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Internal Gravity Waves and Turbulence Closure Model for SBL

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

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Internal Gravity Waves and Turbulence Closure Model for SBL

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  1. 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

  2. Boussinesq Approximation

  3. Laminar and Turbulent Flows Laminar Boundary Layer Turbulent Boundary Layer

  4. Why Turbulence? Why Not DNS? Number degrees of freedom

  5. Turbulent Eddies

  6. Laboratory Turbulent Convection After averaging Before averaging

  7. Velocity Fields

  8. SBL Equations

  9. Total Energy

  10. Total Budget Equations: BL-case

  11. Total Budget Equations for SBL

  12. Total Budget Equations: BL-case

  13. Total Energy The turbulent potential energy: The source:

  14. Steady-state of Budget Equations for SBL

  15. Deardorff (1970) Total Energy

  16. Steady-State Form of the Budget Equations Our model Old classical theory Turbulent temperature diffusivity

  17. vs.

  18. Turbulent Prandtl Number

  19. Total Budget Equations: BL-casein Presents of Gravity Waves

  20. vs. (Waves)

  21. Turbulent Prandtl Number

  22. Anisotropy vs.

  23. vs.

  24. vs. (Waves)

  25. 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 large- scale internal gravity waves.

  26. References • 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) • 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. • 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. • Zilitinkevich S., Elperin T., Kleeorin N., Rogachevskii I., Esau I., Mauritsen T. and Miles M.,2008, "Turbulence Energetics inStably Stratified Geophysical Flows: Strong and Weak Mixing Regimes". Quarterly Journal of Royal Meteorological Societyv. 134, 793-799.

  27. Many Thanks to

  28. THE END

  29. Tturbulence and Anisotropy Isotropy Anisotropy

  30. Total Energy

  31. Anisotropy in Observations Isotropy

  32. Equations for Atmospheric Flows

  33. Budget Equation for TKE Balance in K-space Balance in R-space ( Heisenberg, 1948 ) Isotropy

  34. Mean Profiles

  35. Turbulent Prandtl Number

  36. Total Budget Equations • Turbulent kinetic energy: • Potential temperature fluctuations: • Flux of potential temperature :

  37. Momentum flux derived Heat flux derived Boundary Layer Height

  38. Calculation

  39. vs.

  40. Total Budget Equations • Turbulent kinetic energy: • Potential temperature fluctuations: • Flux of potential temperature :

  41. vs.

  42. Temperature Forecasting Curve

  43. Anisotropy vs.

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