Vertical Discretization in the NCAR Community Atmospheric Model CAM 2'0 PowerPoint PPT Presentation

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Title: Vertical Discretization in the NCAR Community Atmospheric Model CAM 2'0


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Method of Vertical Discretization in the NCAR
Community Atmospheric Model (CAM 2.0)
  • AT 745
  • September 25, 2002
  • Jonathan Vigh

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What is the CAM 2.0?
  • The atmospheric component of the Community
    Climate System Model (CCSM), a comprehensive
    climate modeling system developed and maintained
    by NCAR and the university community
  • Previously called the Community Climate Model
    (CCM)

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Brief Overview CCM0A (c. 1982)
  • CCM0A was based on the Australian spectral model
    developed by Bourke, McAvaney, Puri, and Thurling
  • Was modified to adopt more efficient Fourier
    transform routines and the improved
    radiation/cloudiness parameterizations of
    Ramanathan and Dickinson
  • Focus was climate simulations

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Brief Overview CCM0B (c. 1983)
  • In 1981, decision was made that one model should
    serve both climate research and forecasting
    research
  • CCM0A was scrapped in favor of a new version
    based on the adiabatic, inviscid version of the
    spectral model developed at ECMWF
  • Vertical and temporal finite differences matched
    the Australian spectral model
  • New model included physical parameterizations
    for
  • Radiation and cloud routines
  • Convective adjustment
  • Stable condensation
  • Vertical diffusion
  • Surface fluxes
  • Surface-energy-balance prescription

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Brief Overview CCM1 (Jul 1987)
  • Substantial changes included
  • Radiation scheme modified
  • Vertical finite-difference approximations were
    modified to conserve energy without adversely
    affecting the model simulations
  • Frictional heating included
  • Horizontal diffusion modified to hyperdiffusion
    form in troposphere
  • Local moisture adjustment was generalized for a
    global horizontal borrowing in a conserving
    manner
  • Vertical diffusion was converted to a nonlinear
    form for which eddy-mixing coefficient depended
    on local shear and stability (applied throughout
    whole atmosphere eliminated need for dry
    convective adjustment in troposphere)
  • Surface drag coefficient made a function of
    stability (Deardorff, 1972)
  • Equation of state modified to formally account
    for moisture in the atmosphere (using Tv when
    appropriate)
  • Climate mode had optional seasonal mode with
    interactive hydrology
  • Method of initialization for global forecast mode

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Brief Overview CCM2 (Oct 1992)
  • Changes in model formulation were so extensive
    that it should not be thought of as being evolved
    from CCM1
  • T42L18 (approximately 2.8 x 2.8 deg resolution,
    top at 2.917 mb)
  • The following were carried over from CCM1
  • Semi-implicit, leap-frog time integration scheme
  • Spectral transform method for treating the dry
    dynamics
  • Bi-harmonic horizontal diffusion operator

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CCM2 Changes, contd.
  • Shape preserving Semi-Lagrangian Transport (SLT)
    methods used for the advection of water vapor and
    other scalar fields
  • Incorporation of a terrain-following hybrid
    vertical coordinate (Simmons and Strüfing, 1981),
    but allows an upper boundary at finite height as
    in Kasahara (1974)
  • A d-Eddington approximation used to calculate
    solar absorption
  • Cloud radiative parameterization of Slingo (1989)
  • Diurnal cycle included
  • Land and sea ice surfaces are included with and
    without snow cover
  • Subsurface temperatures obey a thermal diffusion
    equation
  • Net energy flux at surface/atmosphere interface
    is calculated using bulk exchange formulae in
    which the transfer coefficients depend on
    stability
  • Cloud fraction parameterization a generalization
    of Slingo (1987)
  • Cloud fraction depends on RH, vertical motion,
    static stability, and convective precipitation
    rate
  • Turbulence in PBL mixes heat, moisture, momentum
    and passive scalars
  • Simple mass flux scheme by Hack (1993) used to
    represent all types of moist convection
  • Biosphere-Atmosphere Transfer Scheme of Dickinson
    et al. (1986) available

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Brief Overview CCM3 (1996)
  • Major changes in parameterized physics, modest
    changes in dynamical formulation
  • Modification in physics made to
  • Address serious systematic errors and biases in
    CCM2 simulations (in TOA and surface energy
    budgets)
  • Allow for more suitable coupling of the model
    atmosphere with land, ocean, and sea-ice
    component models
  • Changes fall under five categories
  • Modifications to the representation of radiative
    transfer through both clear and cloudy
    atmospheric columns
  • Modifications to hydrologic processes (PBL, moist
    convection, and surface energy exchange)
  • Incorporation of sophisticated land surface model
  • Incorporation of an optional slab mixed-layer
    ocean/thermodynamic sea-ice component
  • Other changes in model formalism which dont
    significantly change the model climate

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Brief overview of CAM 2.0 (2002)
  • Incorporated prognostic cloud-water
    parameterization (Rasch and Kristjansson,1998)
  • Incorporated scheme to allow a greater variety of
    cloud overlap assumptions (Collins, 2001)
  • Updated water vapor absorptivity and emissivity
    with work of Collins, Hackney, and Edward (2002)
  • Standard model grid has 26 vertical grid levels,
    with the additional levels added near the
    tropopause
  • New ozone dataset (1990 NOAA) and new topography
    with diffusive filter to smooth oceanic ridges
  • Sea-ice model replaced with simplified
    thermodynamic version of the CCSM Community
    Sea-Ice Model (CSIM4)
  • Community Land Model (CLM2.0) replaces previous
    land model (LSM1)
  • Model operates on true land, ocean, and ice
    fractional areas rather than binary
    representation
  • Atmospheric model now determines partitioning of
    rain and snow rather than the land-surface model
  • Added precipitation evaporation to model
  • Orographic drag was removed from ocean
  • Code made more modular for testing of various
    physics packages

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Computational Environment
  • Code has been reworked for a distributed
    computing environment (massively parallel
    processing)
  • Support for IBM SP3 clusters and Linux PC
  • Many runs are done at NCAR on the IBM SP3 running
    at 1.27 TF/s (18th fastest computer in the world)
  • BlueSky gets delivered Oct. 2002
  • (9 TF/s, 2nd ranked if list stood still)
  • Compare to
  • NEC Earth Simulator (35.86 TF/s, 1st ranked)
  • ECMWF/IBM (1.84 TF/s, 12th ranked)
  • NAVOCEANO (1.41 TF/s, 16th ranked)
  • NCEP/IBM (1.18 TF/s, 20th and 21st ranked) -gt 5
    TF/s by 2003, 50 TF/s by 2009

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