
d2387f71ce26968a492ab5382b843685.ppt
- Количество слайдов: 46
L. N. Gutman Conference on Mesoscale Meteorology and Air Pollution, Odessa, Ukraine, September 15 -17, 2008 Internal Gravity Waves and Turbulence Closure Model for SBL Sergej Zilitinkevich Division of Atmospheric Sciences, Department of Physical Sciences University of Helsinki and Finnish Meteorological Institute Helsinki, Finland Tov Elperin, Nathan Kleeorin and Igor Rogachevskii Department of Mechanical Engineering The Ben-Gurion University of the Negev Beer-Sheba, Israel Victor L’vov Department of Chemical Physics, Weizmann Institute of Science, Israel
Boussinesq Approximation
Laminar and Turbulent Flows Laminar Boundary Layer Turbulent Boundary Layer
Why Turbulence? Why Not DNS? Number degrees of freedom
Turbulent Eddies
Laboratory Turbulent Convection After averaging Before averaging
Velocity Fields
SBL Equations
Total Energy
Total Budget Equations: BL-case
Total Budget Equations for SBL
Total Budget Equations: BL-case
Total Energy The turbulent potential energy: The source:
Steady-state of Budget Equations for SBL
Total Energy Deardorff (1970)
Steady-State Form of the Budget Equations Our model Old classical theory Turbulent temperature diffusivity
vs.
Turbulent Prandtl Number
Total Budget Equations: BL-case in Presents of Gravity Waves
vs. (Waves)
Turbulent Prandtl Number
Anisotropy vs.
vs.
vs. (Waves)
Conclusions - Total turbulent energy (potential and kinetic) is conserved - No critical Richardson number - Reasonable turbulent Prandtl number from theory - Reasonable explanation of scattering of the observational data by the influence of the largescale internal gravity waves.
References Ø Elperin, T. , Kleeorin, N. , Rogachevskii, I. , and Zilitinkevich, S. 2002 Formation of large-scale semi-organized structures in turbulent convection. Phys. Rev. E, 66, 066305 (1 --15) Ø Elperin, T. , Kleeorin, N. , Rogachevskii, I. , and Zilitinkevich, S. 2006 Tangling turbulence and semi-organized structures in convective boundary layers. Boundary Layer Meteorology, 119, 449 -472. Ø Zilitinkevich, S. , Elperin, T. , Kleeorin, N. , and Rogachevskii, I, 2007 "Energy- and flux-budget (EFB) turbulence closure model for stably stratified flows. Boundary Layer Meteorology, Part 1: steady-state homogeneous regimes. Boundary Layer Meteorology, 125, 167 -191. Ø Zilitinkevich S. , Elperin T. , Kleeorin N. , Rogachevskii I. , Esau I. , Mauritsen T. and Miles M. , 2008, "Turbulence Energetics in. Stably Stratified Geophysical Flows: Strong and Weak Mixing Regimes". Quarterly Journal of Royal Meteorological Societyv. 134, 793 -799.
Many Thanks to
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Tturbulence and Anisotropy Isotropy Anisotropy
Total Energy
Anisotropy in Observations Isotropy
Equations for Atmospheric Flows
Budget Equation for TKE Balance in R-space Balance in K-space ( Heisenberg, 1948 ) Isotropy
Mean Profiles
Turbulent Prandtl Number
Total Budget Equations Ø Turbulent kinetic energy: Ø Potential temperature fluctuations: Ø Flux of potential temperature :
Boundary Layer Height Momentum flux derived Heat flux derived
Calculation
vs.
Total Budget Equations Ø Turbulent kinetic energy: Ø Potential temperature fluctuations: Ø Flux of potential temperature :
vs.
Temperature Forecasting Curve
Anisotropy vs.