Modeling Stratocumulus Clouds: From Cloud Droplet to the Meso-scales Stephan de Roode Clouds, Climate & Air Quality Multi-Scale Physics (MSP), Faculty.

Slides:



Advertisements
Similar presentations
Introduction Irina Surface layer and surface fluxes Anton
Advertisements

What’s quasi-equilibrium all about?
Clouds and radiation in a LSM L=50km. Veldhoven, Stratocumulus cloud albedo: example cloud layer depth = 400 m effective cloud droplet.
BBOS meeting on Boundary Layers and Turbulence, 7 November 2008 De Roode, S. R. and A. Los, QJRMS, Corresponding paper available from
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.
Evaluation of HARMONIE using a single column model in the KNMI
The Problem of Parameterization in Numerical Models METEO 6030 Xuanli Li University of Utah Department of Meteorology Spring 2005.
Hurricanes Innovative Grid-Enable Multiple-scale Hurricane modeling system Konstantinos Menelaou International Hurricane Research Center Department of.
The Atmospheric Boundary Layer (ABL) over Mesoscale Surface Heterogeneity 25 June 2009 Song-Lak Kang Research Review.
Low clouds in the atmosphere: Never a dull moment Stephan de Roode (GRS) stratocumulus cumulus.
Buoyancy driven turbulence in the atmosphere
Lecture 7-8: Energy balance and temperature (Ch 3) the diurnal cycle in net radiation, temperature and stratification the friction layer local microclimates.
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.
Modeling Clouds and Climate: A computational challenge Stephan de Roode Clouds, Climate & Air Quality Multi-Scale Physics (MSP), Faculty of Applied Sciences.
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.
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.
7 oktober 2009 Challenge the future Delft University of Technology Clouds and Climate KNMI Climate Course 2011 A. Pier Siebesma KNMI & TU Delft Multiscale.
Multi-Scale Physics Faculty of Applied Sciences The formation of mesoscale fluctuations by boundary layer convection Harm Jonker.
The representation of stratocumulus with eddy diffusivity closure models Stephan de Roode KNMI.
Atmospheric TU Delft Stephan de Roode, Harm Jonker clouds, climate and weather air quality in the urban environmentenergy.
Clouds, Aerosols and Precipitation GRP Meeting August 2011 Susan C van den Heever Department of Atmospheric Science Colorado State University Fort Collins,
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 Feedback: Its Role in Climate Formation and Climate Change Igor N. Esau.
Cloud Feedbacks on Climate: A Challenging Scientific Problem Joel Norris Scripps Institution of Oceanography Fermilab Colloquium May 12, 2010.
Stephan de Roode (KNMI) Entrainment in stratocumulus clouds.
Update on model developments: Meteo-France NWP model / clouds and turbulence CLOUDNET workshop / Paris 27-28/05/2002 Jean-Marcel Piriou Centre National.
1 Indirect evidence of vertical humidity transport during very stable conditions at Cabauw Stephan de Roode
Budgets of second order moments for cloudy boundary layers 1 Systematische Untersuchung höherer statistischer Momente und ihrer Bilanzen 1 LES der atmosphärischen.
Xin Xi Feb. 28. Basics  Convective entrainment : The buoyant thermals from the surface layer rise through the mixed layer, and penetrate (with enough.
The ASTEX Lagrangian model intercomparison case Stephan de Roode and Johan van der Dussen TU Delft, Netherlands.
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
The formation of mesoscale fluctuations by boundary layer convection
Evaluating forecasts of the evolution of the cloudy boundary layer using radar and lidar observations Andrew Barrett, Robin Hogan and Ewan O’Connor Submitted.
Atmospheric dry and shallow moist convection
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.
Toulouse IHOP meeting 15 June 2004 Water vapour variability within the growing convective boundary layer of 14 June 2002 with large eddy simulations and.
Large Eddy Simulation of Low Cloud Feedback to a 2-K SST Increase Anning Cheng 1, and Kuan-Man Xu 2 1. AS&M, Inc., 2. NASA Langley Research Center, Hampton,
April Hansen et al. [1997] proposed that absorbing aerosol may reduce cloudiness by modifying the heating rate profiles of the atmosphere. Absorbing.
Boundary Layer Clouds.
1 Large Eddy Simulation of Stable Boundary Layers with a prognostic subgrid TKE equation 8 th Annual Meeting of the EMS, Amsterdam, 2008 Stephan R. de.
Simulating Stratocumulus clouds sensitivity to representation of: Drizzle Cloud top entrainment Cloud-Radiation interaction Large scale subsidence Vertical.
Modeling and Evaluation of Antarctic Boundary Layer
MM5 studies at Wageningen University (NL) Title Jordi Vilà (Group 4) NL North sea Radar MM5 NL North sea.
LES modeling of precipitation in Boundary Layer Clouds and parameterisation for General Circulation Model O. Geoffroy J.L. Brenguier CNRM/GMEI/MNPCA.
A Thermal Plume Model for the Boundary Layer Convection: Representation of Cumulus Clouds C. RIO, F. HOURDIN Laboratoire de Météorologie Dynamique, CNRS,
Federal Department of Home Affairs FDHA Federal Office of Meteorology and Climatology MeteoSwiss Component testing of the COSMO model’s turbulent diffusion.
Stratocumulus-topped Boundary Layer
Stephan de Roode The art of modeling stratocumulus clouds.
A Case Study of Decoupling in Stratocumulus Xue Zheng MPO, RSMAS 03/26/2008.
PAPERSPECIFICS OF STUDYFINDINGS Kohler, 1936 (“The nucleus in and the growth of hygroscopic droplets”) Evaporate 2kg of hoar-frost and determined Cl content;
THE INFLUENCE OF WIND SPEED ON SHALLOW CUMULUS CONVECTION from LES and bulk theory Louise Nuijens and Bjorn Stevens University of California, Los Angeles.
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.
Large Eddy Simulations of Entrainment and Inversion Structure Alison Fowler (MRes Physics of Earth and Atmosphere) Supervisor: Ian Brooks Entrainment Zone.
Pier Siebesma Today: “Dry” Atmospheric Convection
Investigating Cloud Inhomogeneity using CRM simulations.
Seamless turbulence parametrization across model resolutions
Multiscale aspects of cloud-resolving simulations over complex terrain
Entrainment rates in stratocumulus computed from a 1D TKE model
NRL POST Stratocumulus Cloud Modeling Efforts
Colombe Siegenthaler - Le Drian
Kurowski, M .J., K. Suselj, W. W. Grabowski, and J. Teixeira, 2018
Presentation transcript:

Modeling Stratocumulus Clouds: From Cloud Droplet to the Meso-scales Stephan de Roode Clouds, Climate & Air Quality Multi-Scale Physics (MSP), Faculty of Applied Sciences, TU Delft

Clouds, Climate and Air Quality atmospheric boundary layer in the laboratory N2ON2OCH 4 new methods for measuring emission rates cloud-climate feedback detailed numerical simulation

Landsat satellite ~65 km Large Eddy Simulation ~10 km ~mm viscous dissipation ~1 km shallow cumulus ~1  m-100  m Cloud droplets Earth ~13000 km slide by Harm Jonker

Contents (1) Eddy diffusivity profiles in stratocumulus Does its shape matter? When is a turbulent flux countergradient? (2) Grid resolution in weather forecast models Are parameterizations independent of the grid size? (3) Stratocumulus equilibrium states How will global warming affect cloud amount? (4) “Cloud droplets” on the ground: dew formation Can we measure it? (5) Summary and outlook Stratocumulus equilibrium states, an interesting study case for WRF?

GEWEX Cloud Systems Study (GCSS) Stratocumulus Intercomparison Cases Stratocumulus case based on observations (FIRE I) Use observations to prescribe - initial state - large-scale horizontal advection - large-scale subsidence rate Simulation of diurnal cycle - 1D versions of General Circulation Models - Large-Eddy Simulation Models (LES)

GEWEX Cloud Systems Study (GCSS) Stratocumulus Intercomparison Cases Stratocumulus case based on observations (FIRE I) Use observations to prescribe - initial state - large-scale horizontal advection - large-scale subsidence rate Simulation of diurnal cycle - 1D versions of General Circulation Models - Large-Eddy Simulation Models (LES) initial jumps for three GCSS stratocumulus cases

3D results from Large-Eddy Simulation results - The cloud liquid water path

1D results from General Circulation Models - The cloud liquid water path (LWP) Single Column Model liquid water path results very sensitive to entrainment rate drizzle parameterization convection scheme (erroneous triggering of cumulus clouds) Duynkerke, P. G., S. R. de Roode, M. C. van Zanten, J. Calvo, J. Cuxart, S. Cheinet, A. Chlond, H. Grenier, P. J. Jonker, M. Koehler, G. Lenderink, D. Lewellen, C.-L. Lappen, A. P. Lock, C.-H. Moeng, F. Mller, D. Olmeda, J.-M. Piriou, E. Sanchez, I. Sednev, 2004: Observations and numerical simulations of the diurnal cycle of the EUROCS stratocumulus case. Quart. J. R. Met. Soc., 130,

Entrainment - mixing of relatively warm and dry air from above the inversion into the cloud layer - important for cloud evolution

Entrainment parameterizations - Implementation in K-diffusion schemes Turbulent flux at the top of the boundary layer due to entrainment with rate w e : ("flux-jump" relation) Top-flux with K-diffusion:

Diagnose eddy- diffusivity coefficients from LES results

K-coefficients from FIRE I LES

Importance of eddy-diffusivity coefficients on internal boundary- layer structure Vary magnitude K profile Compute solutions  l and q t for given surface and entrainment fluxes

Total water content profiles for different K-profiles but identical vertical fluxes For weakly unstable conditions above sea : small values for the eddy diffusivity if it depends on the convective velocity scale w *

Liquid water content profiles for different K-profiles Magnitude K-coefficient in interior BL important for liquid water content! K factorLWP [g/m 2 ]  109 De Roode, S. R., 2007: The role of eddy diffusivity profiles on stratocumulus liquid water path biases. Monthly Weather Rev., 135,

Contents (1) Eddy diffusivity profiles in stratocumulus Does its shape matter? When is a turbulent flux countergradient? (2) Grid resolution in weather forecast models Are parameterizations independent of the grid size? (3) Stratocumulus equilibrium states How will global warming affect cloud amount? (4) “Cloud droplets” on the ground: dew formation Can we measure it? (5) Summary and outlook Stratocumulus equilibrium states, an interesting study case for WRF?

Countergradient fluxes: Clear Convective Boundary Layer (CBL)

Flux profiles in the Clear Convective Boundary Layer virtual potential temperature (buoyancy) potential temperature (temperature) moisture

Countergradient fluxes in the CBL temperature buoyancy moisture No countergradient flux if vertical flux does not change sign in the mixed layer De Roode, S. R., et al., 2004: Countergradient fluxes of conserved variables in the clear convective and stratocumulus-topped boundary layer. The role of the entrainment flux., Bound.-Lay. Meteor, 112,

Contents (1) Eddy diffusivity profiles in stratocumulus Does its shape matter? When is a turbulent flux countergradient? (2) Grid resolution in weather forecast models Are parameterizations independent of the grid size? (3) Stratocumulus equilibrium states How will global warming affect cloud amount? (4) “Cloud droplets” on the ground: dew formation Can we measure it? (5) Summary and outlook Stratocumulus equilibrium states, an interesting study case for WRF?

Cloud dynamics 10 m100 m1 km10 km100 km1000 km10000 km turbulence  Cumulus clouds Cumulonimbus clouds Mesoscale Convective systems Extratropical Cyclones Planetary waves Large Eddy Simulation (LES) Model Cloud System Resolving Model (CSRM) Numerical Weather Prediction (NWP) Model Global Climate Model The Zoo of Atmospheric Models DNS mm Cloud microphysics

Countergradient fluxes in the CBL Dx = 25.6 km Dy = 25.6 km t=8h

Countergradient fluxes: destruction of variance prohibiting growth of length scales temperature buoyancy moisture De Roode, S. R., P. G. Duynkerke and H. J. J. Jonker, 2004: Large Eddy Simulation: How large is large enough? J. Atmos. Sci., 61,

Stratocumulus cloud albedo: example cloud layer depth = 400 m effective cloud droplet radius= 10  m optical depth  = 25 homogeneous stratocumulus cloud layer

Real clouds are inhomogeneous Stratocumulus albedo from satellite

Albedo for an inhomgeneous cloud layer 27 Redistribute liquid water: optical depths  = 5 and 45 inhomogeneous stratocumulus cloud layer mean albedo = 0.65 < 0.79

Cloud albedo in a weather forecast or climate model Decrease optical thickness: Cahalan et al (1994):  = 0.7 (FIRE I observations)  effective  mean inhomogeneous albedo homogeneous albedo

Analytical results for the inhomogeneity factor  Assumption: Gaussian optical depth distribution

Value of correction factor depends on grid size De Roode, S. R., and A. Los, 2008: The effect of temperature and humidity fluctuations on the liquid water path of non-precipitating closed cell stratocumulus clouds. Quart. J. Roy. Meteor. Soc., 134,

Contents (1) Eddy diffusivity profiles in stratocumulus Does its shape matter? When is a turbulent flux countergradient? (2) Grid resolution in weather forecast models Are parameterizations independent of the grid size? (3) Stratocumulus equilibrium states How will global warming affect cloud amount? (4) “Cloud droplets” on the ground: dew formation Can we measure it? (5) Summary and outlook Stratocumulus equilibrium states, an interesting study case for WRF?

Feedback effects in a changing climate Dufresne & Bony, Journal of Climate 2008 Radiative effects only Water vapor feedback Surface albedo feedback Cloud feedback

The playground for cloud physicists: Hadley circulation deep convectionshallow cumulusstratocumulus

EU Cloud Intercomparison, Process Study and Evaluation Project (EUCLIPSE) Future Sea water temperature: T+  T  enhanced surface evaporation Present Sea water temperature: T Positive Feedback? Entrainment drying dominates moisture tendency Negative Feedback?

CGILS: CFMIP-GCSS Intercomparison of Large-Eddy and Single-Column Models

CGILS – Simulation details Simulation time 10 days adaptive time step, dtmax = 10 secs radiation time step = 60 secs Domain size 4.8 x 4.8 x 4 km 3, 96 x 96 x 128 grid points (  z = 25 m in lower part) Total CPU hours on 32 processors 2700 hours

CGILS Hourly-averaged vertical mean profiles during the last 5 hours

CGILS Cloud liquid water path (LWP)

Top Of Atmosphere Net Radiative Fluxes

Contents (1) Eddy diffusivity profiles in stratocumulus Does its shape matter? When is a turbulent flux countergradient? (2) Grid resolution in weather forecast models Are parameterizations independent of the grid size? (3) Stratocumulus equilibrium states How will global warming affect cloud amount? (4) “Cloud droplets” on the ground: dew formation Can we measure it? (5) Summary and outlook Stratocumulus equilibrium states, an interesting study case for WRF?

Dew formation at Cabauw

Mean surface energy balance at Cabauw during the night De Roode, S. R., F. C. Bosveld and P. S. Kroon, 2010: Dew formation, eddy-correlation latent heat fluxes, and the surface energy imbalance at Cabauw during stable conditions. In press, Bound.-Layer Meteorology.

Summary and outlook Equilibrium states  Good approach to investigate model representation of stratocumulus NWP future  Scale dependency of paramaterizations (variances, mass flux approach) Stable boundary layers and dew formation  Dew formation can occus for very stable conditions (Ri B >1)  Difficult to measure References CGILS case Papers can be downloaded from -> publicationswww.srderoode.nl/