Evaluation of CMIP5 Simulated Clouds and TOA Radiation Budgets in the SMLs Using NASA Satellite Observations

Similar documents
Supplement of Insignificant effect of climate change on winter haze pollution in Beijing

S16. ASSESSING THE CONTRIBUTIONS OF EAST AFRICAN AND WEST PACIFIC WARMING TO THE 2014 BOREAL SPRING EAST AFRICAN DROUGHT

Supplementary Information for Impacts of a warming marginal sea on torrential rainfall organized under the Asian summer monsoon

Supplemental Material for

Desert Amplification in a Warming Climate

Decadal shifts of East Asian summer monsoon in a climate. model free of explicit GHGs and aerosols

Supplemental material

Future freshwater stress for island populations

Twenty-first-century projections of North Atlantic tropical storms from CMIP5 models

Supplementary Figure 1 A figure of changing surface air temperature and top-1m soil moisture: (A) Annual mean surface air temperature, and (B) top

Supporting Information for Relation of the double-itcz bias to the atmospheric energy budget in climate models

SUPPLEMENTARY INFORMATION

INVESTIGATING THE SIMULATIONS OF HYDROLOGICAL and ENERGY CYCLES OF IPCC GCMS OVER THE CONGO AND UPPER BLUE NILE BASINS

Geophysical Research Letters. Supporting Information for. Ozone-induced climate change propped up by the Southern Hemisphere oceanic front

Snow occurrence changes over the central and eastern United States under future. warming scenarios

Global Warming Attenuates the. Tropical Atlantic-Pacific Teleconnection

Forcing of anthropogenic aerosols on temperature trends of the subthermocline

Drylands face potential threat under 2 C global warming target

Recent Walker circulation strengthening and Pacific cooling amplified by Atlantic warming

Supporting Information for. [Strong dependence of U.S. summertime air quality on the decadal variability of Atlantic sea surface temperatures]

Understanding the regional pattern of projected future changes in extreme precipitation

Supplementary Figure 1 Observed change in wind and vertical motion. Anomalies are regime differences between periods and obtained

The final push to extreme El Ninõ

Research Article Detecting Warming Hiatus Periods in CMIP5 Climate Model Projections

Climate Impacts Projections

Climate Change Scenario, Climate Model and Future Climate Projection

Changes in the El Nino s spatial structure under global warming. Sang-Wook Yeh Hanyang University, Korea

Evaluating the Formation Mechanisms of the Equatorial Pacific SST Warming Pattern in CMIP5 Models

2 nd CCliCS Workshop, April 1 3, 2013, Taipei, Taiwan

Early benefits of mitigation in risk of regional climate extremes

Supplementary Figure S1: Uncertainty of runoff changes Assessments of. R [mm/yr/k] for each model and the ensemble mean.

Southern Hemisphere jet latitude biases in CMIP5 models linked to shortwave cloud forcing

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION

Sensitivity of climate simulations to low-level cloud feedbacks

Reconciling the Observed and Modeled Southern Hemisphere Circulation Response to Volcanic Eruptions Supplemental Material

The Implication of Ural Blocking on the East Asian Winter Climate in CMIP5 Models

Robust Arctic sea-ice influence on the frequent Eurasian cold winters in past decades

Energetic and precipitation responses in the Sahel to sea surface temperature perturbations

Differences from CERES EBAF

The Response of ENSO Events to Higher CO 2 Forcing: Role of Nonlinearity De-Zheng Sun, Jiabing Shuai, and Shao Sun

Paul W. Stackhouse, Jr., NASA Langley Research Center

Significant anthropogenic-induced changes. of climate classes since 1950

Supplementary Material for On the evaluation of climate model simulated precipitation extremes

Effects of a Warming Climate on Daily Snowfall Events in the Northern Hemisphere

Enhanced warming of the subtropical mode water in the North Pacific and North Atlantic

Getting our Heads out of the Clouds: The Role of Subsident Teleconnections in Climate Sensitivity

Projected strengthening of Amazonian dry season by constrained climate model simulations

How Will Low Clouds Respond to Global Warming?

1" 2" 3" 4" 5" 6" 7" 8" 9" 10" 11" 12" 13" 14" 15" 16" 17" 18" 19" 20" 21" 22" 23" 24" 25" 26" 27" 28" 29" 30" 31" 32" 33" 34" 35"

Supplemental Material

Maritime Continent seasonal climate biases in AMIP experiments of the CMIP5 multimodel ensemble

SEACLID/CORDEX Southeast Asia: A Regional Initiative to Provide Regional Climate Change Information and Capacity Building

Shortwave Cloud Radiative Forcing on Major Stratus Cloud Regions in AMIP-type Simulations of CMIP3 and CMIP5 Models

9.7 Climate Sensitivity and Climate Feedbacks

Interannual Variability of the Winter North Atlantic Storm Track in CMIP5 Models

Statistical downscaling of multivariate wave climate using a weather type approach

More extreme precipitation in the world s dry and wet regions

Hydrological Sensitivity in W m 2 K 1 (% K 1 ) a. BCC_csm1.1*# Beijing Climate Center, China (2.49)

On the interpretation of inter-model spread in CMIP5 climate sensitivity

Contents of this file

Beyond IPCC plots. Ben Sanderson

PUBLICATIONS. Geophysical Research Letters

Climate Feedbacks from ERBE Data

Extratropical and Polar Cloud Systems

A revival of Indian summer monsoon rainfall since 2002

SUPPLEMENTARY INFORMATION

Impacts of Climate Change on Surface Water in the Onkaparinga Catchment

Large divergence of satellite and Earth system model estimates of global terrestrial CO 2 fertilization

SUPPLEMENTARY INFORMATION

NetCDF, NCAR s climate model data, and the IPCC. Gary Strand NCAR/NESL/CGD

The ability of CMIP5 models to simulate North Atlantic extratropical cyclones

Projections of heavy rainfall over the central United States based on CMIP5 models

SST forcing of Australian rainfall trends

Karonga Climate Profile: Full Technical Version

Planetary boundary layer depth in Global climate. models induced biases in surface climatology

Contents of this file

CMIP5 Projection of Significant Reduction in Extratropical Cyclone Activity over North America

Evalua&on, applica&on and development of ESM in China

STI for Climate Extremes

what do global climate models say about increasing variance in the california current upwelling ecosystem

Satellite-derived warm rain fraction as constraint on the cloud lifetime effect

>200 LWP+IWP (g m 2 )

ENSO and annual cycle interaction: the combination mode representation in CMIP5 models

Transpose-AMIP. Steering committee: Keith Williams (chair), David Williamson, Steve Klein, Christian Jakob, Catherine Senior

The importance of ENSO phase during volcanic eruptions for detection and attribution

Update on Cordex-AustralAsia domain

Ocean carbon cycle feedbacks in the tropics from CMIP5 models

Experiments with Statistical Downscaling of Precipitation for South Florida Region: Issues & Observations

Influence of Clouds and Aerosols on the Earth s Radiation Budget Using Clouds and the Earth s Radiant Energy System (CERES) Measurements

Low-level wind, moisture, and precipitation relationships near the South Pacific Convergence Zone in CMIP3/CMIP5 models

Abstract: The question of whether clouds are the cause of surface temperature

Decreased monsoon precipitation in the Northern Hemisphere due to anthropogenic aerosols

What Controls the Mean East West Sea Surface Temperature Gradient in the Equatorial Pacific: The Role of Cloud Albedo

Gennady Menzhulin, Gleb Peterson and Natalya Shamshurina

EXPERT MEETING TO ASSESS PROGRESS MADE IN THE PROCESS TO FORMULATE AND IMPLEMENT ANATIONAL ADAPTATION PANS (NAPs)

Projection Results from the CORDEX Africa Domain

Projected change in extreme rainfall events in China by the end of the 21st century using CMIP5 models


Transcription:

Evaluation of CMIP5 Simulated Clouds and TOA Radiation Budgets in the SMLs Using NASA Satellite Observations Erica K. Dolinar Xiquan Dong and Baike Xi University of North Dakota This talk is based on Dolinar et al. (2014, Clim. Dyn.) March 18, 2014 University of Washington, Seattle, WA Workshop on Clouds, Radiation, Aerosols, and the Air-Sea Interface in the S. Midlatitude Ocean

Motivation In many climate models, details in the representation of clouds can substantially affect the model estimates of cloud feedback and climate sensitivity. Moreover, the spread of climate sensitivity estimates among current models arises primarily from inter-model differences in cloud feedbacks. Therefore, cloud feedbacks remain the largest source of uncertainty in climate sensitivity estimates. IPCC Fourth Assessment Report (2007) Want to understand the impacts of simulated clouds on the TOA radiation budget and cloud radiative forcings in our current climate so that we may better predict the future climate 1

Satellite Products Clouds CERES MODIS SYN1degree Total Column Cloud Fraction CCCM (CloudSat, CALIPSO, CERES, MODIS) Vertically integrated Cloud Fraction Vertical Velocities (omega) MERRA Reanalysis Radiation CERES EBAF TOA radiation budgets TOA cloud radiative forcing (CRF) Products are Level-3 and have been either downloaded or provided by Science Team members *Caveat Observations have uncertainties (Dolinar et al. 2014) but are used as truth in this study 2

Study Groundwork 28 uncoupled - AMIP (atmosphere-only) models Climatologically prescribed SSTs 03/2000 02/2008 (8 years) SML: 70 30 South Ocean 3

Cloud Fraction (CF) Comparison Observations [81.5%] Multimodel Ensemble [69.3%] Bias [ 12.2%] Model simulated total cloud fraction is largely under estimated over the SMLs compared to CERES-MODIS observed CF 4

Cloud Water Path (Ice + Liquid) Observations [190.3 gm 2 ] A fair proxy for cloud optical depth Multimodel Ensemble [134.5 gm 2 ] Bias [ 55.8 gm 2 ] Model simulated cloud water path is largely under estimated in the SMLs compared to CERES-MODIS observation 5

CF Profile The under estimation of CF in the SML oceans is primarily a result of under estimated low- and midlevel (950 500 hpa) clouds. There does exist some over estimation of cloud fraction at higher levels (~250 hpa) At 850 hpa Multimodel Mean: 24.5% CCCM: 43.5% Bias: -19.0% 6 *Only 23 simulations available

Vertical Velocities Convective cloud types are commonly parameterized by the consideration of mass flux and vertical velocities while stratiform-type cloud schemes are based upon RH relationships At 850 hpa MERRA: 1.0 hpa day -1 (down) Multimodel Mean: -0.1 hpa day -1 Regime shift The dynamic forcing in this region is different (or slightly modified) than what is observed (reanalyzed) 7 Up Down *Only 26 simulations available

Vertical Velocities at 850 hpa Down Up Down Up The overall distribution of vertical velocities (convection/subsidence) at 850 hpa is correctly simulated by the multimodel ensemble in the Southern Mid-latitudes, but either the strength of the descending branch of the Hadley Cell is weaker or the ascending branch of the Ferrell Cell is stronger than reanalyzed ones 8

Cloud Fraction at ~850 hpa Observations [43.5%] Multimodel Ensemble [24.5%] Bias [ 19.0%] The largest biases at ~850 hpa coincide with the ascending/descending branches of the Hadley and Ferrell Cells 9

Summary I: CF Comparisons Total column cloud fraction is under estimated, on average, by the 28 model ensemble by 12.2% in the Southern mid-latitudes over the ocean Cloud water path is under estimated by 55.8 gm 2 Currently large uncertainties in observed CWC profiles Cloud fraction is under estimated by ~20% in the low-levels (~850 hpa) (23/28 models) Due to, but not limited to, a potential dynamical regime shift or lack of cloud water Would be interesting to analyze other simulated synoptic conditions What effect do these results have on the TOA radiation budget? 10

Reflected SW and OLR Flux differences (Model CERES) eled TOA reflectedswfluxishigherwhile OLR is lower CERES observations over the SMLs se results do not make physical sense compared to restimated CF and CWP in model

TOA SW and LW CRF differences (Model CERES) CRF = All - Clr The magnitude of TOA SW (LW) CRF cooling (warming) is underestimated in the SMLs Regions of positive (negative) biases are consistent with the SW (LW) radiation flux results 12

The simulated magnitude of the Net CRF cooling is under estimated in the SMLs but there does exist an area of stronger cooling due to clouds between S. America and Australia in the models Summary II: TOA Radiation Results All TOA radiation and the cloud radiative heating/cooling is under estimated in the SMLs Areas of over estimated SW/Net cooling due to clouds Results are consistent with each other but not with corresponding CF and CWP results Less clouds, more reflection/cooling and less outgoing/warming? How? A topic for further consideration and research 13

Acknowledgements Workshop organizers Drs Jonathan Jiang and Hui Su at JPL for their help and support over the past year Research group at UND All of you! 14

Questions erica.dolinar@my.und.edu 15

Backup 16

Modeling Center (or Group) Model Name Grid Spacing Commonwealth Scientific and Industrial Research Organization (CSIRO) and Bureau of ACCESS1.0 1.875 1.25, L38 Meteorology (BOM), Australia Beijing Climate Center, China Meteorological Administration BCC-CSM1.1 BCC-CSM1.1 (m) 1.25 1.25, L26 2.8125 2.8125, L26 College of Global Change and Earth System Science, Beijing Normal University, China BNU-ESM 2.8125 2.8125, L26 Canadian Centre for Climate Modeling and Analysis CanAM4 2.8125 2.8125, L35 National Center for Atmospheric Research (NCAR), USA CCSM4 1.25 0.9375, L26 Community Earth System Model Contributors (NSF- DOE-NCAR), USA CESM1 (CAM5) 1.25 0.9375, L30 Centro-Euro-Mediterraneo per I Cambiamenti Climatici, Italy CMCC-CM 0.75 0.75, L31 Centre National de Recherches Meteorologiques/ Centre Europeen de Recherche et Formation Avancees en Calcul CNRM-CM5 1.4 1.4, L31 Scientifique, France Commonwealth Scientific and Industrial Research Organization in collaboration with Queensland CSIRO-Mk3.6.0 1.875 1.875, L18 Climate Change Centre of Excellence, Australia LASG, Institute of Atmospheric Physics, Chinese Academy of Sciences CESS, Tsinghua University FGOALS-s2 FGOALS-g2 2.8125 1.666, L26 2.8125 3.0, L26 NOAA Geophysical Fluid Dynamics Laboratory, USA GFDL-CM3 GFDL-HIRAM-C180 GFDL-HIRAM-C360 2.5 2.0, L48 0.625 0.5, L32 0.3125 0.25, L32 NASA Goddard Institute for Space Studies, USA GISS-E2-R 2.5 2.0, L29 Met Office Hadley Centre, United Kingdom HadGEM2-A 1.875 1.25, L38 Institute for Numerical Mathematics, Russia INM-CM4 2.0 1.5, L21 Institut Pierre-Simon Laplace, France IPSL-CM5A-LR IPSL-CM5A-MR IPSL-CM5B-LR 3.75 1.875, L39 2.5 1.25, L39 3.75 1.875, L39 Atmosphere and Ocean Research Institute (The University of Tokyo), National Institute for Environmental Studies, and Japan Agency for Marine- MIROC5 1.4 1.4, L40 Earth Science and Technology Max Planck Institute for Meteorology, Germany MPI-ESM-MR MPI-ESM-LR 1.875 1.875, L95 1.875 1.875, L47 Meteorological Research Institute, Japan MRI-AGCM3.2H MRI-AGCM3.2S MRI-CGCM3 0.5625 0.5625 0.1875 0.1875 1.125 1.125, L35 Norwegian Climate Centre 17 NorESM1-M 2.5 1.875, L26

Relative Humidity 15-20% uncertainty in AIRS RH Stratiform type clouds are commonly parameterized with the consideration of relative humidity Relative humidity is over estimated at all levels (with the exception of one model below 900 hpa) BUT we do not know which models contain both liquid and ice RHs so we will not put any faith in these results 18 *Only 13 simulations available

Summary Variable Observed Mean* Ensemble Mean Mean Bias** Cloud Fraction 81.5 69.3 ± 8.0 12.2 Cloud Water Path 190.3 134.5 ± 47.0 55.8 TOA Reflected SW 105.3 103.6 ± 8.1 1.7 TOA Outgoing LW 223.8 222.5 ± 3.9 1.3 TOA SW CRF 63.1 60.8 ± 8.9 2.3 TOA LW CRF 28.9 27.0 ± 5.2 1.9 TOA Net CRF 34.2 33.8 ± 5.8 0.4 *Observed values are from CERES MODIS/EBAF ** Mean biases in CRFs correspond to the relative warming/cooling effects 19