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JCSDA Community Radiative Transfer Model (CRTM)

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Title: JCSDA Community Radiative Transfer Model (CRTM)


1
JCSDACommunity Radiative Transfer Model (CRTM)
  • Paul van Delst (CIMSS)
  • Yong Han (NESDIS)
  • Quanhua Liu (QSS)


5th MURI Workshop 7-9 June 2005 Madison WI
2
JCSDA Mission
  • Accelerate and improve the quantitative use of
    research and operational satellite data in
    weather and climate prediction models

JCSDA Partners
NOAA/NWS/NCEP Environmental Modeling Center NASA/GSFC Global Modeling Assimilation Office
NOAA/NESDIS Office of Research and Applications NOAA/OAR Office of Weather and Air Quality
US Navy Oceanographer of the Navy Naval Research Laboratory (NRL) US Air Force Air Force Director of Weather Air Force Weather Agency
3
JCSDA Goals
  • Reduce from two years to one year the average
    time for operational implementation of new
    satellite technology
  • Increase uses of current satellite data in NWP
    models
  • Advance the common NWP models and data
    assimilation infrastructure
  • Assess the impacts of data from advanced
    satellite sensors on weather and climate
    predictions

4
CRTM Contributors
  • JCSDA/CIMSS. Framework, CloudScatter, IR
    SfcOptics for water, RTSolution for validation
    (VDISORT)
  • AER Inc Jean-Luc Moncets group. OSS
    AtmAbsorption.
  • NOAA/ETL Al Gasiewskis group. CloudScatter (?W)
    and RTSolution.
  • NASA/GSFC Clark Weaver. AerosolScatter (IR).
  • NOAA/NESDIS Fuzhong Wengs group. Microwave
    SfcOptics for land, snow, ice.
  • AOS/SSEC/CIMSS/UWisc-Madison Ralf Bennartzs
    group. SOI RTSolution.
  • UCLA Kuo-Nan Lious group. ?-4 stream
    RTSolution.

5
CRTM Schematic
6
What is the CRTM Framework?
  • At the simplest level, its a collection of
    structure definitions, interface definitions, and
    stub routines.
  • There are User and Developer interfaces, as well
    as Shared Data interfaces and I/O.

Why do this?
  • The radiative transfer problem is split into
    various components (e.g. gaseous absorption,
    scattering etc) to facilitate independent
    development.
  • Want to minimise or eliminate potential software
    conflicts and redundancies.
  • Components developed by different groups can
    simply be dropped into the framework.
  • Faster implementation of new science/algorithms.

http//cimss.ssec.wisc.edu/paulv/CRTM
7
AtmAbsorption (1)
  • Two methodologies
  • OPTRAN. Polychromatic (two versions). Adjoint
    Jacobians.
  • OSS. Monochromatic. Analytic Jacobians.

OPTRAN OSS
Total channel resolution transmittance Predict band transmittance for each absorbing gas from absorption coefficient, ?, predicted from regression fits Select the regression coefficients, cijk, for each gas that minimises transmittance errors. Channel radiances are obtained from a weighted sum of monochromatic radiances for a set of predefined nodes, The monochromatic Rn are obtained from the OSS monochromatic optical depth profiles for the selected node frequencies. Nodes are selected and weights calculated for a channel to satisfy a specified accuracy (e.g. 0.05K). Higher accuracy ? more nodes ? longer computation times.
8
AtmAbsorption (2)Computation and Memory
Efficiency
Time needed to process 48 profiles with 7
observation angles
Instrument OPTRAN-V7 Adjoint CompactOPTRAN Adjoint OSS Adjoint
AIRS 22m36s 35m12s 3m10s
HIRS 13s 17s 9s
Memory resource required (Megabytes)
Instrument OPTRAN-V7 Double precision CompactOPTRAN Double precision OSS Single precision
AIRS 66 5 97
HIRS 0.5 0.04 4
9
CloudScatter (1)
  • NESDIS/ORA lookup table (Liu et al, 2005).
  • Mass extinction coefficient
  • Single scatter albedo
  • Asymmetry factor
  • Legendre phase coefficients and delta-truncation
    factors for 2-, 4-, 6-, 8-, and 16-streams
  • Analytic phase functions (HG and Rayleigh)
  • Infrared (Intensity only)
  • Spherical particles for liquid water and ice
    cloud (Simmer, 1994)
  • Non-spherical ice cloud (Liou and Yang, 1995
    Macke et al,1997 Baum et al, 2001)
  • Microwave (including polarisation)
  • Spherical particles for rain drops and ice cloud
    (Simmer, 1994)
  • The number of streams is determined using Mie
    size parameter, 2?reff/?

10
CloudScatter (2)
  • ETL library is microwave only, fixed stream (8)
  • Mie spherical scattering model
  • Five hydrometeor phases, exponential size
    distributions
  • Phase functions
  • Currently, Henyey-Greenstein phase function
    matrix.
  • Being extended to incorporate full Mie scattering
    phase functions via an exact Mie library.
  • Currently, no polarisation capability.
  • Scattering matrix Jacobians are analytical.

11
AerosolScatter
  • Currently only handles aerosol absorption.
    Aerosol scattering is planned.
  • Seven aerosol types
  • Dust
  • Sea salt
  • Dry and wet organic carbon
  • Dry and wet black carbon
  • Sulfates
  • Multiple size distribution modes.
  • Uses same scattering structure definition as
    CloudScatter routines

12
SfcOptics
  • Microwave
  • Land (Weng et al, 2001) Snow and sea ice (Yan
    and Weng, 2003)
  • Ocean
  • Wind vector dependent (Liu and Weng, 2003)
  • Wind speed dependent (English, 1998 FASTEM-3)
  • Infrared
  • Land
  • Measurement database for 24 surface types in
    visible and infrared (NPOESS Net heat Flux ATBD,
    2001)
  • Regression methods
  • Retrieval methods
  • Ocean
  • IRSSE (van Delst, 2003). Based on Wu-Smith (1997)
    model.
  • Nick Nalli (NESDIS/ORA) also working on sea
    surface emissivity and reflectivity model.
  • New surface optical models are also being
    developed by other groups (Land data assimilation
    folks)

13
RTSolution (1)
  • SOI, Successive Order of Interaction
    (UWisc-Madison)
  • Truncated doubling technique for layer
    transmission, reflection and source functions.
    Successive order of scattering (SOS) used to
    integrate emission and scattering events from
    surface and atmosphere. IR and ?W. (Heidinger et
    al, 2005)
  • Vector delta 4-stream (UCLA)
  • Delta truncation is applied to reduce phase
    functions to four expansion terms. The optical
    depth and single scattering albedo, as well as
    the expansion coefficients, are rescaled to take
    account of strong forward scattering. The layer
    transmission, reflection, and source functions
    are solved analytically. Adding method is used
    for vertical integration. IR and ?W. (Liou et al,
    2005)

14
RTSolution (2)
  • DOTLRT, Discrete ordinate tangent linear raditive
    transfer (NOAA/ETL)
  • Layer transmission and reflection computed using
    a matrix operator method. Symmetric phase matrix
    is used to simplify matrix manipulation. Layer
    source function is obtained from the transmission
    and reflection. Adding method is used for
    vertical integration. IR and ?W. (Voronovich et
    al, 2004)
  • No polarisation capability.
  • VDISORT (NOAA/NESDIS/ORA)
  • Used for validation.
  • Valid for visible, infrared and microwave
    sensors fully polarimetric (all Stokes vectors).
  • Matrix operator method is used for layer
    transmission, reflection and source functions.
    Vertical integration is performed with linear
    algebra system where continuity at boundaries is
    ensured. (Weng and Liu, 2003)

15
Current Status
  • Currently we are working on the integration of
    the various CRTM components.
  • Goal is to produce a working version of an
    OSS-based CRTM by end of June (!).
  • An OPTRAN-based model is also being worked on for
    migration purposes in the GFS.
  • The development process was deliberately informal
    so there is a bit of integration work still to
    do.
  • Some codes have to be modified from a
    channel-based form (e.g. IRSSE model) to a
    frequency-based form for use with OSS.
  • Other outstanding issues are that some codes
    produce analytic Jacobians rather than coding
    adjoints via the forward ? tangent linear ?
    adjoint ? K-matrix methodology.

16
Jacobians. Analytic or adjoint?
  • Here Im talking about the use of Jacobians in
    NWP. Other applications may have other
    requirements.
  • Analytic Jacobians are generally not suitable for
    variational analysis. This is difficult to prove,
    but experience in NWP has shown this to be the
    case.
  • The Jacobian has to take into account any
    numerical approximations used in the forward
    model, e.g. quadrature, regression fitting,
    interpolations, etc.
  • The Jacobian has to be entirely numerically
    consistent with the forward model.
  • Minimisation algorithms in NWP are sensitive to
    very small inconsistencies or errors.
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