Model Information of Potential Use to the IPCC Lead Authors and the AR4.
CCSM3
31 January 2005
I. Model identity:
A. Institution, sponsoring agency, country
National Center for Atmospheric Research (NCAR),
NSF (a primary sponsor), DOE (a primary sponsor), NASA, and NOAA
USA
B. Model name (and names of component atmospheric, ocean, sea ice,
etc. models)
Coupled model - Community Climate System Model, version 3.0 (CCSM3)
Atmosphere - Community Atmosphere Model, version 3.0 (CAM3)
Ocean - Parallel Ocean Program,
version 1.4.3 (POP 1.4.3)
Sea ice - Community Sea Ice Model, version
5.0 (CSIM5)
Land - Community Land
Model, version 3.0 (CLM3)
C. Vintage (i.e., year that model version was first used in a
published application)
6irst control runs and IPCC runs were run and submitted for
publication in 2004. First publication containing CCSM3 results
will appear in 2005.
D. General published references and web pages
Main website - http://www.ccsm.ucar.edu
Publications submitted to a special issue of the Journal of Climate describing
CCSM3 are available from http://www.ccsm.ucar.edu/publications/jclim04/Papers_JCL04.html
E. References that document changes over the last ~5 years (i.e.,
since the IPCC TAR) in the coupled model or its
components. We
are specifically looking for references that document changes in
some aspect(s) of model performance.
There are a series of NCAR technical reports available from
http://www.ucar.edu/communications/technotes/technotes401-.shtml
TN-455+STR The Sea Ice Simulation of the Community System Model, Version
Two, B.P. Briegleb, E.C. Hunke, C.M. Bitz, W.H. Lipscomb, M.M. Holland, J.L
Schramm, and R.E. Moritz, CGD. 38 pp. January 2004. NTIS #PB2004-105849.
TN-461+STR Technical Description of the Community Land Model (CLM), Keith
W. Oleson, Yongjiu Dai, Gordon Bonan, Mike Bosilovich, Robert Dickinson, Paul
Dirmeyer, Forrest Hoffman, Paul Houser, Samuel Levis, Guo-Yue Niu, Peter
Thornton, Mariana Vertenstein, Zong-Liang Yang, Xubin Zeng, CGD. 183 pp. May
2004, NTIS #PB2004-105836.
TN-463+STR Scientific Description of the Sea Ice Component in the
Community Climate System Model, Version Three, B.P. Briegleb, C.M. Bitz, E.C.
Hunke, W.H. Lipscomb, M.M. Holland, J.L. Schramm, and R.E. Moritz, CGD, 75
pp. June 2004, NTIS #PB2004-106574.
TN-464+STR Description of the NCAR Community Atmosphere Model (CAM
3.0), W.D. Collins, P.J. Rasch, B.A. Boville, J.R. McCaa,
D.L. Williamson, J.T. Kiehl, B. Briegleb, C. Bitz, S.-J. Lin,
M. Zhang, and Y. Dai, CGD, 214 pp. June 2004.
LANL technical reports:
Smith, R. D. and P. R. Gent, 2002: Reference manual for the Parallel Ocean
Program (POP), ocean component of the Community Climate System
Model (CCSM2.0 and 3.0). Technical Report LA-UR-02-2484, Los Alamos
National Laboratory, available online at
http://www.ccsm.ucar.edu/models/ccsm3.0/pop.
Refereed papers (partial list):
Bonan, G. B., K. W. Oleson, M. Vertenstein, S. Levis, X. Zeng, Y. Dai,
R. E. Dickinson and Z.-L. Yang, 2002: The land surface climatology
of the Community Land Model coupled to the NCAR Community
Climate Model. J. Clim., 15, 3123-3149.
Bonan, G. B., S. Levis, L. Kergoat, and K. W. Oleson, 2001: Landscapes as
patches of plant functional types: An integrating approach for climate
and
ecosystem models. Glob. Biogeochem. Cycles, 16, 5.1-5.23.
Boville, B. A. and C. S. Bretherton, 2003: Heating and dissipation in the
NCAR Community Atmosphere Model. J. Clim., 16, 3877-3887.
Collins, W. D., 2001: Parameterization of generalized cloud overlap for
radiative calculations in general circulation models. J. Atmos. Sci.,
58, 3224-3242.
Collins, W. D., J. K. Hackney, and D. P. Edwards, 2002: A new
parameterization for infrared emission and absorption by water vapor in
the
National Center for Atmospheric Research Community Atmosphere
Model. J. Geophys. Res., 107, 8028, doi:10.1029/2000JD000032.
Connolley, W. M., J. M. Gregory, E. C. Hunke, and A. J. McLaren, 2004: On the
consistent scaling of terms in the sea ice dynamics equation. J. Phys.
Oceanogr., 1776-1780.
Kiehl, J. T. and P. R. Gent, 2004: The Community Climate System Model,
Version Two. J. Clim., 17, 3666-3682.
Libscomb, W. H. and E. C. Hunke, 2004: Modeling sea-ice transport using
incremental remapping. Mon. Wea. Rev., 132, 1341-1354.
Ohlmann, J. C., 2004: Ocean radiant heating in climate models.
J. Clim., 16, 1337-1351.
Williamson, D. L., 2002: Time-split versus process-split coupling of
parameterizations and dynamical core. Mon. Wea. Rev., 130, 2024-2041.
Zhang, M., W. Lin, C. B. Bretherton, J. J. Hack, and P. J. Rasch, 2003:
A modified formulation of fractional stratiform condensation rate
in the NCAR Community Atmosphere Model (CAM2). J. Geophys. Res.,
108, 4035, doi:10.1029/2002JD002523.
F. IPCC model version's global climate sensitivity (KW-1m2) to
increase in CO2 and how it was determined (slab ocean expt.,
transient expt--Gregory method, =B12K Cess expt., etc.)
2.7 K / (3.5 W/m^2), from a slab ocean experiment
G. Contacts (name and email addresses), as appropriate, for:
1. coupled model
William Collins, wcollins@ucar.edu
2. atmosphere
Philip Rasch, pjr@ucar.edu
3. ocean
Bill Large: wily@ucar.edu
4. sea ice
Marika Holland, mholland@ucar.edu
5. land surface
Gordon Bonan, bonan@ucar.edu
6. vegetation
Gordon Bonan, bonan@ucar.edu
7. other?
IPCC runs: Jerry Meehl, meehl@ucar.edu
II. Besides atmosphere, ocean, sea ice, and prescription of
land/vegetated surface, what can be included (interactively) and was
it active in the model version that produced output stored in the
PCMDI database?
A. atmospheric chemistry?
Qualified yes: two processes are active:
(1. Modification to GHG concentrations by chemical processes; and
(2. Conversion of SO2 and DMS to sulfate aerosols (the sulfur cycle).
B. interactive biogeochemistry?
No
C. what aerosols and are indirect effects modeled?
No indirect forcing effects are included.
The semi-direct effect (reduction in cloud amount by aerosol heating) is
included.
Aerosol species included:
(1. Sulfates
(2. Black and organic carbon
(3. Sea salt
(4. Soil dust
(5. Stratospheric volcanic aerosols
D. dynamic vegetation?
No
E. ice-sheets?
No (glaciers are specified, but there are no dynamic ice sheets)
III. List the community based projects (e.g., AMIP, C4MIP, PMIP,
PILPS, etc.) that your modeling group has participated in and indicate
if your model results from each project should carry over to the
current (IPCC) version of your model in the PCMDI database.
AOMIP -- no
Global Land-Atmosphere Coupling Experiment (GLACE): yes
AMIP: no
AMIP2: no
CMIP: no
C4MIP: possibly yes
IV. Component model characteristics (of current IPCC model version):
A. Atmosphere
1. resolution
Lateral resolution from 85-wavenumber triangular spectral truncation
of the dynamics. At the equator, the spatial resolution is
approximately 1.4 degrees.
2. numerical scheme/grid (advective and
time-stepping schemes;
model top; vertical coordinate and number of layers above 200 hPa
and below 850 hPa)
Numerical scheme - Eulerian spectral transform,
with semi-Lagrangian tracer transport
Grid - T85
Time stepping - semi-implicit leapfrog
Model top - 2.2 hPa
Vertical coordinate - generalized terrain-following hybrid coordinate,
26 levels
Number of layers above 200 hPa - 13
Number of layers below 850 hPa - 4
3. list of prognostic variables (be sure
to include, as
appropriate, liquid water, chemical species, ice, etc.)
a. Vorticity
b. Divergence
c. Temperature
d. Specific humidity
e. Surface pressure
f. Grid box averaged liquid condensate
amount
g. Grid box averaged ice condensate
amount
h. Nitrous
Oxide
i.
Methane
j.
CFC11
k.
CFC12
l.
SO2
m.
SO4
n.
DMS
o.
H2O2
4. name, terse descriptions, and
references (journal articles,
web pages) for all major parameterizations. Include, as
appropriate, descriptions of:
a. clouds
Prognostic cloud condensate with diagnotic cloud amount
Rasch, P. J., and J. E. Kristjansson, A comparison of the CCM3 model
climate using diagnosed and predicted condensate parameterizations,
J. Climate, 11, 1587-1614, 1998.
Zhang, M., W. Lin, C. S. Bretherton, J. J. Hack, and P. J. Rasch, A modified
formulation of fractional stratiform condensation rate in the NCAR
community atmospheric model CAM2, J. Geophys. Res., 108
(D1), 2003.
Boville, B. A., P. J. Rasch, J. J. Hack, and J. R. McCaa, 2005: Representation
of clouds and precipitation processes in the Community Atmosphere Model
(CAM3). J. Clim., submitted.
b. convection
Deep convection:
Zhang, G. J., and N. A. McFarlane, Sensitivity of climate simulations to the
parameterization of cumulus convection in the Canadian Climate Centre
general circulation model, Atmosphere-Ocean, 33, 407-446, 1995.
Shallow convection:
Hack, J. J., Parameterization of moist convection in the National Center
for Atmospheric Research Community Climate Model (CCM2),
J. Geophys. Res., 99, 5551-5568, 1994.
c. boundary layer
Non-local atmospheric bounday layer scheme
Holtslag, A. A. M., and B. A. Boville, Local versus nonlocal boundary-layer
diffusion in a global climate model, J. Climate, 6, 1825-1842,
1993.
Boville, B. A., and C. S. Bretherton, Heating and dissipation in the NCAR
community atmosphere model, J. Climate, 16, 3877-3887, 2003.
d. SW, LW
radiation
LW: absorptivity-emissivity method for clear-skies, plus Truncated
Independent Column Approximation (TICA) for all-sky
SW: delta-Eddington with exponential-sum fit representation of
near-IR, truncated ICA (TICA) for all-sky
pre-CCSM3: Kiehl, J. T., J. J. Hack, G. B. Bonan, B. B. Boville, D. L.
Williamson, and
P. J. Rasch, The National Center for Atmospheric Research Community
Climate Model: CCM3, J. Climate, 11, 1131-1149, 1998.
Subsequent improvements:
Collins, W. D., Parameterization of generalized cloud overlap for radiative
calculations in general circulation models, J. Atmos. Sci., 58,
3224-3242, 2001.
Collins, W. D., J. K. Hackney, and D. P. Edwards, A new parameterization for
infrared emission and absorption by water vapor in the National Center
for Atmospheric Research Community Atmosphere Model,
J. Geophys. Res., 107 (D22), 2002.
e. any special
handling of wind and temperature at top of model
Horizontal diffusion of temperature and wind with a del-squared
diffusion operator is introduced in the top three layers of the
model.
B. Ocean
1. resolution
nominal 1 degree displaced pole horizontal grid
320x384 horizontal grid points
40 vertical levels
1.125degx0.27deg resolution on the equator
northern pole in Greenland
2. numerical scheme/grid, including
advection scheme, time-stepping scheme, vertical coordinate,
free surface or rigid lid, virtual salt flux or freshwater flux
third-order upwinding advection
3-time-level second-order modified leapfrog time stepping
40-level geopotential grid extending to 5500m, with resolution increasing
from 10m
at the surface to 250m in the deep ocean.
implicit free surface
virtual salt flux
3. list of prognostic variables and
tracers
grid-oriented zonal and meridional velocity components
vertical velocity
pressure
density
potential temperature
salinity
ideal age
cfc's (included in some integrations, but not all)
4. name, terse descriptions, and
references (journal articles, web pages) for all parameterizations.
Include, as appropriate, descriptions of:
Scientific description of POP ocean model available for download
at:
http://www.ccsm.ucar.edu/models/ccsm3.0/pop/
a. eddy
parameterization
Gent-McWilliams
Gent, P.R. and J.C. McWilliams, 1990: Isopycnal mixing in ocean
circulation models. J. Phys. Oceanogr., 20, 150-155.
aa. horizontal viscosity
anisotropic with Smagorinsky-type coefficients
Large, W.G., G. Danabasoglu, J.C. McWilliams, P.R. Gent, and
F.O. Bryan, 2001: Equatorial circulation of a global ocean
climate model with anisotropic horizontal viscosity. J. Phys.
Oceanogr., 31, 518-536.
Smith, R. and J.C. McWilliams, 2003: Anisotropic horizontal
viscosity for ocean models. Ocean Modelling, 5, 129-156.
b. bottom boundary
layer treatment and/or sill overflow treatment
None
c. mixed-layer
treatment
KPP boundary layer mixing with modifications as described in Danabasoglu et al.
Large, W.G., J.C. McWilliams and S.C. Doney, 1994: Oceanic vertical
mixing:
A review and a model with a nonlocal boundary layer parameterization,
Reviews of Geophysics, 32, 363-403.
Danabasoglu, G., W.G. Large, J.J. Tribbia, P.R. Gent, and B.P. Briegleb,
2005: Diurnal Ocean-Atmosphere Coupling, J. Climate, submitted.
d. sunlight
penetration
shortwave penetration based on observed monthly chlorophyll distribution and
parameterization developed by Carter Ohlmann.
Ohlmann, J.C., 2003: Ocean radiant heating in climate models, J. Climate,
16, 1337-1351.
Danabasoglu, G., W.G. Large, J.J. Tribbia, P.R. Gent, and B.P. Briegleb,
2005: Diurnal Ocean-Atmosphere Coupling, J. Climate, submitted.
e. tidal mixing
None
f. river mouth mixing
river runoff implemented as a surface freshwater flux, spread over active ocean
grid
points nearest the river mouth, with a falloff distance roughly compatible with
observed sea surface salinity distributions.
g. mixing isolated
seas with the ocean
A pointwise freshwater balance in isolated seas diverts any excess/deficit
freshwater flux to nearby active ocean regions as a surface flux.
h. treatment of
North Pole "singularity" (filtering, pole rotation, artificial
island?)
Northern grid pole displaced into Greenland to ~(80N,40W).
Timestep is small enough so that no filtering is necessary.
C. sea ice
Complete documentation available from:
http://www.ccsm.ucar.edu/models/ccsm3.0/csim/
1. horizontal resolution, number of layers, number of thickness
categories
gx1v3 grid (nominally 1 degree, displaced pole grid. see ocean
resolution)
number of layers - 4 layers in ice + a single snow layer
number of thickness categories - 5 ice plus one open water
category
2. numerical scheme/grid, including advection scheme, time-stepping
scheme,
advection scheme - incremental remapping (Lipscomb and Hunke, Mon Wea.
Rev, 132,
1341-1354, 2004)
ITD solved using linear remapping (Lipscomb, 2001)
vertical heat equation solved using an implicit backwards-Euler
space-centered
scheme
3. list of prognostic variables
for each gridcell : sea ice velocity; stress tensor
components (not resolved
across the thickness
distribution)
for each gridcell and each ice category: sea ice
concentration, sea ice volume,
snow volume, surface
temperature
for each ice category and each ice level: sea ice internal
energy
4. completeness (dynamics? rheology? leads? snow treatment on sea
ice)
dynamics - elastic-viscous-plastic (Hunke and Dukowicz,
1997) with
updates (Hunke, 2001; Hunke and Dukowicz,
2002; Hunke and Dukowicz, 2003)
thermodynamics - Bitz and Lipscomb (1999)
ITD present with linear remapping (see Bitz et al., 2001;
Lipscomb, 2001)
snow treated as a single layer
lateral melting following Steele (1992)
5. treatment of salinity in ice
salinity fixed at constant 4ppt for ice/ocean exchange
salinity profile used for thermodynamic considerations
(see Bitz and Lipscomb, 1999)
6. brine rejection treatment
brine rejection based on constant 4ppt salinity in the
sea ice
7. treatment of the North Pole "singularity" (filtering,
pole rotation, artificial island?)
pole is rotated into Greenland
D. land / ice sheets (some of the following may be omitted if
information is clearly included in cited references.
An extensive technical description of the Community Land Model (CLM) can be
found in:
Oleson, K.W. et al. 2004: Technical description of the Community Land Model
(CLM),
NCAR Technical Note NCAR/TN-461+STR, National Center for Atmospheric Research,
Boulder,
Colorado, 173 pp.
1. resolution (tiling?), number of layers
for heat and water
Spatial land surface heterogeneity is represented as a nested subgrid hierarchy
in which
grid cells are composed of multiple landunits, snow/soil columns, and plant
functional
types (PFTs). The specific landunits are glacier, lake, wetland, vegetation
The vegetation portion is divided into patches of up to 4 of 16 PFTs
types. All PFTs in a grid cell share a single soil column. Plant functional
types and
leaf area index are specified from satelllite data.
Soil water is predicted from a ten-layer model, in which the vertical
soil moisture transport is governed by infiltration, surface and
sub-surface runoff, gradient diffusion, gravity, and root extraction
through canopy transpiration. Soil temperature is predicted from the
same ten-layer model accounting for phase change.
2. treatment of frozen soil and permafrost
Explicit treatment of ice and liquid water in soil column.
3. treatment of surface runoff and river
routing scheme
A conceptual form of TOPMODEL (Beven and Kirkby [1979]) is used to parameterize
runoff. The River Transport Model (RTM) of Branstetter [2001], and
Branstetter and Famiglietti [1999] is used to transport runoff from the land to
the ocean
Beven, K.J., and Kirkby, M.J. 1979. A physically based variable contributing
area model of basin hydrology. Hydrol. Sci. Bull. 24: 43-69.
Branstetter, M.L. 2001. Development of a parallel river transport algorithm and
applications to climate studies. Ph.D. dissertation, University of Texas at Austin.
Branstetter, M.L., and Famiglietti, J.S. 1999. Testing the sensitivity of
GCM-simulated runoff to climate model resolution using a parallel river
transport
algorithm. Preprints, 14th Conference on Hydrology, Dallas, TX, Amer. Meteor.
Soc.,
391-392.
4. treatment of snow cover on land
Snow is modeled with up to five layers depending on total snow depth accounting
for ice and liquid water contents in each layer and liquid water movement
between
layers.
5. description of water storage model and
drainage
Water is stored on land in the soil column, in wetlands, lakes and glaciers,
and in snow. However, the areal extent of wetlands, lakes, and glaciers is
constant in
time. Runoff from land (surface runoff, sub-surface drainage) is routed to
the river transport model as is runoff from wetlands, lakes, and glaciers, the
latter
being determined from the mass balance residual. All of this water is then
distributed to the oceans based on the routing scheme.
6. surface albedo scheme
Radiative transfer within vegetative canopies is calculated from the two-stream
approximation.
Soil albedos are determined from soil color.
7. vegetation treatment (canopy?)
Vegetated surfaces are comprised of up to 4 of 16 possible plant functional
types (PFTs). These
PFTs differ in physiological and morphological traits along with climatic
preferences.
Sensible and latent heat fluxes from vegetated surfaces are derived from Monin-Obukhov
similarity theory applied to the surface layer. Transpiration fluxes are
predicted using
a coupled canopy conductance-photosynthesis scheme.
8. list of prognostic variables
Multi-layer SNOW (up to five layers depending on total snow depth)
number of snow layers
thickness of snow layer (m)
depth of snow layer interface (m)
node depth of snow layer (midpoint) (m)
liquid water content of snow layer (kg m-2)
ice content of snow layer (kg m-2)
total snow depth (m)
total snow water equivalent (kg m-2)
snow age (influences snow albedo)
snow layer temperature (K)
Ten-layer SOIL
soil liquid water content (kg m-2)
soil ice content (kg m-2)
soil temperature (K)
Vegetation temperature (K)
Ground temperature (K)
Canopy water (kg m-2)
9. ice sheet characteristics (How are snow
cover, ice melting, ice accumulation, ice dynamics handled? How are the
heat and water fluxes handled when the ice sheet is melting?)
Glaciers are generally initialized as a column of pure ice with a depth equal
to the soil
column depth and a snow pack of 1000 kg/m2 snow water equivalent . Snow may
melt or accumulate
but the snow is constrained to have a snow water equivalent of less than 1000
kg/m2. Glacier
dynamics such as ice calving are not modeled.
E. coupling details
1. frequency of coupling
ocean coupled once per day, atm/lnd/ice coupled once per hour
2. Are heat and water conserved by
coupling scheme?
yes
3. list of variables passed between
components:
a. atmosphere -
ocean
b. atmosphere -
land
c. land - ocean
d. sea ice - ocean
e. sea ice -
atmosphere
------------------------------------------------------------------------------
Atmosphere Model - Data recieved (* -> used for diagnostic purposes only)
states
o 2 meter reference air temperature* (merged lnd/ice/ocn)
o 2 meter reference specific humidity* (merged lnd/ice/ocn)
o albedo: visible
direct
(merged lnd/ice/ocn)
o albedo: near-infrared
direct (merged lnd/ice/ocn)
o albedo: visible
diffuse
(merged lnd/ice/ocn)
o albedo: near-infrared diffuse
(merged lnd/ice/ocn)
o surface
temperature
(merged lnd/ice/ocn)
o ocn sea surface temperature
o land snow
height
o ice fraction
o ocean fraction
o land fraction
fluxes
o zonal surface
stress
(merged lnd/ice/ocn)
o meridional surface
stress
(merged lnd/ice/ocn)
o latent
heat
(merged lnd/ice/ocn)
o sensible
heat
(merged lnd/ice/ocn)
o longwave radiation
upward
(merged lnd/ice/ocn)
o
evaporation
(merged lnd/ice/ocn)
------------------------------------------------------------------------------
Ice Model - Data received
states
o ocn: temperature
o ocn: salinity
o ocn: zonal velocity
o ocn: meridional velocity
o ocn: dh/dx: zonal surface slope
o ocn: dh/dy: meridional surface slope
o atm: layer height
o atm: zonal velocity
o atm: meridional velocity
o atm: potential temperature
o atm: temperature
o atm: specific humidity
o atm: density
fluxes
o ocn: : heat of fusion or : melting potential
o atm: shortwave radiation: downward visible direct
o atm: shortwave radiation: downward near-infrared direct
o atm: shortwave radiation: downward visible diffuse
o atm: shortwave radiation: downward near-infrared diffuse
o atm: longwave radiation downward
o atm: precipitation: liquid
o atm: precipitation: frozen
------------------------------------------------------------------------------
Land Model - Data received
states
o atm layer height
o atm zonal velocity
o atm meridional velocity
o atm potential temperature
o atm specific humidity
o atm pressure
o atm temperature
fluxes
o atm precipitation: liquid convective
o atm precipitation: liquid large-scale
o atm precipitation: frozen convective
o atm precipitation: frozen large-scale
o atm longwave radiation downward
o atm shortwave radiation: downward visible direct
o atm shortwave radiation: downward near-infrared direct
o atm shortwave radiation: downward visible diffuse
o atm shortwave radiation: downward near-infrared diffuse
------------------------------------------------------------------------------
Ocean Model - Data received
states
o atm equivalent sea level pressure (only used for BGC work, non-IPCC?)
o atm 10m wind speed squared
(only used for BGC work, non-IPCC?)
o ice fraction
fluxes
o atm shortwave radiation net
o atm latent heat
o atm sensible heat
o atm longwave radiation upward
o atm longwave radiation downward
o atm precipitation: rain
o atm precipitation: snow
o atm+ice zonal surface
stress (merged over
one grid cell)
o atm+ice meridional surface stress (merged over
one grid cell)
o atm evaporation
o ice ocean heat (melting potential) used for melting
o ice salt flux
o ice melt water
o lnd coastal runoff
4. Flux adjustment? (heat?, water?,
momentum?, annual?,
monthly?).
none
VI. Simulation Details (report separately for each IPCC simulation contributed
to database at PCMDI):
A. IPCC "experiment" name
See the excel chart with the "Local
Abbrev" column that I mailed you last week
B. Describe method used to obtain initial conditions for each
component model
1. If initialized from a control run, which
month/year.
2. For control runs, describe spin-up
procedure.
See the excel chart with the "Local
Abbrev" column that I mailed you last week
C. For pre-industrial and present-day control runs, describe
radiative forcing agents (e.g., non-anthropogenic aerosols, solar variability)
present=2E Provide references or web pages containing further information
as to the distribution and temporal changes in these agents.
Still working on this...
D. For perturbation runs, describe radiative forcing agents (e.g.,
which greenhouse gases, which aerosols, ozone, land surface changes, etc.)
present. Provide references or web pages containing further information
as to the distribution and temporal changes in these agents.
Still working on this