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Physical Climate Models

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Title: Physical Climate Models


1
Physical Climate Models
  • Simulate behavior of climate system
  • Ultimate objective
  • Understand the key physical, chemical and
    biological processes that govern climate
  • Obtain a clearer picture of past climates by
    comparison with empirical observation
  • Predict future climate change
  • Models simulate climate on a variety of spatial
    and temporal scales
  • Regional climates
  • Global-scale climate models simulate the
    climate of the entire planet

2
Climate Processes
  • Three processes that must be considered when
    constructing a climate model
  • 1) radiative - the transfer of radiation through
    the climate system (e.g. absorption, reflection)
  • 2) dynamic - the horizontal and vertical transfer
    of energy (e.g. advection, convection,
    diffusion)
  • 3) surface process - inclusion of processes
    involving land/ocean/ice, and the effects of
    albedo, emissivity and surface-atmosphere energy
    exchanges

3
Constructing Climate Models
  • Basic laws and relationships necessary to model
    the climate system are expressed as a series of
    equations
  • Equations may be
  • Empirical derivations based on relationships
    observed in the real world
  • Primitive equations that represent theoretical
    relationships between variables
  • Combination of the two
  • Equations solved by finite difference methods
  • Must consider the model resolution in time and
    space i.e. the time step of the model and the
    horizontal/vertical scales

4
Simplifying the Climate System
  • All models must simplify complex climate system
  • Limited understanding of the climate system
  • Computational restraints
  • Simplification may be achieved by limiting
  • Space and time resolution
  • Parameterization of the processes that are
    simulated

5
Model Simplification
  • Simplest models are zero order in spatial
    dimension
  • The state of the climate system is defined by a
    single global average
  • Other models include an ever-increasing
    dimensional complexity
  • 1-D, 2-D and finally to 3-D models
  • Whatever the spatial dimension, further
    simplification requires limiting spatial
    resolution
  • Limited number of latitude bands in a 1-D model
  • Limited number of grid points in a 2-D model
  • Time resolution of climate models varies
    substantially, from minutes to years depending on
    the models and the problem under investigation
  • To preserve computational stability, spatial and
    temporal resolution must be linked
  • Can pose problems when systems with different
    equilibrium time scales have to interact as a
    very different resolution in space and time may
    be needed

6
Parameterization
  • Involves inclusion of a process as a simplified
    function rather than an explicit calculation from
    first principles
  • Sub-grid scale phenomena, like thunderstorms,
    must be parameterized
  • Not possible to deal with these explicitly
  • Other processes are parameterized to reduce
    computation required
  • Certain processes omitted from model if their
    contribution negligible on time scale of interest
  • Role of deep ocean circulation while modeling
    changes over time scales of years to decades
  • Models may handle radiative transfers in detail
    but neglect or parameterize horizontal energy
    transport
  • Models may provide 3-D representation but contain
    much less detailed radiative transfer information

7
Modeling Climate Response
  • Ultimate purpose of a model
  • Identify response of the climate system
  • Change in the parameters and processes that
    control the state of the system
  • Climate response occurs to restore equilibrium
    within the climate system
  • If radiative forcing associated with an increase
    in atmospheric CO2 perturbs the climate system
  • Model will assess how the climate system responds
    to this perturbation to restore equilibrium

8
Model Equilibrium
  • Model may require many years of simulated change
    to reach equilibrium
  • Final years of simulation averaged

9
Nature of the Model
  • One of two modes
  • Equilibrium mode
  • No account taken of energy storage processes that
    control evolution of climate response with time
  • Assume climate responds instantaneously following
    system perturbation
  • Transient mode
  • Inclusion of energy storage processes
  • Simulate development of a climate response with
    time
  • Models typically run twice
  • In a control run with no forcing
  • In a test run including forcing and perturbation
    of the climate system

10
Climate Sensitivity
  • Critical parameters
  • In the most complex models
  • Climate sensitivity calculated explicitly through
    simulations of processes involved
  • In simpler models
  • Climate sensitivity is parameterized by reference
    to the range of values suggested by the more
    complex models
  • This approach, where more sophisticated models
    are nested in less complex models, is common in
    the field of climate modeling

11
Data-Model Comparisons
  • Models constructed to simulate Modern circulation
  • Changes based on Earth History inserted in model
  • Climate output compared with observations

12
One-Dimensional Models
  • Simplified representation of of entire planet
  • Model driven by global mean incoming solar
    radiation and albedo
  • Single vertical column of air divided into layers
  • Each layer contains important constituents (dust,
    greenhouse gases, etc)
  • Layers exchange only vertically

13
Types of Models
  • Energy balance models (EBMs)
  • Simulate two fundamental climate processes
  • Global radiation balance
  • Latitudinal (equator-to-pole) energy transfer
  • Radiative-convective models (RCMs)
  • Simulate detailed energy transfer through the
    depth of the atmosphere
  • Radiative transformations that occur as energy is
    absorbed, emitted and scattered
  • Role of convection

14
EBMs
  • 0-D EBMs
  • Earth is a single point in space
  • Global radiation balance modeled
  • In 1-D models latitude is included
  • Temperature for each latitude band is calculated
  • Using latitudinal value for albedo, energy flux,
    etc.
  • Latitudinal energy transfer estimated from linear
    empirical relationships
  • Difference between latitudinal temperature and
    global average temperature

15
RBMs
  • Surface albedo, cloud amount and atmospheric
    turbidity
  • Used to determine heating rates atmospheric
    layers
  • Imbalance between net radiation at top and bottom
    of each layer determined
  • If calculated vertical temperature profile (lapse
    rate) exceeds some stability criterion (critical
    lapse rate)
  • Convection is assumed to take place (i.e. the
    vertical mixing of air) until the stability
    criterion is no longer breached

16
Two-Dimensional Models
  • Multi-layered atmosphere coupled with Earths
    physical properties averaged by latitude
  • Allows simulations of climatic processes that
    vary with latitude
  • Angle of incoming solar radiation
  • Albedo of Earths surface
  • Heat capacity changes

17
Statistical-Dynamical Models
  • Combine horizontal energy transfer modeled by
    EBMs with the radiative-convective approach of
    RCMs
  • Equator-to-pole energy transfer is more
    sophisticated
  • Parameters like wind speed and wind direction
    modeled by statistical relations
  • Laws of motion are used to obtain a measure of
    energy diffusion
  • Particular useful to investigate role of
    horizontal energy transfer and processes that
    directly disturb that transfer

18
2-D Models
  • Advantage
  • Simulate long intervals of time quickly and
    inexpensively
  • Disadvantage
  • Not sensitive to climate processes that depend on
    geographic position of continents and oceans

19
Three-Dimensional Models - GCM
  • 3-D representation of Earths surface and
    atmosphere
  • Most sophisticated attempt to simulate the
    climate system
  • 3-D model based on fundamental laws of physics
  • Conservation of energy
  • Conservation of momentum
  • Conservation of mass
  • Ideal Gas Law

20
GCMs
  • Represent key features affecting climate
  • Spatial distribution of land, water, ice
  • Regional variation in heat capacity and albedo of
    surface
  • Elevation of mountains and glaciers
  • Concentrations of greenhouse gases
  • Seasonal variations in solar radiation
  • Calculations at interactions of grid boxes

21
GCMs
  • Atmospheric variables at each grid point requires
    the storage, retrieval, recalculation and
    re-storage of 105 figures at every time-step
  • Models contain thousands of grid points
  • GCMs are computationally expensive
  • Can provide accurate representations of planetary
    climate
  • Simulate global and continental scale processes
    in detail
  • GCMs cannot simulate synoptic regional
    meteorological phenomena (e.g.,tropical storms)
  • Play an important part in the latitudinal
    transfer of energy and momentum
  • Spatial resolution of GCMs limited in vertical
    dimension
  • Many boundary layer processes must be
    parameterized

22
Sensitivity Test
  • Control case established
  • Modern climate simulated
  • One boundary condition altered at a time
  • Model output compared with present day climate
    simulation
  • Information reveals impact of that boundary
    condition
  • Boundary condition examples
  • Continental configuration
  • Ice sheet expansion
  • Solar radiation influx
  • Greenhouse gas concentrations

23
Model Resolution
  • Can it image New Zealand? this is probably now
    out of date! (2 lat x 3 long)

24
Atmospheric and Ocean GCMs
  • Atmospheric GCM more sophisticated
  • Much detail known about atmospheric circulation,
    elevations, landmasses, etc.
  • Ocean GCM primitive
  • Rudimentary knowledge of oceanic circulation
  • Deep water formation
  • Difficult to model important small features
  • Fast-moving narrow currents

25
Oceanic GCMs
  • Similar in construction to atmospheric GCM
  • Lower boundary seafloor
  • Water column divided grid boxes
  • Low resolution, fewer layers/boxes, biology
  • Output temperature, salinity, sea ice, gases

26
Atmospheric and Ocean GCMs
  • Oceanic GCMs simulates circulation over several
    years to decades
  • Atmospheric GCMs simulates circulation over
    several hours to weeks
  • Basic incompatibility between models
  • A-GCMs may be used to drive O-GCMs
  • Asynchronous coupling
  • Atmospheric conditions drive ocean
  • Oceanic conditions drive atmosphere
  • Alternation keeps systems from getting wacky

27
Geochemical Models
  • Mass balance models
  • Follow movement of Earth materials from one
    reservoir to another
  • Physical or chemical form
  • Models focus on sources, rates of transfer and
    depositional fate of materials
  • Commonly trace fate of materials using a
    geochemical tracer
  • Example 18O content of seawater

28
One-way Mass Transfer Models
  • Movement from source to sink
  • Movement from one reservoir to another
  • If materials transferred has unique chemical or
    physical signature
  • Flux rate (mass transfer time-1) can be
    determined
  • Example calving of icebergs
  • Influx of ice-rafted debris
  • Determined by physical sedimentology
  • Quantified by point-counts

29
Mass Balance Equations
  • Simple mass balance
  • Ftotal F1 F2 F3
  • Tracer mass balance
  • TR (F1T1 F2T2 F3T3)/(F1 F2 F3)
  • TR is the mean value of tagged inputs
  • Mass balance of two components in system
  • Tracer entering tracer leaving
  • TR Æ’inTin (1 Æ’out)Tout

30
Tracer Mass Balance Example
  • Global carbon redox balance
  • Average d13C of carbon on Earth -4.6
  • CO2 in hydrothermal vents
  • Average d13C of carbonates 0.6
  • Average d13C of organic carbon -25.4
  • Know
  • 13C entering 13C leaving
  • dR Æ’odo (1 Æ’o)dcarb
  • 4.6 Æ’o(-25.4) (1 Æ’o)0.6
  • 20 of carbon buried in marine sediments is
    organic carbon

31
Chemical Reservoirs
  • Earth reservoirs
  • Atmosphere, ocean, ice, vegetation and sediments
  • Ocean most important reservoir
  • Interacts with other reservoirs
  • Receives weathering products
  • New minerals deposited in sediments
  • Tracer is carried to ocean, mixed and trapped in
    sedimentary mineral archive

32
Steady State Tub
  • If flux of tracer into and out of reservoir are
    equal, the system is at steady state

33
Residence Time
  • Time it takes for tracer to pass through tub
  • Residence time reservoir size/flux
  • Residence time of tracer typically gt mixing time
    of the ocean (1500 y)
  • Tracer distribution homogenous
  • Tracer concentration or isotopic composition is
    everywhere equal
  • Records whole-ocean chemistry during deposition

34
Reservoir Exchange Models
  • Models can be designed to track reversible
    exchange between different sized reservoirs

35
Reservoir Exchange
  • Monitor cycling of tracers between reservoirs
    through time
  • Tracer with distinctive value moves freely
    between reservoirs
  • Typically between small and large reservoirs
  • Ocean and atmosphere, vegetation, land
  • Monitors change in size of smaller reservoir
  • Tracer exchange detected in sedimentary minerals
  • Exchange produces change in volume and tracer
    value in ocean

36
Reservoir Exchange Example
  • Change in the d18O of seawater
  • d18O of glacial ice and seawater different
  • Change in glacial ice volume
  • Produces small changes in the oxygen isotopic
    composition of seawater
  • Change in seawater d18O recorded
  • Calcareous shells or sediment porewater
  • Glacial ice small reservoir and ocean large
    reservoir

37
Time-Dependent Models
  • Most geochemical models assume steady-state
    conditions
  • Time-dependent models assume steady-state only
    during equilibrium conditions
  • Steady-state conditions imply no change in
    reservoir size
  • Time-dependent models allow changes in reservoir
    size
  • From one equilibrium state to another
  • Under equilibrium
  • Steady-state conditions prevail

38
CO2 and Long-Term Climate
  • What has moderated Earth surface temperature over
    the last 4.55 by so that
  • All surface vegetation did not spontaneously
    catch on fire and all lakes and oceans vaporize?
  • All lakes and ocean did not freeze solid?

39
Greenhouse Worlds
  • Why is Venus so much hotter than Earth?
  • Although solar radiation 2x Earth, most is
    reflected but 96 of back radiation absorbed

40
What originally controlled C?
  • In solar nebula most carbon was CH4
  • Lost from Earth and Venus
  • Earth captured 1 in 3000 carbon atoms
  • Tiny carbon fraction in the atmosphere as CO2
  • 60 out of every million C atoms
  • Bulk of carbon in sediments on Earth
  • CaCO3 (limestone and dolostone) and organic
    residues (kerogen)
  • Venus probably had similar early planetary
    history
  • Most carbon is in atmosphere as CO2
  • Venus has conditions that would prevail on Earth
  • All CO2 locked up in sediments were released to
    the atmosphere

41
Earth and Venus
  • Water balance different on Earth and Venus
  • If Venus and Earth started with same components
  • Venus should have either
  • Sizable oceans
  • Atmosphere dominated by steam
  • H present initially as H2O escaped to space
  • H2O transported "top" of the Venusian atmosphere
  • Disassociated forming H and O atoms
  • H escaped the atmosphere
  • Oxygen stirred back to surface
  • Reacted with iron forming iron oxide

42
Planetary Evolution Similar
  • Although Earth and Venus started with same
    components
  • Earth evolved such that carbon safely buried in
    early sediments
  • Avoiding runaway greenhouse effect
  • Venus built up CO2 in the atmosphere
  • Build-up led to high temperature
  • High enough to kill all life
  • If life ever did get a foothold
  • Once hot, could not cool

43
Why Runaway Greenhouse?
  • Don't know why Venus climate went haywire
  • Extra sunlight Venus receives?
  • Life perhaps never got started?
  • No sink for carbon in organic matter
  • Was the initial component of water smaller than
    that on Earth?
  • Did God make Venus as a warning sign?

44
Early Earth Faint Young Sun
  • Solar Luminosity 4.55 bya 25 lower than today
  • Faint young Sun paradox
  • If early Earth had no atmosphere or todays
    atmosphere
  • Radiant energy at surface well below 0C for
    first 3 billion years of Earth history
  • No evidence in scant Archean rock record that
    planet was frozen

45
Early Earth A Greenhouse World
  • Earth was more Venus-like during Archean
  • Models indicate that greenhouse required
  • Several greenhouse gases
  • H2O, CO2, CH4, NH3, N2O
  • H2O and CO2 most likely
  • 102-103 x PAL CO2

46
Archean Atmosphere
  • Faint young Sun paradox presents dilemma
  • 1) What is the source for high levels of
    greenhouse gases in Earths earliest atmosphere?
  • 2) How were those gases removed with time?
  • Models indicate Suns strength increased slowly
    with time
  • Geologic record strongly suggests Earth
    maintained a moderate climate throughout Earth
    history (i.e., no runaway greenhouse like on
    Venus)

47
Source of Greenhouse Gases
  • Input of CO2 and other greenhouse gases from
    volcanic emissions
  • Most likely cause of high levels in Archean
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