Implementation of the quasi-normal scale elimination (QNSE) theory of turbulence in a weather prediction model HIRLAM Veniamin Perov¹, Boris Galperin².

Slides:



Advertisements
Similar presentations
Basics of numerical oceanic and coupled modelling Antonio Navarra Istituto Nazionale di Geofisica e Vulcanologia Italy Simon Mason Scripps Institution.
Advertisements

Parametrization of surface fluxes: Outline
Parametrization of PBL outer layer Martin Köhler Overview of models Bulk models local K-closure K-profile closure TKE closure.
Parametrization of PBL outer layer Irina Sandu and Martin Kohler
Institut für Meteorologie und Klimatologie Universität Hannover
Section 2: The Planetary Boundary Layer
Training course: boundary layer IV Parametrization above the surface layer (layout) Overview of models Slab (integral) models K-closure model K-profile.
A drag parameterization for extreme wind speeds that leads to improved hurricane simulations Gerrit Burgers Niels Zweers Vladimir Makin Hans de Vries EMS.
THE PARAMETERIZATION OF STABLE BOUNDARY LAYERS BASED ON CASES-99 Zbigniew Sorbjan Marquette University, Milwaukee Zbigniew Sorbjan Marquette University,
Direct numerical simulation study of a turbulent stably stratified air flow above the wavy water surface. O. A. Druzhinin, Y. I. Troitskaya Institute of.
Atmospheric Analysis Lecture 3.
0.1m 10 m 1 km Roughness Layer Surface Layer Planetary Boundary Layer Troposphere Stratosphere height The Atmospheric (or Planetary) Boundary Layer is.
Introduction to surface ocean modelling SOPRAN GOTM School Warnemünde: Hans Burchard Baltic Sea Research Institute Warnemünde, Germany.
Internal Gravity Waves and Turbulence Closure Model for SBL Sergej Zilitinkevich Division of Atmospheric Sciences, Department of Physical Sciences University.
Vertical Mixing Parameterizations and their effects on the skill of Baroclinic Tidal Modeling Robin Robertson Lamont-Doherty Earth Observatory of Columbia.
Turbopause and Gravity Waves Han-Li Liu HAO National Center for Atmospheric Research.
Verification of Numerical Weather Prediction systems employed by the Australian Bureau of Meteorology over East Antarctica during the summer season.
Atmospheric turbulence Richard Perkins Laboratoire de Mécanique des Fluides et d’Acoustique Université de Lyon CNRS – EC Lyon – INSA Lyon – UCBL 36, avenue.
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association INSTITUTE OF METEOROLOGY AND CLIMATE RESEARCH,
SMHI in the Arctic Lars Axell Oceanographic Research Unit Swedish Meteorological and Hydrological Institute.
Prediction of Atlantic Tropical Cyclones with the Advanced Hurricane WRF (AHW) Model Jimy Dudhia Wei Wang James Done Chris Davis MMM Division, NCAR Jimy.
Verification and Case Studies for Urban Effects in HIRLAM Numerical Weather Forecasting A. Baklanov, A. Mahura, C. Petersen, N.W. Nielsen, B. Amstrup Danish.
Equations that allow a quantitative look at the OCEAN
Momentum Equations in a Fluid (PD) Pressure difference (Co) Coriolis Force (Fr) Friction Total Force acting on a body = mass times its acceleration (W)
Modeling the upper ocean response to Hurricane Igor Zhimin Ma 1, Guoqi Han 2, Brad deYoung 1 1 Memorial University 2 Fisheries and Oceans Canada.
Modeling the Atmospheric Boundary Layer (2). Review of last lecture Reynolds averaging: Separation of mean and turbulent components u = U + u’, = 0 Intensity.
How Small-Scale Turbulence Sets the Amplitude and Structure of Tropical Cyclones Kerry Emanuel PAOC.
Chapter 6 Introduction to Forced Convection:
Some Aspects of Parameterisation in Small Scaled Models Thomas Roschke German Weather Service Department of Aviation Meteorology.
Estimating the Optimal Location of a New Wind Farm based on Geospatial Information System Data Dec Chungwook Sim.
Pre-operational testing of Aladin physics Martina Tudor 1, Ivana Stiperski 1, Vlasta Tutiš 1, Dunja Drvar 1 and Filip Vana 2 1 Meteorological and Hydrological.
CITES 2005, Novosibirsk Modeling and Simulation of Global Structure of Urban Boundary Layer Kurbatskiy A. F. Institute of Theoretical and Applied Mechanics.
INTERCOMPARISON – HIRLAM vs. ARPA-SIM CARPE DIEM AREA 1 Per Kållberg Magnus Lindskog.
STUDIES OF NONLINEAR RESISTIVE AND EXTENDED MHD IN ADVANCED TOKAMAKS USING THE NIMROD CODE D. D. Schnack*, T. A. Gianakon**, S. E. Kruger*, and A. Tarditi*
Conservation of Salt: Conservation of Heat: Equation of State: Conservation of Mass or Continuity: Equations that allow a quantitative look at the OCEAN.
NATO ASI Conference, Kyiv MODELING AND SIMULATION OF TURBULENT PENETRATIVE CONVECTION AND POLLUTANT DISPERSION ABOVE THE URBAN HEAT ISLAND IN STABLY.
Modeling and Evaluation of Antarctic Boundary Layer
NWP models. Strengths and weaknesses. Morten Køltzow, met.no NOMEK
ITSC-1227 February-5 March 2002 Use of advanced infrared sounders in cloudy conditions Nadia Fourrié and Florence Rabier Météo France Acknowledgement G.
Page 1© Crown copyright Modelling the stable boundary layer and the role of land surface heterogeneity Anne McCabe, Bob Beare, Andy Brown EMS 2005.
ARSM -ASFM reduction RANSLESDNS 2-eqn. RANS Averaging Invariance Application DNS 7-eqn. RANS Body force effects Linear Theories: RDT Realizability, Consistency.
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss Component testing of the COSMO model’s turbulent diffusion.
Mattias Mohr, Johan Arnqvist, Hans Bergström Uppsala University (Sweden) Simulating wind and turbulence profiles in and above a forest canopy using the.
Processes in the Planetary Boundary Layer
Numerical experiments with the COSMO Model boundary layer scheme based on a parcel displacement scheme for a turbulent length scale Veniamin Perov and.
A Case Study of Decoupling in Stratocumulus Xue Zheng MPO, RSMAS 03/26/2008.
Parameterization of the Planetary Boundary Layer -NWP guidance Thor Erik Nordeng and Morten Køltzow NOMEK 2010 Oslo 19. – 23. April 2010.
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss Analyzing the TKE budget of the COSMO model for the LITFASS-2003.
Implementation of a boundary layer heat flux parameterization into the Regional Atmospheric Modeling System Erica McGrath-Spangler Dept. of Atmospheric.
OSEs with HIRLAM and HARMONIE for EUCOS Nils Gustafsson, SMHI Sigurdur Thorsteinsson, IMO John de Vries, KNMI Roger Randriamampianina, met.no.
The effect of tides on the hydrophysical fields in the NEMO-shelf Arctic Ocean model. Maria Luneva National Oceanography Centre, Liverpool 2011 AOMIP meeting.
1 LES of Turbulent Flows: Lecture 7 (ME EN ) Prof. Rob Stoll Department of Mechanical Engineering University of Utah Spring 2011.
HYBRID LARGE EDDY SIMULATION/REYNOLDS AVERAGED NAVIER-STOKES FORMULATION FOR NUMERICAL WEATHER PREDICITON H. A. Hassan North Carolina State University,
Model calculationsMeasurements An extreme precipitation event during STOPEX I J.Reuder and I. Barstad Geophysical Institute, University of Bergen, Norway.
HIRLAM coupled to the ocean wave model WAM. Verification and improvements in forecast skill. Morten Ødegaard Køltzow, Øyvind Sætra and Ana Carrasco. The.
Verification of wind gust forecasts Javier Calvo and Gema Morales HIRMAM /ALADIN ASM Utrecht May 11-15, 2009.
A revised formulation of the COSMO surface-to-atmosphere transfer scheme Matthias Raschendorfer COSMO Offenbach 2009 Matthias Raschendorfer.
The Sea Surface Temperature in operational NWP model ALADIN
The Sea Surface Temperature in operational NWP model ALADIN
Pier Siebesma Today: “Dry” Atmospheric Convection
Boris Galperin Univ. South Florida
C. F. Panagiotou and Y. Hasegawa
Turbulence closure problem
“Consolidation of the Surface-to-Atmosphere Transfer-scheme: ConSAT
Multiscale aspects of cloud-resolving simulations over complex terrain
Vertical resolution of numerical models
A hybrid model for the wind profile
Lecture 1: Introduction
NWP Strategy of DWD after 2006 GF XY DWD Feb-19.
  Robin Robertson Lamont-Doherty Earth Observatory
Presentation transcript:

Implementation of the quasi-normal scale elimination (QNSE) theory of turbulence in a weather prediction model HIRLAM Veniamin Perov¹, Boris Galperin² and Semion Sukoriansky³ 1.Swedish Meteorological and Hydrological Institute (SMHI), Norrköping, Sweden 2. College of Marine Science, University of South Florida, St. Petersburg, Florida, USA 3. Ben-Gurion University of the Negev, Beer-Sheva, Israel

Numerical weather prediction (NWP) models involve eddy viscosity and eddy diffusivity, Km and Kh, that account for unresolved turbulent mixing and diffusion. The most sophisticated turbulent closure models used today for NWP belong to the family of Reynolds stress models. These models are formulated for the physical space variables; they consider a hierarchy of turbulent correlations and employ a rational way of its truncation. In the process, unknown correlation are related to the known ones via “closure assumptions” that are based upon preservation of tensorial properties and the principle of invariant modelling

according to which the constants in the closure relationships are universal Although a great deal of progress has been achieved with Reynolds stress closure models over the years, these are still situations in which these models fail. The most difficult flows for the Reynolds stress modelling are those with anisotropy and waves because these processes are scale-dependent and cannot be included in the closure assumptions that pertain to ensemble-averages quantities. Here we employ an alternative approach of deriving expressions for Km and Kh using the spectral space presentation. The spectral model produces expressions for Km and Kh based upon a self-consistent procedure of small-scale modes elimination.

This procedure is based upon the quasi-Gaussian mapping of the velocity and temperature using the Langevun equations. Turbulence and waves are treated as one entity and the effect of the internal waves is easily identifiable. When averaging is extended to all scales, the method yields a Reynolds-averaged, Navier-Stokes based model. The details can be found in the paper “A quasinormal scale elimination model of turbulent flows with stable stratification”, Phys. Fluids, 17, , 2005, by Sukoriansky S, Galperin B. and Staroselsky I.

Results from the theory The turbulent coefficients are recast in terms of gradient Richardson number Ri = N 2 / S 2 or Froude number Fr =  / NK Normalized turbulent exchange coefficients as functions of Ri and Fr. For Ri>0.1, both vertical viscosity and diffusivity decrease, with the diffusivity decreasing faster than the viscosity (“residual” mixing due to effect of IGW?)  Horizontal mixing increases with Ri. The model accounts for flow anisotropy.  The crossover from neutral to stratified flow regime is replicated. No critical Ri.

Stability functions from the QNSE model and from the Mellor-Yamada model modified by Galperin et al. (1988)

Comparison with experimental data Vertical turbulent Prandtl number as a function of Ri. Data points are laboratory measurements by Huq and Stewart (2004) ; solid line represents our model’s results. Inverse Prandtl number k z / z as a function of Ri. Experimental data points are from Monti et al. (2002).

New K-  model : In our model Detering & Etlin, 1985 introduced correction to C 1 due to the Earth rotation We generalized it to include stratification: The constants are: The model is implemented in the 1D version of the weather forecast model HIRLAM where

Neutral ABL Comparison with Leipzig wind profile Comparison with Leipzig wind profile

Comparison with CASES-99

Comparison with BASE Comparison with BASE

Testing in the numerical weather prediction system HIRLAM  NWP system HIRLAM: High Resolution Limited Area Model  Covers the North-East Atlantic, Europe, and Greenland  Hydrostatic model; 438x336 points; 22km x 22km resolution  40 vertical levels  Lateral boundary conditions are from ECMWF operations  Massive data assimilation: over 1000 stations all over Europe  Data assimilation cycle is 6 hours  From each 00, 06, 12, 18 UTC, a +48 hours forecast is run  Total: 120, +48 h forecasts in one month (January 2005)  We replace K m and K h for stable stratification only; run parallel experiment; analyze the difference (new-reference)  Region of interest: Scandinavia

HIRLAM turbulence K-l scheme

Results (versions before 6.2) : -Positive bias in the wind direction, accompanied by too strong near surface winds - Too fast deepening and too slow filling of cyclones, making HIRLAM too active towards the end of the forecast period

HIRLAM turbulence K-l scheme Increasing of the vertical mixing of momentum under stable stratif. Verification score becames better, but Intercomparison in GABLS shows very deep BL and a wind profile has its maximum at the wrong place (too high)

Modification of HIRLAM K-l scheme

Surface sensible heat flux: New-Reference Red – positive Blue - negative

Surface latent heat flux: New-Reference

Surface U-momentum flux: New-Reference

Surface V-momentum flux: New-Reference

Cross-section: Difference in TKE

Cross-section: Difference in temperature

Conclusions Anisotropic turbulent viscosities and diffusivities are in good agreement with experimental data Anisotropic turbulent viscosities and diffusivities are in good agreement with experimental data The model recognizes the horizontal-vertical anisotropy introduces by stable stratification and provides expressions for the horizontal and vertical turbulent viscosities and diffusivities. This is a real possibility to include 3-D turbulence in NWP and mesoscale models The model recognizes the horizontal-vertical anisotropy introduces by stable stratification and provides expressions for the horizontal and vertical turbulent viscosities and diffusivities. This is a real possibility to include 3-D turbulence in NWP and mesoscale models Theory has been implemented in 1-D K-ε and K-l models of stratified ABL Theory has been implemented in 1-D K-ε and K-l models of stratified ABL Good agreement with BASE, SHEBA and CASES99 data sets has been found in 1-D model for cases of moderate and strong stratification Good agreement with BASE, SHEBA and CASES99 data sets has been found in 1-D model for cases of moderate and strong stratification Theory has been implemented in K-l scheme of 3-D NWP model HIRLAM Theory has been implemented in K-l scheme of 3-D NWP model HIRLAM The new K-l scheme improves predictive skills of mean sea level pressure and 2M temperature for +48h weather forecasts over Scandinavia (stable BL) for January 2005 The new K-l scheme improves predictive skills of mean sea level pressure and 2M temperature for +48h weather forecasts over Scandinavia (stable BL) for January 2005