TY - JOUR
T1 - Evidence for Raupach et al.'s mixing-layer analogy in deep homogeneous urban-canopy flows
AU - Zhang, Wen
AU - Zhu, Xiaowei
AU - Yang, Xiang I.A.
AU - Wan, Minping
N1 - Funding Information:
W.Z. and M.W. acknowledges NSFC (grant nos 12102168, 91752201 and 11988102), Shenzhen Science & Technology Program (grant no. KQTD20180411143441009), Department of Science and Technology of Guangdong Province (grant nos 2019B21203001, 2020B1212030001), Key Special Project for Introduced Talents Team of Southern Marine Science and Engineering Guangdong Laboratory (Guangzhou) (grant no. GML2019ZD0103) for financial support. M.W. acknowledges the support from Centers for Mechanical Engineering Research and Education at MIT and SUSTech (MechERE Centers at MIT and SUSTech). Yang acknowledges NSF grant no. 2231037, ONR and Penn State University for financial support. Numerical simulations have been supported by Center for Computational Science and Engineering of Southern University of Science and Technology.
Publisher Copyright:
© The Author(s), 2022. Published by Cambridge University Press.
PY - 2022/8/10
Y1 - 2022/8/10
N2 - The mixing-layer analogy is due to Raupach, Finnigan & Brunet (Boundary-Layer Meteorol., vol. 25, 1996, pp. 351-382). In the analogy, the flow in the roughness sublayer of a homogeneous deep vegetation canopy boundary layer is analogous to a plane mixing layer rather than a surface layer. Evidence for the analogy includes the inflected velocity profile, which resembles the velocity profile in a plane mixing layer, and, most notably, the following estimate as a result of the Kelvin-Helmholtz instability:Λx = 8.1Ls, whereΛx is the spacing of the large-scale eddies, and Ls is the shear length. The mixing-layer analogy has been very successful in vegetation canopy flow research, but has received only limited support in urban-canopy flow research. This work revisits Raupach et al.'s mixing-layer analogy, and we present the evidence for the mixing-layer analogy in urban-canopy flows: the exponential velocity profile in the canopy layer, i.e. (U-Uc)/(Uh-Uc) = exp(z/Lm), and Lm ∼ [(Uh/Uc-1)(Uh/Uc + 3)]-1. Here, z is the vertical coordinate, Lm is the attenuation length and is a measure of the largest eddy in the canopy layer, Uh is the wind speed at the canopy crest and Uc is the velocity in the inactive layer. We conduct direct numerical simulations of various deep homogeneous urban-canopy flows and test the above two scalings. We also discuss why Raupach et al.'s analogy has not seen as many successes in urban-canopy flows as in vegetation canopy flows.
AB - The mixing-layer analogy is due to Raupach, Finnigan & Brunet (Boundary-Layer Meteorol., vol. 25, 1996, pp. 351-382). In the analogy, the flow in the roughness sublayer of a homogeneous deep vegetation canopy boundary layer is analogous to a plane mixing layer rather than a surface layer. Evidence for the analogy includes the inflected velocity profile, which resembles the velocity profile in a plane mixing layer, and, most notably, the following estimate as a result of the Kelvin-Helmholtz instability:Λx = 8.1Ls, whereΛx is the spacing of the large-scale eddies, and Ls is the shear length. The mixing-layer analogy has been very successful in vegetation canopy flow research, but has received only limited support in urban-canopy flow research. This work revisits Raupach et al.'s mixing-layer analogy, and we present the evidence for the mixing-layer analogy in urban-canopy flows: the exponential velocity profile in the canopy layer, i.e. (U-Uc)/(Uh-Uc) = exp(z/Lm), and Lm ∼ [(Uh/Uc-1)(Uh/Uc + 3)]-1. Here, z is the vertical coordinate, Lm is the attenuation length and is a measure of the largest eddy in the canopy layer, Uh is the wind speed at the canopy crest and Uc is the velocity in the inactive layer. We conduct direct numerical simulations of various deep homogeneous urban-canopy flows and test the above two scalings. We also discuss why Raupach et al.'s analogy has not seen as many successes in urban-canopy flows as in vegetation canopy flows.
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U2 - 10.1017/jfm.2022.507
DO - 10.1017/jfm.2022.507
M3 - Article
AN - SCOPUS:85133858442
SN - 0022-1120
VL - 944
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
M1 - A46
ER -