The Response of Marine Boundary Layer Clouds to Climate Change in a Hierarchy of Models Chris Jones Department of Applied Math Advisor: Chris Bretherton.

Slides:



Advertisements
Similar presentations
Met Office Hadley Centre, FitzRoy Road, Exeter, Devon, EX1 3PB United Kingdom Tel: +44 (0) Fax: +44 (0)
Advertisements

© Crown copyright 2006Page 1 CFMIP II sensitivity experiments Mark Webb (Met Office Hadley Centre) Johannes Quaas (MPI) Tomoo Ogura (NIES) With thanks.
© Crown copyright Met Office Towards understanding the mechanisms responsible for different cloud-climate responses in GCMs. Mark Webb, Adrian Lock (Met.
Veldhoven, Large-eddy simulation of stratocumulus – cloud albedo and cloud inhomogeneity Stephan de Roode (1,2) & Alexander Los (2)
Impacts of Large-scale Controls and Internal Processes on Low Clouds
(Mt/Ag/EnSc/EnSt 404/504 - Global Change) Climate Models (from IPCC WG-I, Chapter 8) Climate Models Primary Source: IPCC WG-I Chapter 8 - Climate Models.
The Problem of Parameterization in Numerical Models METEO 6030 Xuanli Li University of Utah Department of Meteorology Spring 2005.
Semi-direct effect of biomass burning on cloud and rainfall over Amazon Yan Zhang, Hongbin Yu, Rong Fu & Robert E. Dickinson School of Earth & Atmospheric.
Low clouds in the atmosphere: Never a dull moment Stephan de Roode (GRS) stratocumulus cumulus.
Aggregated Convection and the Regulation of Tropical Climate Kerry Emanuel Program in Atmospheres, Oceans, and Climate MIT.
Clouds and Climate: Cloud Response to Climate Change SOEEI3410 Ken Carslaw Lecture 5 of a series of 5 on clouds and climate Properties and distribution.
Climate Forcing and Physical Climate Responses Theory of Climate Climate Change (continued)
Earth Systems Science Chapter 6 I. Modeling the Atmosphere-Ocean System 1.Statistical vs physical models; analytical vs numerical models; equilibrium vs.
Clouds and Climate: Cloud Response to Climate Change ENVI3410 : Lecture 11 Ken Carslaw Lecture 5 of a series of 5 on clouds and climate Properties and.
The Centre for Australian Weather and Climate Research A partnership between CSIRO and the Bureau of Meteorology The Effect of Turbulence on Cloud Microstructure,
IACETH Institute for Atmospheric and Climate Science Boundary Layer parametrisation in the climate model ECHAM5-HAM Colombe Siegenthaler - Le Drian, Peter.
Subtropical low cloud feedback in a superparameterized GCM - a mechanism and a CRM column analogue Peter N. Blossey Matthew C. Wyant Christopher S. Bretherton.
Evening Discussion: Toward a better understanding of PBL cloud feedbacks on climate sensitivity Some introductory material Chris Bretherton University.
Relationships between wind speed, humidity and precipitating shallow cumulus convection Louise Nuijens and Bjorn Stevens* UCLA - Department of Atmospheric.
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.
Clouds and climate change
Towards stability metrics for cloud cover variation under climate change Rob Wood, Chris Bretherton, Matt Wyant, Peter Blossey University of Washington.
Warm rain variability and its association with cloud mesoscale structure and cloudiness transitions Robert Wood, University of Washington with help and.
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.
Mesoscale Modeling Review the tutorial at: –In class.
The representation of stratocumulus with eddy diffusivity closure models Stephan de Roode KNMI.
© Crown copyright Met Office CFMIP-2 techniques for understanding cloud feedbacks in climate models. Mark Webb (Met Office Hadley Centre) CFMIP/GCSS BLWG.
1.Introduction 2.Description of model 3.Experimental design 4.Ocean ciruculation on an aquaplanet represented in the model depth latitude depth latitude.
Radiative Properties of Eastern Pacific Stratocumulus Clouds Zack Pecenak Evan Greer Changfu Li.
Radiation Group 3: Manabe and Wetherald (1975) and Trenberth and Fasullo (2009) – What is the energy balance of the climate system? How is it altered by.
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.
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.
EPIC 2001 SE Pacific Stratocumulus Cruise 9-24 October 2001 Rob Wood, Chris Bretherton and Sandra Yuter (University of Washington) Chris Fairall, Taneil.
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.
Large Eddy Simulation of PBL turbulence and clouds Chin-Hoh Moeng National Center for Atmospheric Research.
Synthesis NOAA Webinar Chris Fairall Yuqing Wang Simon de Szoeke X.P. Xie "Evaluation and Improvement of Climate GCM Air-Sea Interaction Physics: An EPIC/VOCALS.
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
Simple tropical models and their relationship to GCMs Adam Sobel, Columbia Chris Bretherton, U. Washington.
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.
Goal: Isolate SP-CAM low cloud response in a simpler setting and examine its resolution sensitivity. Key assumptions: (like Zhang & Bretherton 2008, Caldwell.
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.
1. Introduction Boundary-layer clouds are parameterized in general circulation model (GCM), but simulated in Multi-scale Modeling Framework (MMF) and.
Boundary Layer Clouds.
Workshop on Tropical Biases, 28 May 2003 CCSM CAM2 Tropical Simulation James J. Hack National Center for Atmospheric Research Boulder, Colorado USA Collaborators:
Robert Wood, Atmospheric Sciences, University of Washington The importance of precipitation in marine boundary layer cloud.
Coupled vs. Decoupled Boundary Layers in VOCALS-REx Chris Jones and Chris Bretherton Department of Atmospheric Sciences University of Washington Dave Leon.
Cloud-climate feedbacks: what we think we know and why we think we know it David Mansbach 14 April 2006 T 1
Lazaros Oreopoulos (NASA-GSFC)
Development and testing of the moist second-order turbulence-convection model including transport equations for the scalar variances Ekaterina Machulskaya.
Using WRF-Chem to understand interactions between synoptic and microphysical variability during VOCALS Rhea George, Robert Wood University of Washington.
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;
Mesoscale variability and drizzle in stratocumulus Kim Comstock General Exam 13 June 2003.
THE INFLUENCE OF WIND SPEED ON SHALLOW CUMULUS CONVECTION from LES and bulk theory Louise Nuijens and Bjorn Stevens University of California, Los Angeles.
Important data of cloud properties for assessing the response of GCM clouds in climate change simulations Yoko Tsushima JAMSTEC/Frontier Research Center.
Clouds and Large Model Grid Boxes
Multiscale aspects of cloud-resolving simulations over complex terrain
Cloudsat and Drizzle: What can we learn
Short Term forecasts along the GCSS Pacific Cross-section: Evaluating new Parameterizations in the Community Atmospheric Model Cécile Hannay, Dave Williamson,
VOCALS Open Ocean: Science and Logistics
Cloud-topped boundary layer response time scales in MLM and LES
Cloudsat and Drizzle: What can we learn
Cloudsat and Drizzle: What can we learn
Presentation transcript:

The Response of Marine Boundary Layer Clouds to Climate Change in a Hierarchy of Models Chris Jones Department of Applied Math Advisor: Chris Bretherton Departments of Applied Math and Atmospheric Sciences VOCALS RF05, 72W, 20S

Overview Introduction: Marine boundary layer (MBL) clouds and climate sensitivity Idealized local case studies in a hierarchy of models The well-mixed MBL from observations Comparison of model responses to changes in CO 2 and temperature Summary of proposed future work

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation (NASA) Marine boundary layer clouds especially important because… 1.They’re reflective at visible wavelengths MBL clouds

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation (images courtesy of Chris Bretherton) Marine boundary layer clouds especially important because… 1.They’re reflective at visible wavelengths 2.They cover a lot of area Cloud Fraction Cloud forcing = R(clear sky) – R(all sky) Global net cloud radiative forcing ~ -20 W m -2 (Loeb et al, 2009) Compared to CO 2 ~ 2 W m -2

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation Marine boundary layer clouds especially important because 1.They’re shiny (reflect incoming solar radiation) 2.They cover a lot of area 3.They’re hard to realistically represent in global climate models Interplay between dynamics and physics Nonlinear Turbulent Physics must be parameterized

Climate Change: Response to radiative forcing R = Absorbed Solar Radiation – Outgoing Longwave Radiation Cloud contribution most uncertain (next slide)

Cloud feedbacks dominate climate sensitivity uncertainty in GCMs Clouds dominate overall climate feedback uncertainty Clouds: - Positive feedback, - Large spread between models Bony et al. (2006)

Cloud feedbacks dominate climate sensitivity uncertainty in GCMs Clouds dominate overall climate feedback uncertainty Clouds: - Positive feedback, - Large spread between models Bony et al. (2006)

Cloud feedbacks dominate climate sensitivity uncertainty in GCMs Clouds dominate overall climate feedback uncertainty Low clouds dominate cloud feedback uncertainty Soden and Vecchi (2011) Clouds: - Positive feedback, - Large spread between models Bony et al. (2006)

Parameterizations of Physical Processes Make Profound Impact 3.2K climate sensitivity 4.0 K climate sensitivity (Gettelman et al., 2011) UW turbulence and shallow convection parameterizations largely responsible for increase in climate sensitivity from CAM4 to CAM5 – can our analysis help explain this? Equilibrium response to 2xCO 2

Objectives of This Research Use a localized, idealized column-oriented analysis of prototypical MBL cloud regimes to identify and evaluate MBL cloud-climate radiative response mechanisms Hierarchy of models: – Large eddy simulation (LES): high resolution cloud resolving model – closest we have to “observations” in local climate change simulations – Single-column model (SCM): ties results to GCM – Mixed-layer model (MLM): simplified model for interpretive purposes Seek to relate SCM back to parent GCM Scientific Relevance: Understanding mechanisms of change in GCMs is pre-requisite for constraining through observation and/or improving parameterizations. Mathematical Relevance: Investigate impacts of various parts of model formulation (e.g., subgrid parameterizations, model resolution, applied large-scale forcings); to what extent can models be used to interpret the behavior of other models?

Case studies drawn from CGILS Intercomparison S12: Shallow Stratocumulus (Sc) Well-mixed BL S11: Transition between Sc and shallow cumulus (Cu) Onset of BL decoupling Cu rising into Sc S6: Shallow Cu Zhang et al (2010)

Hierarchy of models GCM (CAM5) SCM (SCAM5) LES (SAM) Image courtesy of NOAA (S6, courtesy of Peter Blossey) SCAM5 Vertical Resolution MLM

Large-scale advection Subsidence Tendencies due to physical processes, e.g., Precipitation Radiation and clouds Microphysics Turbulence Dynamics

(Stevens, 2007) Mixed-layer model equations

Advective cooling/drying Entrainment surface fluxes Radiation Precipitation (Stevens, 2007)

October November 2008 ( How reasonable is the well-mixed assumption? Previous project studied the extent of well-mixed vs. decoupled boundary layers using aircraft data from VOCALS field experiment Classified flight legs as well- mixed or decoupled based on gradient of moisture and temperature quantities

Subcloud layer Cloud layer Well-mixed Decoupled Jones et al. (2011)

Case setup and proposed sensitivity studies Simulation setup Diurnally averaged summertime insolation Models run to steady-state Large-scale forcings specified from observations: – Horizontal divergence – Subsidence – Sea surface temperature – Wind profile CGILS sensitivity studies Control (CTL) – Mimics current climate 4xCO 2 concentration (4xCO2): – Captures “fast” adjustment Uniform +2K temp. increase: – Captures temperature- mediated response – Reduced subsidence (P2K) – Subsidence as in CTL (P2K OM0)

S12 Results: Cloud Fraction LES Results from CGILS intercomparison MLM Results

Preliminary S12 Results: Profiles SAM LES: Liquid static energyMoistureCloud liquid MLM:

SAM LES: Liquid static energyMoistureCloud liquid MLM: SCAM5: (L80)

All models exhibit similar steady-state mean sensitivities: 4xCO 2 has lower inversion, thinner cloud (positive cloud feedback) P2K deepens and thickens relative to control (negative cloud feedback) P2K OM0 thinner than P2K and slightly thinner than CTL (positive cloud feedback) Subsidence (large scale dynamics) plays dominant role in P2K response Preliminary S12 Results: Summary SAM (LES) SCAM5 (SCM) MLM SAM (LES) SCAM5 (SCM) MLM xCO 2 P2K SAM (LES) SCAM5 (SCM) MLM-4 +8 P2K OM0

MLM 4xCO 2 Sensitivity Mechanism: Increased down-welling LW radiation  decreased cloud top radiative cooling (~10% decrease)  Less turbulence (i.e., less entrainment)  Lower z i  Cloud thickness decreases CTL 4xCO2 CTL 4xCO2

SCAM5 S12 Resolution Sensitivity Default CAM5 Resolution doesn’t sustain a cloud Higher resolution does Cloud fraction

Future Work – Apply MLM to interpreting other LESs involved in CGILS case study – Fully investigate SCAM5 S12 behavior What’s driving the resolution sensitivity? – Expand analysis to other locations (MLM may not apply) – Parameter-space representation with SCAM Use SST, Free troposphere lapse rate, CO 2 and/or subsidence as control parameters – Find a way to relate the local cloud response in SCAM to the sensitivity in its parent GCM

Questions? (MODIS satellite image)

Additional slides

Future Work (plenty to keep me busy) – Apply MLM to interpreting other LESs involved in CGILS case study (hypothesis: by tuning entrainment efficiency, can I reproduce their mean properties / sensitivities?) – Dig into roots of SCAM5 S12 sensitivity (interpret w/MLM when appropriate) What’s driving the resolution sensitivity? – Expand analysis to other locations (MLM may not apply) – Parameter-space representation with SCAM, following approach of Caldwell and Bretherton (2009) MLM study Use SST, Free troposphere lapse rate, CO 2 and/or subsidence as control parameters – Find a way to relate the local cloud response in SCAM to the sensitivity in its parent GCM

Additional Slides CRF, adjusted CRF, etc.

SCAM5 Default Resolution vs. VOCALS radar strip

SAM LES Equations Khairoutdinov and Randall (2003) Prognostic TKE SGS model Diagnostic cloud water, cloud ice, rain, and snow Periodic horizontal domain, surface fluxes from Monin-Obukhov similarity theory ISCCP cloud simulator Parallel (MPI)

The proposal (remember the proposal? This is a presentation about the proposal …) Use MLM to interpret output from other LESs (can “tune” parameterizations and entrainment closure as needed) Investigate sensitivities in each model for each location Map out primitive parameter-space representation using SCM (like CB09) Ultimately, most concerned with SCAM, b/c it connects directly to GCM – to what extent can we use this analysis to shed light on the low cloud- climate mechanisms in CAM5?

Large-scale advection Subsidence Tendencies due to physical processes, e.g., Precipitation Radiation and clouds Microphysics Surface fluxes Turbulence

Primitive equations LES: SCAM:

Mixed-layer model equations

Mixed-layer model equations: Advection (cooling,drying) Entrainment warming/drying Latent heat flux Precipitation Radiative cooling Sensible heat flux subsidence

EPIC 2001 (Bretherton, et al.) Contributing Mechanisms for MBL Balance Subsidence Advection

Mixed-layer model: Advection (cooling,drying) Entrainment warming/drying Latent heat flux Precipitation Radiative cooling Sensible heat flux subsidence

Sc (top) vs. Cu (bottom) MBL structure (Stevens et al 2007; Stevens 2006)

MLM time series for S12

Relevant previous column modeling studies Caldwell and Bretherton Zhang and Bretherton …

Model run specifics Grid resolution – CESM 1.0 (CAM5): 1 deg = 0.9 deg x 1.25 deg x 30 levels – (i.e., ~100 km x 137 km x … [variable]) Time steps (?) Length of integration Numerics / miscellaneous

Outline Introduction – Climate sensitivity, feedbacks, and cloud radiative forcing – Why are low clouds important (to climate system, climate sensitivity)? – What has been done, and where does this study fit in? – Feedback flow chart (?) Proposal for this study: Localized case studies using a hierarchy of models – CGILS cases – Primitive equations – An assortment of models GCM (global models, under-resolved,…) SCM (single column of the GCM) LES (high-resolution column model – resolve largest, most energetic eddies, models subgrid) MLM (idealized reduced order model that uses – Decoupling work pepper VOCALS throughout MLM comparison with LES for S12 (and maybe SCAM?) Proposed dissertation topic

Outline Introduction – What is climate sensitivity and why do we care? – Why are low clouds important (to climate system, climate sensitivity)? – What has been done, and where does this study fit in? – Feedback flow chart (?) Proposal for this study – CGILS cases – Primitive equations – An assortment of models GCM (global models, under-resolved,…) SCM (single column of the GCM) LES (high-resolution column model – resolve largest, most energetic eddies, models subgrid) MLM (idealized reduced order model that uses – Decoupling work pepper VOCALS throughout MLM comparison with LES for S12 (and maybe SCAM?) Proposed dissertation topic

Our approach: Consensus that we need better understanding of the processes underlying low-cloud response to climate change (i.e., GCM intercomparison studies demonstrate clearly the global average low cloud response is a big uncertainty, but individual models differ in parameterizations of cloud processes, and climate-change output diverges widely between models) Use IDEALIZED LOCAL CASE STUDIES (drawn from CGILS intercomparison) to investigate cloud sensitivity in a hierarchy of models (LES, SCM, and MLM) to climate-change inspired tests, with the goals of: – Understanding mechanisms behind cloud sensitivity (i.e., do LES and SCM agree? Can this behavior be constrained by observations? Is improved parameterization, informed by LES necessary?) – Connecting these back to the GCM behavior of a given model.

Proposal: use a hierarchy of models to investigate low cloud response to climate perturbations Local analysis: – Focus on 3 regions used in CGILS intercomparison study representing 3 low cloud regimes with idealized large scale forcings – Use 3 types of column models to investigate cloud sensitivity to a variety of perturbations: Ultimate goal: Connect these back to GCM

Subcloud legs drizzle Profiles Surface layer Cloud layer Well-mixed Decoupled

C-130 flight path (grey) Cloud base (lidar-derived) LCL (“well-mixed cloud base”) Radar reflectivity (drizzle proxy) (courtesy of Rob Wood) We use vertical profiles and subcloud level legs

Inversion Jumps Inversion base Inversion “top”

Use REx C-130 profiles to calculate jumps/decoupling, adjacent subcloud legs to calculate cloud fraction. Restrict to flights before 10:00 LT in left panel. κ > 0.4 often (but not always) goes with broken cloud. For κ < 0.5 there is no obvious correlation of κ and decoupling. POC and non-POC distributions overlap Blue = well-mixed Red = decoupled Hollow = POC Dash = Lock (2009) LES results

Shiny clouds MODIS Visible Image

Marine Boundary Layer (MBL) clouds:

CGILS Cases (focus on S12 this talk) S12: Shallow Stratocumulus (Sc) Well-mixed BL => mixed-layer model appropriate Focus of remainder of this talk S11: Transition between Sc and shallow cumulus (Cu) Onset of BL decoupling Cu rising into Sc S6: Shallow Cu

Mixed-layer model equations horizontal advection Entrainment surface fluxes Radiation Precipitation

Marine Boundary Layer (MBL) Clouds (Infrared satellite image, courtesy of Rob Wood)

Marine Boundary Layer (MBL) Clouds NASA MODIS Satellite Image

Questions?

Marine boundary layer clouds: 1.Reflect incoming solar radiation 2.Cover a large fraction of the surface

MODIS visible satellite image Reflective

Clouds in climate models - change in low cloud amount for 2  CO 2 from Stephens (2005) GFDL CCM model number

Subcloud layer Cloud layer Well-mixed Decoupled Approximately 30% of profiles in VOCALS-REx were well-mixed (blue)

Climate Change: Response to radiative forcing R = Absorbed Solar Radiation – Outgoing Longwave Radiation Radiative forcing (e.g., increased CO 2 ) Cloud contribution most uncertain

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation (Infrared satellite image, courtesy of Rob Wood) Marine boundary layer clouds especially important because… 1.They’re reflective at visible wavelengths 2.They cover a lot of area

Climate Change: Response to radiative forcing R = Absorbed Solar Radiation – Outgoing Longwave Radiation Radiative forcing (e.g., increased CO 2 )

Cloud feedbacks dominate climate sensitivity uncertainty in GCMs Clouds dominate overall climate feedback uncertainty Low clouds dominate cloud feedback uncertainty Clouds: - Positive feedback, - Large spread between models Bony et al. (2006)Soden and Vecchi (2011)

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation (NASA) Marine boundary layer clouds especially important because... MBL clouds

IPCC (2007)

The Models LES (high resolution): System for Atmospheric Model (SAM) – High resolution cloud resolving model – Largest, most energetic eddies resolved – Subgrid-scale turbulence is modeled – The closest we have to “observations” for climate change simulations – Parallel effort by Peter Blossey and Chris Bretherton for CGILS LES intercomparision SCM (single column of global model): SCAM5 (CAM5 GCM, operating in single column mode) – Single grid column from the GCM – Approximately 1 degree horizontal resolution, 30 vertical levels – Parameterize subgrid physical processes MLM (idealized, interpretive model): – Idealized reduced order model applicable in Sc region (S12) when MBL remains “well-mixed” – When applicable, good for diagnosing / interpreting sensitivities in other models

Earth’s Radiation Budget: R = Absorbed Solar Radiation – Outgoing Longwave Radiation (NASA MODIS visible satellite image in Eastern Pacific) Marine boundary layer clouds especially important because… 1.They’re reflective at visible wavelengths