WG on role of PBL in deep convection Thanks to all WG participants for a fine discussion and Steve Klein for note-taking.

Slides:



Advertisements
Similar presentations
What’s quasi-equilibrium all about?
Advertisements

Convection plans Alison Stirling.
Some questions on convection that could be addressed through another UK field program centered at Chilbolton Dan Kirshbaum 1.
LARGE EDDY SIMULATION Chin-Hoh Moeng NCAR.
The Problem of Parameterization in Numerical Models METEO 6030 Xuanli Li University of Utah Department of Meteorology Spring 2005.
Observed Updraft & Mass Flux in Shallow Cumulus at ARM Southern Great Plains site Preliminary results Yunyan Zhang, Steve Klein & Pavlos Kollias CFMIP/GCSS.
Relationships between wind speed, humidity and precipitating shallow cumulus convection Louise Nuijens and Bjorn Stevens* UCLA - Department of Atmospheric.
1 COPS Workshop 25 Sept 2006 UK COPS: Convection and Transport in Complex Terrain (CATICT) Alan Blyth and Stephen Mobbs.
Evaluating mass flux closures using cloud resolving model simulations of deep convection Jennifer Fletcher and Chris Bretherton COGS talk May 7, 2009 Evaluating.
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
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.
Geophysical Fluid Dynamics Laboratory Review June 30 - July 2, 2009 Geophysical Fluid Dynamics Laboratory Review June 30 - July 2, 2009.
A new Convection Parameterization: Some Achievements and Some Challenges Hans-F Graf, Cambridge Till M Wagner, Oxford (was Cambridge ) IPAM, UCLA, May.
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.
Scientific Advisory Committee Meeting, November 25-26, 2002 Large-Eddy Simulation Andreas Chlond Department Climate Processes.
Implementation of IPHOC in VVCM: Tests of GCSS Cases Anning Cheng 1,2 and Kuan-Man Xu 2 1.AS&M, Inc. 2.Science Directorate, NASA Langley Research Center.
1 Numerical Weather Prediction Parameterization of diabatic processes Convection III The ECMWF convection scheme Christian Jakob and Peter Bechtold.
The National Environmental Agency of Georgia L. Megrelidze, N. Kutaladze, Kh. Kokosadze NWP Local Area Models’ Failure in Simulation of Eastern Invasion.
Mesoscale Modeling Review the tutorial at: –In class.
29th EWGLAM meeting, Dubrovnik, October 2007 ALARO Physics developments Neva Pristov LACE Working group for physics.
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.
Convective Parameterization Options
Horizontal Mixing and Convection. 1st order prognostic PDE Q is the quadratic fluid dynamics term called the “Dynamical Core”. F is the Forcing “Physics”
HIRLAM 1D model tool B.H. Sass December Overview 1) Introduction 1) Introduction 2) History of 1D-model(s) 2) History of 1D-model(s) 3) Basics of.
Update on model developments: Meteo-France NWP model / clouds and turbulence CLOUDNET workshop / Paris 27-28/05/2002 Jean-Marcel Piriou Centre National.
DYMECS: Dynamical and Microphysical Evolution of Convective Storms (NERC Standard Grant) University of Reading: Robin Hogan, Bob Plant, Thorwald Stein,
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.
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),
CCSM Atmospheric Model Working Group Summary J. J. Hack, D. A Randall AMWG Co-Chairs CCSM Workshop, 28 June 2001 CCSM Workshop, 28 June 2001.
A Numerical Study of Early Summer Regional Climate and Weather. Zhang, D.-L., W.-Z. Zheng, and Y.-K. Xue, 2003: A Numerical Study of Early Summer Regional.
Treatment of Small Scale Land Surface Heterogeneity for Atmospheric Modelling (SSSAM) Günther Heinemann (1) and Michael Kerschgens (2) 1 Meteorologisches.
1 Rachel Capon 04/2004 © Crown copyright Met Office Unified Model NIMROD Nowcasting Rachel Capon Met Office JCMM.
Workshop on Tropical Biases, 28 May 2003 CCSM CAM2 Tropical Simulation James J. Hack National Center for Atmospheric Research Boulder, Colorado USA Collaborators:
New CRM diagnostics dedicated to convective parameterization J-I Yano P. Bechtold, J.-P. Chaboureau, F. Guichard, J.-L. Redelsperger and J.-P. Lafore LMD,
LMDZ Single Column Model + what is it ? + why is it interesting ? + List of 1D cases + how to install and run it ? M-P Lefebvre and LMDZ team.
Mesoscale energy spectra for a simulated squall line Fuqing Zhang Rich Rotunno Y. Qiang Sun Groupmeeting
A dual mass flux scheme for shallow cumulus convection Results for GCSS RICO Roel Neggers, Martin Köhler, Anton Beljaars.
Modeling and Evaluation of Antarctic Boundary Layer
APR CRM simulations of the development of convection – some sensitivities Jon Petch Richard Forbes Met Office Andy Brown ECMWF October 29 th 2003.
Continuous treatment of convection: from dry thermals to deep precipitating convection J.F. Guérémy CNRM/GMGEC.
The Transition from Shallow to Deep Convection over Land: A Diurnal-cycle Analysis of ARM SGP Observations Stephen A. Klein and Yunyan Zhang (LLNL) October.
A Thermal Plume Model for the Boundary Layer Convection: Representation of Cumulus Clouds C. RIO, F. HOURDIN Laboratoire de Météorologie Dynamique, CNRS,
Vincent N. Sakwa RSMC, Nairobi
Convective Parameterization in NWP Models Jack Kain And Mike Baldwin.
African easterly wave dynamics in a full-physics numerical model. Gareth Berry and Chris Thorncroft. University at Albany/SUNY, Albany, NY,USA.
Implementation of a boundary layer heat flux parameterization into the Regional Atmospheric Modeling System Erica McGrath-Spangler Dept. of Atmospheric.
Radiative-Convective Model. Overview of Model: Convection The convection scheme of Emanuel and Živkovic-Rothman (1999) uses a buoyancy sorting algorithm.
Ongoing work to improve convection in the UM Keith Williams (most of the work by Martin Willett) WGNE-31, 28/04/16.
Transport Working Group
Performance of ALARO0 baseline in pre-operational testing
Shifting the diurnal cycle of parameterized deep convection over land
Application Of KF-Convection Scheme In 3-D Chemical Transport Model
On the role of entrainment at the grey zone scales
Seamless turbulence parametrization across model resolutions
Multiscale aspects of cloud-resolving simulations over complex terrain
WP2.1a,b High Resolution Simulations of Convection
April 12, 2018 Hing Ong ATM 419/563 Cumulus parameterization: Kain-Fritsch scheme and other mass-flux schemes This lecture is designed for students who.
National Center for Atmospheric Research
Group interests RICO data required
Cathy Hohenegger 1,2 Linda Schlemmer 1,2 Bjorn Stevens 1
What about the last years?
Models of atmospheric chemistry
Characterizing the response of simulated atmospheric boundary layers to stochastic cloud radiative forcing Robert Tardif, Josh Hacker (NCAR Research Applications.
Consortium Meeting June 14th 2012
Convective Parameterization in NWP Models
Kurowski, M .J., K. Suselj, W. W. Grabowski, and J. Teixeira, 2018
Group interests RICO data in support of studies
Presentation transcript:

WG on role of PBL in deep convection Thanks to all WG participants for a fine discussion and Steve Klein for note-taking.

Progress in past decade PBL and transition-layer dynamics solve the mass flux closure/triggering problem for parameterization of shallow (and likely deep) Cu. CAPE seen to be a necessary condition but not the control parameter. CRM/LES can now model Cu ensemble/PBL interaction with enough realism to help us to improve parameterization. We have lots of repeatable observations of the diurnal cycle of shallow and deep Cu clouds and regime transitions using radars and single-column observations (e.g. tight connection between surface RH and LCL, evolution of cloud and PBL statistics.)

Challenges and Future Directions 1.Parameterization of PBL heterogeneity - PDF of T/q and horizontal power spectrum of w (roles of precipitation-driven downdrafts, surface properties, upscale cascade). -Do mesoscale wakes from stratiform precipitation require special treatment or is it better to consider them a resolved-scale process? -Better downdraft parameterizations required? Stochasticity? 2.Is the coupling of lateral Cu entrainment spectrum to PBL eddy scale and the size spectrum of clouds at cloud base as tight as some recent idealized CRM simulations suggest (or is subgrid free tropospheric heterogeneity in q,T also important)? 3.Improved and more widely used parameterizations of convective momentum transport to improve predictions of surface wind stress/fluxes.

Resolution/technical issues 1.What to do re PBL/shallow cumulus parameterization when model resolution falls to 2-5 km in NWP applications? 2.What is adequate vertical resolution of PBL/transition layer for fluxes, Cu mass-flux and initial parcel properties for deep Cu params that use boundary/transition layer closure? ( m?) How do we balance the refinement of horizontal vs. vertical resolution for deep convective PBL? 3.Separation of and handoff between shallow and deep Cu params –best solved by unification of Cu scheme.

Speculative topics 1.Do we need extra subgrid ‘memory’ in PBL scheme (e.g. prognostic TKE or eddy scale info) to maintain long-lived and redeveloping convective systems? Could interaction between horizontal grid boxes help represent this problem? Cellular automata as a tool 2.Need for temporal memory in Cu convection to help with Cu lifecycle (e.g. diurnal cycle of land convection)?