Large-scale features in turbulent pipe and channel flows
By Jason Monty, J. Stewart, Robert M. Williams, Min S. Chong. Journal of Fluid Mechanics, 2007
379 citations recorded by the source corpus.
Subfields: Computational Mechanics, Environmental Engineering, Global and Planetary Change
View Paper: https://www.semanticscholar.org/paper/8654cf4eba4120506382538e2677537ab4e6938c
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Computational Mechanics
- B. McKeon
- Ivan Marusic
- Nicholas Hutchins
- Ati S. Sharma
- Javier Jiménez
- Jason Monty
- Alexander J Smits
- R. Mathis
In Environmental Engineering
- B. McKeon
- Ivan Marusic
- Nicholas Hutchins
- Ati S. Sharma
- Javier Jiménez
- Jason Monty
- R. Mathis
- Alexander J Smits
In Global and Planetary Change
- B. McKeon
- Ivan Marusic
- Nicholas Hutchins
- Javier Jiménez
- Jason Monty
- R. Mathis
- Alexander J Smits
- Ati S. Sharma
Citations in the corpus
- A predictive inner–outer model for streamwise turbulence statistics in wall-bounded flows (2011, background): “Recent investigations by Monty et al. (2007, 2009) have shown a strong similarity of the large-scale events between internal and external wall-bounded flows, which also have very different wake regions.”
- Coherent Structures and the Dissimilarity of Turbulent Transport of Momentum and Scalars in the Unstable Atmospheric Surface Layer (2011, background): “Kline et al. 1967; Head and Bandyopadhyay 1981; Kim and Adrian 1999; Monty et al. 2007; Ringuette et al. 2008; Marusic et al. 2010a).”
- Very-large-scale motions in a turbulent boundary layer (2010, methodology): “To address these problems, Hutchins & Marusic (2007) and Monty et al. (2007) performed experiments with a spanwise rake of 10 hot wires in the TBL, pipe and channel flows.”
- A critical-layer framework for turbulent pipe flow (2010, methodology): “We investigate n = 10 as a compromise that follows the expected critical-layer aspect ratio discussed in § 4 and is in reasonable agreement with the work of both Monty et al. (2007) and Bailey et al. (2008).”
- Estimating wall-shear-stress fluctuations given an outer region input (2013, background): “…motions have been observed to develop in the outer layer (Kim & Adrian 1999; del Álamo & Jiménez 2003; Tomkins & Adrian 2003; Hambleton, Hutchins & Marusic 2006; Hutchins & Marusic 2007a, amongst others), in all types of wall-bounded flows (Monty et al. 2007; Marusic & Hutchins 2008).”
- Experimental measurement of large-scale three-dimensional structures in a turbulent boundary layer. Part 2. Long structures (2011, background): “As well as being found in the log and lower wake regions of the turbulent boundary layer, these features are also found in pipe and channel flow (Kim & Adrian 1999; Monty et al. 2007).”
- A comparison of turbulent pipe, channel and boundary layer flows (2009, background): “Well beyond the log region, the profiles are clearly different, as previously discussed by Monty et al. (2007). In one of the first detailed comparisons of internal and external flows, Schubauer (1954) also highlights the differences in mean velocity profiles in the outer-flow region (although he ri”
- Towards Reconciling the Large-Scale Structure of Turbulent Boundary Layers in the Atmosphere and Laboratory (2012, result): “Similar experiments performed in channel and pipe flows by Monty et al. (2007) have proven the existence of comparable events in internal boundary layers.”
- High–Reynolds Number Wall Turbulence (2011, background): “Fourth, it has become clear that the relative importance of LSMs, VLSMs, and superstructures depends on the nature of the flow: They behave differently in pipes, channels, and boundary layers (Monty et al. 2007, Bailey et al. 2008), something that is not captured in the attached-eddy model.”
- Aspect ratio effects in turbulent duct flows studied through direct numerical simulation (2014, background): “[5], very large-scale motions with lengths from 5h to 20h are found in fully developed turbulent channel and pipe flows (h being the channel half-height or pipe radius).”
- Turbulence in supersonic boundary layers at moderate Reynolds number (2011, methodology): “The data by Monty et al. (2007), shown in figure 26(b), exhibit the same trend found in the present DNS.”