure 27(a), and by the black diamond symbol for the δ + ≃ 1800 experiment.…”
Section: Diagnostic Plotsupporting
confidence: 67%
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“…Referencing the Newtonian fluid flow cases (δ + ≅ 1800 experiment, δ + = 2004 DNS), it is apparent that these profiles complete their distinct change in slope near U/U cl = 0.68 at the present δ + . As observed by Zhou & Klewicki (2015) in boundary layers over 1450 δ + 19600 this knee in the curve slowly moves to lower U/U cl with increasing δ + , and the onset of the Reynolds number invariant (approximately linear) region closely corresponds to the start of the inertial domain found from consideration of the MMB. For the DNS, this position is denoted by the solid vertical line in figure 27(a), and by the black diamond symbol for the δ + ≃ 1800 experiment.…”
Section: Diagnostic Plotsupporting
confidence: 67%
“…A logarithmic mean velocity profile stems from this self-similar structure. Zhou & Klewicki (2015) investigated the correspondences between the self-similar inertial domain just described, and that found for other measures of self-similar structure in the canonical boundary layer. Notably, to within the uncertainty of their data they found an exact correspondence between 2.6 √ δ + y + δ + /2 and the domain over which the so-called diagnostic plot of Alfredsson et al (2012) exhibits its (approximately) linear decrease.…”
Section: Diagnostic Plotmentioning
confidence: 91%
“…Besides the established logarithmic behaviour for the mean velocity profile, recent data also support the existence of a logarithmic law for the streamwise velocity variance profile as predicted by the attached-eddy hypothesis [49]. Also higher-order even moments have been found to adhere to this scaling [7,50], although with some objections [8]. When it comes to the variance profile, the data are predicted, with increasing Re for a larger interior region, to follow )…”
Section: Reynolds Stresses (A) Streamwise Componentmentioning
confidence: 55%
“…Also higher-order even moments have been found to adhere to this scaling [7,50], although with some objections [8]. When it comes to the variance profile, the data are predicted, with increasing Re for a larger interior region, to follow y + /(R + ) 1/2 values of 2.6-3.9 [7,32,50]. It should be noted that, while the location of the lower bound for the logarithmic region in the aforementioned studies is found empirically, there is a physical basis, as argued by Klewicki and co-workers [52,53]: this position, in fact, should locate the start of the region where the mean dynamics lose a leading-order viscous effect.…”
Section: Reynolds Stresses (A) Streamwise Componentmentioning
confidence: 82%
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