A comparison of turbulent pipe, channel and boundary layer flows

By Jason Monty, Nicholas Hutchins, Henry C.-H. Ng, Ivan Marusic, Min S. Chong. Journal of Fluid Mechanics, 2009

372 citations recorded by the source corpus.

Subfields: Computational Mechanics, Environmental Engineering, Mechanical Engineering

View Paper: https://www.semanticscholar.org/paper/47187c7c6646d1c44b152b3d331d877aabd8020a

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Citations in the corpus

A critical-layer framework for turbulent pipe flow (2010, background): “This has included differences in some characteristics between the canonical cases of pipe, channel and zero-pressuregradient boundary-layer flow (Monty et al. 2009), in contrast to the long-standing hypothesis of universality of near-wall scaling.”
Direct numerical simulation of turbulent channel flow up to $\mathit{Re}_{{\it\tau}}\approx 5200$ (2014, background): “To the best of our knowledge, DNS of turbulent channel flow up to Reτ ≈ 5200 409 such distinct peaks have only previously been observed in high-Reynolds-number experimental data (Hutchins & Marusic 2007; Monty et al. 2009; Marusic, Mathis & Hutchins 2010a; Marusic et al. 2010b).”
Spectral analysis of the budget equation in turbulent channel flows at high Reynolds number (2018, background): “…EΨ (k, y) dk. (3.14c) Selecting a cutoff wavenumber is somewhat arbitrary and controversial in the context of defining the large scales (Hutchins et al. 2009; Monty et al. 2009; Marusic et al. 2010c; Ganapathisubramani et al. 2012; Wu, Baltzer & Adrian 2012; Chin et al. 2014; Ahn, Lee &…”
High–Reynolds Number Wall Turbulence (2011, background): “…the smallest scale corresponds to the diameter of the filamentary (or worm-like) vortex structures (Stanislas et al. 2008), and the largest scale corresponds to the streamwise extent of the very-large-scale motions (VLSMs) that have been observed in pipes (Kim & Adrian 1999, Monty et al. 2009).”
A predictive inner–outer model for streamwise turbulence statistics in wall-bounded flows (2011, methodology): “…from a channel flow (with matched hot-wire length l+ = 22), and while it is clear that differences in the largest scales between internal and external geometries exist, for present purposes a reasonable comparison of the inner layer is likely to be valid (Monty et al. 2009; Mathis et al. 2009b).”
High Reynolds number effects in wall turbulence (2010, background): “This secondary emergent peak is the energetic signature due to highly elongated (and correlated) meandering regions of spanwise alternating positive and negative u fluctuations that have been observed in the log and wake regions of wall-bounded turbulent flows (so-called superstructures or VLSM (Kim”
The engine behind (wall) turbulence: perspectives on scale interactions (2017, background): “At length scales related to the outer scale, both large-scale motions (LSMs) and very-large-scale motions (VLSMs) can be identified via the streamwise spectrum in the canonical flows, (e.g. Monty et al. 2009).”
Large-eddy simulation of large-scale structures in long channel flow (2010, background): “See Monty et al. (2009) for a description of the differences between the characteristics of these large structures in the different canonical flows.”
Colour of turbulence (2016, background): “One such example is that of boundary layer flows where experiments (Hutchins & Marusic 2007b; Mathis et al. 2009; Monty et al. 2009; Guala et al. 2011; Marusic et al. 2013) and simulations (Wu & Moin 2009; Schlatter & Örlü 2010; Sillero, Jiménez & Moser 2013, 2014) have provided insight into coheren”