A dual mass flux scheme for shallow cumulus convection Results for GCSS RICO Roel Neggers, Martin Köhler, Anton Beljaars.

Slides:



Advertisements
Similar presentations
Boundary Layer Verification ECMWF training course May 2010 Maike Ahlgrimm.
Advertisements

Introduction Irina Surface layer and surface fluxes Anton
1 Numerical Weather Prediction Parameterization of diabatic processes Convection III The ECMWF convection scheme Christian Jakob and Peter Bechtold.
Hirlam Physics Developments Sander Tijm Hirlam Project leader for physics.
Veldhoven, Large-eddy simulation of stratocumulus – cloud albedo and cloud inhomogeneity Stephan de Roode (1,2) & Alexander Los (2)
A new unified boundary-layer scheme for RACMO: The DualM-TKE scheme Stephan de Roode with contributions from Geert Lenderink Roel Neggers Reinder Ronda.
LARGE EDDY SIMULATION Chin-Hoh Moeng NCAR.
Pedro M. M. Soares* Pedro M. A. Miranda* João Teixeira^ *University of Lisbon, CGUL, IDL, Lisbon, Portugal ^Jet Propulsion Laboratory – California Institute.
Evaluation of HARMONIE using a single column model in the KNMI
Parameterization of convective momentum transport and energy conservation in GCMs N. McFarlane Canadian Centre for Climate Modelling and Analysis (CCCma.
How to represent subgrid atmospheric processes in Climate |Models Multiscale Physics Regional Climate Division A. Pier Siebesma Faculty.
The Problem of Parameterization in Numerical Models METEO 6030 Xuanli Li University of Utah Department of Meteorology Spring 2005.
Sc-Cu transition CPT Goal: Improve the representation of the cloudy boundary layer in global weather/climate models with a focus on the subtropical stratocumulus.
Low clouds in the atmosphere: Never a dull moment Stephan de Roode (GRS) stratocumulus cumulus.
Simulation of Cloud Droplets in Parameterized Shallow Cumulus During RICO and ICARTT Knut von Salzen 1, Richard Leaitch 2, Nicole Shantz 3, Jonathan Abbatt.
The role of the mean relative humidity on the dynamics of shallow cumuli - LES Sensitivity experiments Stephan de Roode (KNMI/IMAU) Simon Axelsen (IMAU)
Mass Flux Concepts:  Pier Siebesma KNMI, De Bilt The Netherlands Mass flux approximations Entraining Plume model Mixing.
The Centre for Australian Weather and Climate Research A partnership between CSIRO and the Bureau of Meteorology The Effect of Turbulence on Cloud Microstructure,
Relationships between wind speed, humidity and precipitating shallow cumulus convection Louise Nuijens and Bjorn Stevens* UCLA - Department of Atmospheric.
Observational study of the transition from unbroken marine boundary layer stratocumulus to the shallow cumulus regime Irina Sandu and Bjorn Stevens Max-Planck-Institut.
Why are we here, at the UCLA Conf. Center in June 2005? What is the best way of representing the physics of the atmospheric PBL in weather and climate.
GFS Deep and Shallow Cumulus Convection Schemes
WG on role of PBL in deep convection Thanks to all WG participants for a fine discussion and Steve Klein for note-taking.
The scheme: A short intro Some relevant case results Why a negative feedback? EDMF-DualM results for the CFMIP-GCSS intercomparison case: Impacts of a.
Current issues in GFS moist physics Hua-Lu Pan, Stephen Lord, and Bill Lapenta.
1 Dry Convection Phenomenology, Simulation and Parameterization of Atmospheric Convection Pier Siebesma Yesterday: “Dry” Atmospheric Convection Today:
Length Scale analysis of the transition from shallow to deep convection João Paulo A. Martins (1) Pedro M. A. Miranda (1) Pedro M. M. Soares (1) João Teixeira.
Large-Eddy Simulation of a stratocumulus to cumulus transition as observed during the First Lagrangian of ASTEX Stephan de Roode and Johan van der Dussen.
Scientific Advisory Committee Meeting, November 25-26, 2002 Large-Eddy Simulation Andreas Chlond Department Climate Processes.
GardeGarde Designing unified convection parameterizations: two proposals related to equation sets and entrainment. Jean-Marcel Piriou, Météo-France. GCSS.
T q sat(T) qtqt. (T,q t ) Statistical cloud scheme Determine cloud cover and liquid water using the sub-grid variability :
The representation of stratocumulus with eddy diffusivity closure models Stephan de Roode KNMI.
Can we use a statistical cloud scheme coupled to convection and moist turbulence parameterisations to simulate all cloud types? Colin Jones CRCM/UQAM
A dual mass flux framework for boundary layer convection Explicit representation of cloud base coupling mechanisms Roel Neggers, Martin Köhler, Anton Beljaars.
Vertical Structure of the Tropical Troposphere (including the TTL) Ian Folkins Department of Physics and Atmospheric Science Dalhousie University.
Case Study Example 29 August 2008 From the Cloud Radar Perspective 1)Low-level mixed- phase stratocumulus (ice falling from liquid cloud layer) 2)Brief.
Stephan de Roode (KNMI) Entrainment in stratocumulus clouds.
Budgets of second order moments for cloudy boundary layers 1 Systematische Untersuchung höherer statistischer Momente und ihrer Bilanzen 1 LES der atmosphärischen.
Yanjun Jiao and Colin Jones University of Quebec at Montreal September 20, 2006 The Performance of the Canadian Regional Climate Model in the Pacific Ocean.
The ASTEX Lagrangian model intercomparison case Stephan de Roode and Johan van der Dussen TU Delft, Netherlands.
The Role of Virtual Tall Towers in the Carbon Dioxide Observation Network Martha Butler The Pennsylvania State University ChEAS Meeting June 5-6, 2006.
Large Eddy Simulation of PBL turbulence and clouds Chin-Hoh Moeng National Center for Atmospheric Research.
II: Progress of EDMF, III: comparison/validation of convection schemes I: some other stuff Sander Tijm (HIRLAM) Contributions of: Siebesma, De Rooy, Lenderink,
Forecast simulations of Southeast Pacific Stratocumulus with CAM3 and CAM3-UW. Cécile Hannay (1), Jeffrey Kiehl (1), Dave Williamson (1), Jerry Olson (1),
Lecture 15, Slide 1 Physical processes affecting stratocumulus Siems et al
Evaluating forecasts of the evolution of the cloudy boundary layer using radar and lidar observations Andrew Barrett, Robin Hogan and Ewan O’Connor Submitted.
1. Introduction Boundary-layer clouds are parameterized in general circulation model (GCM), but simulated in Multi-scale Modeling Framework (MMF) and.
Boundary Layer Clouds.
Improvement of the EDMF Scheme using Kain Fristch approach for Meso-NH and AROME Improvement of the Eddy-Diffusivity Mass Flux scheme using Kain-Fritsch.
Georg A. Grell (NOAA / ESRL/GSD) and Saulo R. Freitas (INPE/CPTEC) A scale and aerosol aware stochastic convective parameterization for weather and air.
1 Making upgrades to an operational model : An example Jongil Han and Hua-Lu Pan NCEP/EMC GRAPES-WRF Joint Workshop.
PBL schemes for ICON: CGILS test Martin Köhler (DWD) Dmitrii Mironov, Matthias Raschendorfer, Ekaterina Machulskaya (DWD) Roel Neggers (KNMI)  Prognostic.
LES Intercomparison Case of Precipitating Shallow Cumulus Margreet van Zanten, Bjorn Stevens, Pier Siebesma, Louise Nuijens A.S. Ackerman, H. Jiang, D.
Continuous treatment of convection: from dry thermals to deep precipitating convection J.F. Guérémy CNRM/GMGEC.
A Thermal Plume Model for the Boundary Layer Convection: Representation of Cumulus Clouds C. RIO, F. HOURDIN Laboratoire de Météorologie Dynamique, CNRS,
Development and testing of the moist second-order turbulence-convection model including transport equations for the scalar variances Ekaterina Machulskaya.
Stratocumulus-topped Boundary Layer
MODELING OF SUBGRID-SCALE MIXING IN LARGE-EDDY SIMULATION OF SHALLOW CONVECTION Dorota Jarecka 1 Wojciech W. Grabowski 2 Hanna Pawlowska 1 Sylwester Arabas.
Stephan de Roode The art of modeling stratocumulus clouds.
Shallow Moist Convection Basic Moist Thermodynamics Remarkable Features of Moist Convection Shallow Cumulus (Stratocumulus) Courtesy: Dave Stevens.
A simple parameterization for detrainment in shallow cumulus Hirlam results for RICO Wim de Rooy & Pier Siebesma Royal Netherlands Meteorological Institute.
Pier Siebesma Today: “Dry” Atmospheric Convection
Parametrization of turbulent fluxes in the outer layer Irina Sandu
Arome SCM mini-intercomparison
Shallow Cumulus Growth, (an idealized view)
Theories of Mixing in Cumulus Convection
Analysis of Parameterization in Single-Column Model
thanks to Pier Siebesma, Adrian Tompkins, Anton Beljaars
Entrainment rates in stratocumulus computed from a 1D TKE model
transport equations for the scalar variances
Presentation transcript:

A dual mass flux scheme for shallow cumulus convection Results for GCSS RICO Roel Neggers, Martin Köhler, Anton Beljaars

Contents The DualM scheme An extension to EDMF for shallow cumulus convection A *VERY* short overview (more on Thursday) RICO results Mean state Equilibration Updraft profiles & fluxes Variances Cloudy state & precipitation Experiments with an entrainment efficiency closure for cumulus

Eddy diffusivity - mass flux (EDMF) decomposition for turbulent transport The current PBL scheme (cy30r1) Siebesma et al. (Submitted to JAS) Currently applied to dry PBL and stratocumulus topped PBL only Goal: upgrade EDMF to enable representation of i) shallow cumulus convection ii) transitions What is needed? K moist updraft K dry updraft

The dual mass flux scheme – main EDMF upgrades Moist updrafts Flexible area partitioning a up Dry updrafts K diffusion a 1 up a 2 up h z0z0 1 - a up I. Multiple updrafts N=2: dry updrafts stopping at cloud base, moist updrafts continuing as cumulus clouds. II. Flexible updraft area fractions Closure as a function of model state Facilitates representation of i) gradual regime transitions, ii) coupling of cumuli to mixed layer III. Extension of EDMF partitioning into the statistical cloud scheme A matching bimodal PDF (passive clouds and updraft clouds) Consistent treatment of PBL transport and cloudiness IV. Top-entrainment efficiency closures for cumulus V. … and many more … Explicit treatment of transport across strong unresolved gradients ( cu inversion, transition layer)

Flexible updraft area fractions facilitate representation of gradual regime transitions E LCL h  h EE M2M2 M1M1 Stratocumulus Shallow cumulus Dry convection M1M1 M2M2 a2a2 a1a1 Moist and dry updrafts can co-exist at any time

Closure of the flexible updraft area fractions Explicit representation of the coupling between cumulus updrafts and mixed-layer III. Vertical integration of updraft budgets then reconstructs the joint-PDF I. First guess of cloud core fraction at cloud base, using local variance scaling II. These fractions are subsequently used in surface initialization of updrafts Knowledge of how many updrafts manage to reach LFC is `back-stitched` into the partitioning and initialization of the updrafts This carries information on cloud base transition layer properties

RICO results – mean state

RICO results – cloudy state DualM cy30r1

RICO results - equilibration The flexibility of a and its closure introduce a valve mechanism in M, always acting to equilibrate the mixed layer budgets Area fraction is retained in the updraft mass flux

RICO results - updrafts Lateral entrainment closure makes differently initialized updrafts diverge with height.

RICO results - fluxes LES

RICO results – variance I Used in statistical cloud scheme

RICO results – variance II qtqt ll Updraft PDF Diffusive PDF Lewellen & Yoh (JAS,1993) Extension of EDMF into the modelling of clouds – a bimodal distribution Relations between moments

RICO results – variance II Closure of updraft variance

RICO results – bimodal clouds

Passive clouds Updraft clouds

RICO results - precipitation

How important is it? RICOBOMEX

RICO results – entrainment efficiency experiments RICOATEX Wyant et al. (1997) All flux into cu inversion is explicitly modelled through the K-component of EDMF

Summary A shallow cumulus extension is formulated for EDMF More complexity is added to the system of equations, in various new ways: - multiple transporting updrafts - flexible updraft area fractions - EDMF partitioning is extended into the PBL cloud scheme (a bimodal PDF) Assuming flexible updraft area fractions facilitates representation of gradual regime transitions Closure of the updraft area fractions allows explicit representation of the coupling between cumuli and the mixed layer, introducing a valve mechanism in the cumulus mass flux The mean, turbulent and cloud structure of the RICO short composite case is reproduced Precipitation appears to be an important player in the SCM thermodynamic budgets A more detailed discussion of model physics on Thursday…