Scaling of the streamwise velocity component in turbulent pipe flow

By J. Morrison, B. McKeon, W. Jiang, Alexander J Smits. Journal of Fluid Mechanics, 2004

234 citations recorded by the source corpus.

Subfields: Computational Mechanics, Environmental Engineering

View Paper: https://www.semanticscholar.org/paper/bc522da822e04f7215f1f67252c54b70aa04860e

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Citations in the corpus

Turbulence measurements using a nanoscale thermal anemometry probe (2010, methodology): “One experiment where the effects of spatial filtering are particularly evident is the Princeton/ONR Superpipe experiment described by Zagarola & Smits (1998) and Morrison et al. (2004).”
Spectral analysis of the budget equation in turbulent channel flows at high Reynolds number (2018, background): “Further, the contribution of the large-scale outer turbulence is shown to grow with increasing Re, causing the streamwise velocity variance to have both an inner-layer peak and an outerlayer peak (Fernholz & Finley 1996; Morrison et al. 2004).”
Scaling of the velocity fluctuations in turbulent channels up to Reτ=2003 (2006, background): “2 , Couette flows; 4 , pipes and channels; *, pipes from Morrison et al. (2004); +, boundary layers; ◦ , present numerical channels.”
Spatial resolution correction for wall-bounded turbulence measurements (2011, background): “For example, Morrison et al. (2004) found that in a pipe, at sufficiently high Reynolds numbers an outer peak was formed, located near the lower edge of the log-region.”
Interactions within the turbulent boundary layer at high Reynolds number (2011, background): “In particular, the definition of ‘active’ and ‘inactive’ motions in the sense of Townsend has been revisited, alongside a renewed investigation of the Reynolds number dependency of the near-wall velocity field (e.g. Metzger & Klewicki 2001; Morrison et al. 2004; Hutchins & Marusic 2007a; Morrison 20”
A predictive inner–outer model for streamwise turbulence statistics in wall-bounded flows (2011, methodology): “The predicated trend at very high Reynolds number, with a second outer peak appearing in u2/U 2τ , is a topic of some controversy (Fernholz & Finley 1996; Morrison et al. 2004; Hutchins et al. 2009; Marusic et al. 2010c).”
Developments In Smooth Wall Turbulent Duct Flows (2005, unknown): “A Universal constant in the logarithmic law of the wall A1 Universal constant in the logarithmic u′2 formulation A2 Universal constant in the w′2 formulation A3 Universal constant in the v′2 formulation As Aspect ratio of rectangular duct a0 Universal constant in the mean velocity formulation of Nic”
High Reynolds number effects in wall turbulence (2010, result): “Previous studies by Morrison et al. (2004) in the Princeton superpipe have proposed”
Logarithmic scaling of turbulence in smooth- and rough-wall pipe flow (2013, methodology): “The smooth pipe was the same as that used by Zagarola & Smits (1998) and McKeon et al. (2004), and Morrison et al. (2004), with an average inner radius of R = 64.68 mm and a surface roughness of krms = 0.15 µm, resulting in a relative roughness of krms/R= 2.3× 10−6.”
Hot-wire spatial resolution issues in wall-bounded turbulence (2009, methodology): “Note that for this figure we use wavenumber (kx) rather than wavelength (λx = 2π/kx) for consistency with Morrison et al. (2004) and Nickels et al.”
Turbulent fluctuations above the buffer layer of wall-bounded flows (2008, background): “It should be mentioned at this point that Morrison et al. (2004) have proposed that the trend in figure 4(b) is a low-Reynolds-number effect.”
DNS of turbulent Couette flow with emphasis on the large-scale structure in the core region (2006, unknown): “[35] yields results consistent with Hites’ experiments.”