Rough-wall boundary layers: mean flow universality
By I. Castro. Journal of Fluid Mechanics, 2007
198 citations recorded by the source corpus.
Subfields: Computational Mechanics, Environmental Engineering, Mechanical Engineering
View Paper: https://www.semanticscholar.org/paper/52efdb62724b40dca9b54af99f671a32462eaa26
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Citations in the corpus
- Channel flow over large cube roughness: a direct numerical simulation study (2010, methodology): “This, incidentally, means that the viscous length scale (ν/uτ ) is not a relevant near-wall scale and such flows are therefore much less dependent on Reynolds numbers, like the momentum thickness Reynolds number Reθ , than are smooth-wall flows (Castro 2007).”
- Exponential roughness layer and analytical model for turbulent boundary layer flow over rectangular-prism roughness elements (2016, background): “A moderate wake correction of Π = 0.2 is added (Castro 2007).”
- Turbulence structure in a boundary layer with two-dimensional roughness (2009, methodology): “results of Cheng & Castro (2002), who used staggered rows of cubes spaced at p/k = 2 in both the streamwise and spanwise directions.”
- Direct numerical simulation of the turbulent boundary layer over a cube-roughened wall (2010, result): “This result is consistent with those of the experimental study of flow in the presence of cube roughness by Castro (2007).”
- Effects of spanwise spacing on large-scale secondary flows in rough-wall turbulent boundary layers (2015, background): “This development distance is nearly double the suggested length of 20δ to ensure fully developed conditions in rough-wall turbulent boundary layers (Antonia & Luxton 1971; Castro 2007), where δ is the boundary layer thickness and is reported below in section 3.”
- Double-averaging analysis and local flow characterization of near-bed turbulence in gravel-bed channel flows (2009, background): “Note that the universality of the log law was once more confirmed for organized rough boundary layers by Castro (2007). The displacement height z was found to be very small, z − 0.”