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Climate Modeling OCN760

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to develop the mathematical-physical basis of the climate components and their interactions ... Bering strait closure: preventing THC collapse. Term projects ... – PowerPoint PPT presentation

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Title: Climate Modeling OCN760


1
Climate ModelingOCN-760
  • Axel Timmermann

2
Prolegomena
3
Main goals of the class
  • to develop the mathematical-physical basis of the
    climate components and their interactions
  • to provide a practical introduction into
    numerical techniques used in climate research
  • to develop skills that help you to solve
    complicated climate problems with publicly
    available tools

4
Concept of climate modeling
Dynamical equations
Mechanisms
Climate model numerical solution
Thermodynamical equations
Model output
unresolved processes
Observations
climate forcing
5
Hierarchy of climate models
  • simplified models understanding basic processes
    and prediction
  • intermediate complexity models understanding
    interactions between components, paleo-modeling
  • comprehensive models comparison with
    observations, diagnosing mechanism, prediction

6
Climate models versus reality
climate processes
climate archives
climate data
climate model data
climate models
process studies
Synthesis
7
Limitations of climate models
  • a climate model is always a simplification of
    mother nature
  • complexity has different aspects number of
    unresolved processes and model resolution
  • both are limited
  • it is important to use a hierarchy of models to
    understand and to simulate nature, to
    flasify/verify hypotheses

8
Historical development
  • Vilhelm Bjerknes (1862-1951) suggests weather
    forecasting is a matter of mathematics and
    physics (deterministic, nonchaotic approach)
  • Lewis Fry Richardson (1881-1953) first numerical
    weather forecast 3x1.8 degree, 5 vertical layers
    over Europe, 12 (p,T) profiles over Europe as
    initial conditions, 24 hour forecast took 3
    months, primitive equations, unstable numerical
    technique

9
Historical development
  • N. Philipps 1955 first Atmospheric General
    Circulation Model run on ENIAC
  • Syukuro Manabe and Smagorinsky 1963-1969, fisrt
    coupled atmosphere-ocean model using flux
    corrections
  • since 1990s climate models include chemistry,
    carbon cycle, biosphere, vegetation etc -gt
    climate modeling becomes multidisciplinary

10
Climate goes engineering
  • 1969 Budyko disperse ashes over Siberia -gt
    reduce snow-covered area -gt more area for
    agriculture
  • iron ferilization of the oceans iron in Southern
    ocean -gt more biological productivity -gt drawback
    of atmospheric CO2
  • Bering strait closure preventing THC collapse

11
Term projects
  • Hasselmann's socio-economic climate model
  • Socio-economic-physical modeling using Gildors
    model
  • 1.5 layer equatorial beta plane model
  • Stationary Gill-type model
  • Simple ice-sheetsimple ocean model
  • barotropic vorticity equation and jets
  • Diagnostics of 4th AR models thermostats vs.
    runnaway-greenhouse effects
  • Patterns of sea-level rise and climate change for
    west-Antarctic ice sheet collapse (Thomas)
  • Exploration of JEBAR term in BARBIEy

12
Term projects
  • ENSO forecasting using nonlinear ENSO model
  • Paleo-ocean circulation with BARBIE
  • bifurcation analysis of hydrodynamical equations
  • geothermal processes and THC stability
  • POSTER of term projects

13
Components of the climate system and Earth system
history
14
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15
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16
Radiation and its influences on global climate
17
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18
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19
Energy balance of the earth
  • 4pR2 h?C dT/dtp R2 (1-a)S -4pR2 esT4
  • a Reflectivity 0.3
  • e Emissivity 0.6 (Erde, 1 black body)
  • C Specifiic heat of air 1000 J/kg/K
  • S Solarconstant 1367 W/m2
  • s5.67 10-8 Wm-2K-4
  • T(1-a)S/4/e/s)0.25

20
Energy Balance of the Earth
  • T black body -18.3 C
  • T for emissivity 0.6 15 C
  • Natural Greenhouse effect 33 Cdue to water vapor
  • However Problem is true emissivity is 0.8

21
Energy Balance of the earth
  • Introduce cirrus clouds that cover fraction c and
    have temperature T2, whereas ground temperature
    is T1
  • p R2 (1-a)S c4pR2 esT244pR2 esT14
  • with further geometrical considerations
  • using true e0.886
  • T2-38.8 C
  • T114 C
  • infrared radiation is emitted from each
    atmospheric level

22
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23
Climate Sensitivity
  • ? response of climate system to 1W/m2 radiation
    change
  • Albedo-Backscattered LW radiation climate
    feedbacks (clouds, CO2) Forcing 0
  • A(T)-B(T)W(T)Q'0
  • TTT'
  • A(T)-B(T)W(T)ATT'-BTT'WTT'Q'0
  • T'-Q'/(AT -BTWT)

24
Climate sensitivity
  • Climate sensitivity ?T'/Q'
  • -?-1?A-1-?B-1?W-1
  • EBM with clouds (1-a)S/4 -esT4 c/2 esT40
  • ?A-1-S/4 da/dT
  • ?B-14esT3
  • ?W-12c esT3esT4/2 dc/dT
  • let us assume only longwave feedback, no cloud
    and albedo effect
  • ?0.3 K/W/m2
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