an introduction to climate models: principles and applications
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An Introduction to Climate Models: Principles and Applications. William D. Collins National Center for Atmospheric Research Boulder, Colorado USA. Topics. The climate-change context Components of the climate system Representation of climate in global models The NCAR climate model CCSM3 - PowerPoint PPT PresentationTRANSCRIPT
Colloquium on Climate and Health17 July 2006
An Introduction to Climate Models:Principles and Applications
William D. CollinsNational Center for Atmospheric Research
Boulder, Colorado USA
Colloquium on Climate and Health17 July 2006
Topics
• The climate-change context
• Components of the climate system
• Representation of climate in global models
• The NCAR climate model CCSM3
• Applications to global change
• Transition from climate models to Earth system models
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Climate Simulations for the IPCC AR4(IPCC = Intergovernmental Panel on Climate Change)
IPCC Emissions Scenarios
Climate Change Simulations
IPCC 4th Assessment
Results:• 10,000 simulated years• Largest submission to IPCC• 100 TB of model output
2007
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Exchange of Energy in the Climate
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Components of the Climate System
Slingo
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Time Scales in the Climate System
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Configuration of NCAR CCSM3(Community Climate System Model)
Atmosphere(CAM 3.0)
T85 (1.4o)
Ocean(POP 1.4.3)
(1o)
Coupler(CPL 6)
Sea Ice(CSIM 4)
(1o)
Land(CLM2.2)
T85 (1.4o)
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Why are there multiple Climate Models?
• Ongoing research on processes:– The carbon cycle– Interactions of aerosols and clouds– Interactions of climate and vegetation
• No “1st principles” theories (yet) for:– Physics of cloud formation– Physics of atmospheric convection
• Inadequate data to constrain models
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• 1922: Lewis Fry Richardson– Basic equations and methodology of numerical weather prediction
• 1950: Charney, Fjørtoft and von Neumann (1950)– First numerical weather forecast (barotropic vorticity equation model)
• 1956: Norman Phillips– 1st general circulation experiment (two-layer, quasi-geostrophic hemispheric model)
• 1963: Smagorinsky, Manabe and collaborators at GFDL, USA– Nine level primitive equation model
• 1960s and 1970s: Other groups and their offshoots began work– University of California Los Angeles (UCLA), National Center for Atmospheric Research (NCAR, Boulder, Colorado)
and UK Meteorological Office
• 1990s: Atmospheric Model Intercomparison Project (AMIP)– Results from about 30 atmospheric models from around the world
• 2001: IPCC Third Assessment Report– Climate projections to 2100 from 9 coupled ocean-atmosphere-cryosphere models.
• 2007: IPCC Fourth Assessment Report– Climate projections to 2100+ from 23 coupled ocean-atmosphere-cryosphere models.
Brief History of Climate Modeling
Slingo
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Richardson’s Vision of a Climate Model
“Myriad computers are at work upon the weather of the part of the map where each sits, but each computer attends only to one equation or part of an equation. The work of each region is coordinated by an official of higher rank. Numerous little 'night signs' display the instantaneous values so that neighboring computers can read them. Each number is thus displayed in threeadjacent zones so as to maintain communication to North and South of the map…”
Lewis Fry RichardsonWeather Prediction by Numerical Process (1922)
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Evolution of Climate Models
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• Momentum equation:
dV/dt = -p -2^V –gk +F +Dm
• Where =1/ ( is density), p is pressure, is rotation rate of the Earth, g is acceleration due to gravity (including effects of rotation), k is a unit vector in the vertical, F is friction and Dm is vertical diffusion of momentum
• Thermodynamic equation:
dT/dt = Q/cp + (RT/p) + DH
• where cp is the specific heat at constant pressure, R is the gas constant, is the vertical velocity, DH is the vertical diffusion of heat and Q is the internal heating from radiation and condensation/evaporation; Q = Qrad + Qcon
• Continuity equation for moisture (similar for other tracers):
dq/dt = E – C + Dq
• where E is the evaporation, C is the condensation and Dq is the vertical diffusion of moisture
Basic Equations for the Atmosphere
Slingo
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Vertical Discretization of Equations
Vertical Grid for Atmosphere
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Horizontal Discretization of Equations
T31 T42
T85 T170
Strand
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• Processes that are not explicitly represented by the basic dynamical and thermodynamic variables in the basic equations (dynamics, continuity, thermodynamic, equation of state) on the grid of the model need to be included by parameterizations.
• There are three types of parameterization;1. Processes taking place on scales smaller than the grid-scale, which are therefore
not explicitly represented by the resolved motion;• Convection, boundary layer friction and turbulence, gravity wave drag
• All involve the vertical transport of momentum and most also involve the transport of heat, water substance and tracers (e.g. chemicals, aerosols)
2. Processes that contribute to internal heating (non-adiabatic)• Radiative transfer and precipitation
• Both require the prediction of cloud cover
3. Processes that involve variables additional to the basic model variables (e.g. land surface processes, carbon cycle, chemistry, aerosols, etc)
Physical Parameterizations
Slingo
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Parameterized Processes
Slingo
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The current version includes:• Biogeophysics• Hydrology• River routing
The next version will include:• Natural and human-mediated changes in land cover• Natural and human-mediated changes in ecosystem functions• Coupling to biogeogeochemistry
Drainage
Hydrology
Canopy Water
Evaporation
Interception
SnowMelt
Sublimation
ThroughfallStemflow
Infiltration Surface Runoff
Evaporation
Transpiration
Precipitation
Soil Water
Redistribution
Direct Solar
Radiation
Absorbed SolarRadiation
Diff
use
Sol
ar
Rad
iatio
n
Long
wav
e R
adia
tion
Reflected Solar Radiation
Em
itted
Lon
g-w
ave
Rad
iatio
n
Sen
sibl
e H
eat
Flu
x
Late
nt H
eat
Flu
x
ua0
Momentum FluxWind Speed
Soil Heat Flux
Heat Transfer
Pho
tosy
nthe
sis
Biogeophysics
Processes Included in the CCSM Land Model
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Subgrid Structure of the Land Model
Gridcell
Glacier Wetland Lake
Landunits
Columns
PFTs
UrbanVegetated
Soil Type 1
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“Products” of Global Climate Models
• Description of the physical climate:– Temperature– Water in solid, liquid, and vapor form– Pressure– Motion fields
• Description of the chemical climate:– Distribution of aerosols– Evolution of carbon dioxide and other GHGs– Coming soon: chemical state of surface air
• Space and time resolution (CCSM3):– 1.3 degree atmosphere/land, 1 degree ocean/ice– Time scales: hours to centuries
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The CCSM Program
Scientific Objectives:
• Develop a comprehensive climate model to study the Earth’s Climate.
• Investigate seasonal and interannual variability in the climate.
• Explore the history of Earth’s climate.
• Estimate the future of the environment for policy formulation.
Recent Accomplishments:
• Release of a new version (CCSM3) to the climate community.
• Studies linking SST fluctuations, droughts, and extratropical variability.
• Simulations of last 1000 years, Holocene, and Last Glacial Maximum.
• Creation of largest ensemble of simulations for the IPCC AR4.
http://www.ccsm.ucar.edu
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The CCSM Community
Atmosphere(CAM 3)
Ocean(POP 1)
Coupler(CPL 6)
Sea Ice(CSIM 4)
Land(CLM 3)
CCSM3
Model Users Climate Community
Development Group
NCAR Universities Labs
Physics Applications Chemistry
Current Users:• Institutions: ~200
Downloads of CCSM3:• Users: ~600
Publications:• NCAR: 87• Universities: 94• Labs/Foreign: 48
Total: 229
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Changes in Atmospheric Composition
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Forcing: Changes in Exchange of Energy
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Back Scattering (Cooling)
Absorption(Atmospheric Warming)
Dimming of Surface Surface Cooling
Absorption (Column Warming)
Cloud Evaporation(Warming)Cloud Seeding(Cooling)
Suppression of Rain; increase of life time (Cooling)
Forward Scattering
Components of Aerosol Forcing
Ramaswamy
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Simulations of Aerosol Distributions
1995-2000
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Fidelity of 20th Century Simulations with the CCSM3
• Criteria for the ocean/atmosphere system
– Realistic prediction of sea-surface temperature given realistic forcing
– Realistic estimates of ocean heat uptakeEffects of ocean on transient climate response
– Realism of ocean mixed layer and ventilationOcean uptake of CO2 and passive tracers (CFCs)
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Simulation of Sea-Surface Temperature
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Increases in Global Ocean Temperatures(Results from CCSM3 Ensemble)
Gent et al, 2005
L = Levitus et al (2005)
EnsembleMembers
Relative ModelError < 25%
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Global Ocean Inventory of CFC-11(Passive tracer proxy for CO2)
Gent et al, 2005
EnsembleMembers}
Data
CCSM3
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Penetration Depth of CFC-11
WOCE data (Willey et al, 2004)
Gent et al, 2005
CCSM3 Simulation
m
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Projections for Global Surface Temperature
Meehl et al, 2005
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Projections for Regional Surface Temperature Change
Meehl et al, 2005
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Projections for Global Sea Level
Meehl et al, 2005
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Committed Change:Global Temperature and Sea Level
Teng et al, 2005
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Changes in Sea Ice Coverage
Meehl et al, 2005
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Changes in Permafrost Coverage
Lawrence and Slater, 2005: Geophys. Res. Lett.
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Scientific objectives for the near future
• Major objective: Develop, characterize, and understand the most realistic and comprehensive model of the observed climate system possible.
• Subsidiary objectives:– Analyze and reduce the principal biases in our
physical climate simulations using state-of-the-art theory and observations.
– Simulate the observed climate record with as much fidelity as possible.
– Simulate the interaction of chemistry, biogeochemistry, and climate with a focus on climate forcing and feedbacks.
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Recent evolution of climate forcing
Hansen and Sato, 2001
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Simulating the chemical state of the climate system
EmissionsChemistry + BGC +
Physics + Ecosystems
ChemicalReservoirs
Concentrations ForcingClimateResponse
Feedbacks
• In the past, we have generally used offline models to predict concentrationsand read these into CCSM.
• This approach is simple to implement, but It cuts the feedback loops. It eliminates the chemical reservoirs.
• The next CCSM will include these interactions.
Offline models
Feedbacks
ChemicalReservoirs
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CCSM4: a 1st generation Earth System Model
Atmosphere Ocean
Coupler
Sea IceLand
C/NCycle
Dyn.Veg.
Ecosystem & BGCGas chem.Prognostic
AerosolsUpperAtm.
LandUse
IceSheets
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Historical changes in agricultural land use
Johan Feddema
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Changes in surface albedo by land use
Johan Feddema
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Evolution of tropospheric ozone(1890-2100, following A2 scenario)
Lamarque et al, 2005
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Flux of CO2 into the world oceans(Ocean ecosystem model)
Moore, Doney, and Lindsay
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Conclusions
• Modern climate models can be applied to:– Studying the integrated climate system
– Modeling climates of the past
– Projecting future climate change and its impact
• Challenges ahead for modelers:– Process-oriented modeling of the climate
– Coupled chemistry/climate modeling
• Challenges ahead for the community:– Better linkages between modelers, health specialists, & policy makers
– Better modeling of chemical and biological climate change