Characterization of wind-shear effects on entrainment in a convective boundary layer

Direct numerical simulations are used to characterize wind-shear effects on entrainment in a barotropic convective boundary layer (CBL) that grows into a linearly stratified atmosphere. We consider weakly to strongly unstable conditions �����zenc=LOb &4, where zenc is the encroachment CBL depth...

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Detalhes bibliográficos
Autores: Haghshenas, Armin, Mellado González, Juan Pedro|||0000-0001-7506-6539
Tipo de documento: artigo
Data de publicação:2019
País:España
Recursos:Universitat Politècnica de Catalunya (UPC)
Repositório:UPCommons. Portal del coneixement obert de la UPC
Idioma:inglês
OAI Identifier:oai:upcommons.upc.edu:2117/179796
Acesso em linha:https://hdl.handle.net/2117/179796
https://dx.doi.org/10.1017/jfm.2018.761
Access Level:Acceso aberto
Palavra-chave:Turbulence
Atmospheric turbulence
Atmospheric flows
Stratified turbulence
Turbulent convection
Turbulència atmosfèrica
Àrees temàtiques de la UPC::Física
Descrição
Resumo:Direct numerical simulations are used to characterize wind-shear effects on entrainment in a barotropic convective boundary layer (CBL) that grows into a linearly stratified atmosphere. We consider weakly to strongly unstable conditions �����zenc=LOb &4, where zenc is the encroachment CBL depth and LOb is the Obukhov length. Dimensional analysis allows us to characterize such a sheared CBL by a normalized CBL depth, a Froude number and a Reynolds number. The first two non-dimensional quantities embed the dependence of the system on time, on the surface buoyancy flux, and on the buoyancy stratification and wind velocity in the free atmosphere. We show that the dependence of entrainment-zone properties on these two non-dimensional quantities can be expressed in terms of just one independent variable, the ratio between a shear scale .1zi/s p 1=31u=N0 and a convective scale .1zi/c 0:25zenc, where 1u is the velocity increment across the entrainment zone, and N0 is the buoyancy frequency of the free atmosphere. Here .1zi/s and .1zi/c represent the entrainment-zone thickness in the limits of weak convective instability (strong wind) and strong convective instability (weak wind), respectively. We derive scaling laws for the CBL depth, the entrainment-zone thickness, the mean entrainment velocity and the entrainment-flux ratio as functions of .1zi/s=.1zi/c. These scaling laws can also be expressed as functions of only a Richardson number .N0zenc=1u/2, but not in terms of only the stability parameter �����zenc=LOb.