|
Simulations used for the U.S.
National Assessment
1. CGCM1
Canadian Centre for Climate Modelling and Analysis (CCCma):
First generation Coupled General Circulation Model (CGCM1)
Simulations:
3 ensemble (ensembles have different initial conditions but similar
boundary conditions) runs from 1850 - 2100 using:
- 1% equivalent CO2 increase per year +
sulfate aerosols (IS92a): Core scenario for the National
Assessment is GHG+A Ensemble # 1. Daily and monthly
0.5o gridded time series available for the U. S. from VEMAP.
Optional additional scenarios for the National
Assessment (1 run each).
time series: 1850, scenarios start 1990
2.
HADCM2
United Kingdom Meteorological Office/ Hadley Centre
for Climate Prediction and Research: HADCM2
Simulations:
4 ensemble runs from 1860 - 2099 (scenarios start 1990) using
Optional additional scenarios for the National Assessment (4 ensembles
each).
1 control simulation
time series: 1860, scenarios start 1990
3. ECHAM4/OPYC3
4. NCAR
CSM (Climate System Model)
These scenarios (1 run each) are run from 1980-2100,
and they don't start diverging until after 2010. NCAR also has run a
20th century scenario (from 1870-1998) and an unforced control, but these
simulations are not publicly available.
GFDL
DOE PCM
(Department of Energy Parallel Climate Model, at NCAR)
|
|
CGCM1 |
HADCM2 |
ECHAM4/OPYC3 |
GFDL |
NCAR
CSM |
DOE PCM |
HADCM3 |
|
Atmosphere |
3.75o x 3.75o/10
T32 |
2.5o x 3.75o/19
grid |
2.8o x 2.8o/19
T42 |
3.75o x 2.25o/14
R30 |
2.8o x 2.8o/18 T42 |
2.8o x 2.8o/18 T42 |
2.5o x 3.75o/19
grid |
|
Land |
modified bucket |
canopy processes and stomatal resistance included |
canopy processes and stomatal resistance included |
bucket |
canopy processes and stomatal resistance
included |
canopy processes and stomatal resistance included |
canopy processes, stomatal resistance, and CO2
processes included (MOSES) |
|
Ocean |
1.8o x 1.8o
/29
Based on GFDL MOM 1.1 |
2.5o x 3.75o/20 |
2.8o x 2.8o/9 |
1.875o x 2.25o /18
GFDL MOM 1.1 |
2.4o x 1.2o(VAR)/45 |
0.66o x 0.66o (VAR)/32 |
1.25o x 1.25o/20 |
|
Sea Ice |
Thermodynamic only |
Dynamic and Thermodynamic |
Dynamic and Thermodynamic |
Dynamic and Thermodynamic |
Dynamic and Thermodynamic |
Dynamic and Thermodynamic |
Dynamic and Thermodynamic |
|
Coupler |
flux-adjusted |
flux-adjusted |
flux-adjusted |
flux-adjusted |
not flux-adjusted |
not flux-adjusted |
not flux-adjusted |
|
Multiple Greenhouse Gases |
no |
no |
no |
no |
yes |
yes |
yes |
|
Sulfate Chemistry Model |
no |
no |
no |
no |
yes |
no |
yes |
|
Sensitivity |
3.5o C |
2.6o C |
2.6o C |
3.4o C |
2.0o C |
2.0o C |
3.3o C |

Emission Scenarios

Figure
1a: The 1% equivalent CO2 increase per year case is
scenario IS92a before present and 1% per year compounded increase of CO2
into the future. Equivalent CO2 is a way of increasing
the CO2 concentration to account for the radiative effects of
the other greenhouse gases (N2O, CH4, O3,
Halogenated compounds). The figure shows IS92a for CO2
alone (red) and equivalent CO2 (black). The CO2
concentration by 2100 is about 700 ppmv, but increases to about 1050 ppmv
when the effects of the other greenhouse gases are included. The 1%
increase per year scenario (blue) leads to a slightly larger increase than
the IS92a equivalent CO2 scenario, resulting in around 1250
ppmv by 2100. The 0.5% equivalent CO2 increase per year
case is actually just IS92d. The CO2 alone concentration
for IS92d (light blue) results in 540 ppmv by 2100, whereas the equivalent
CO2 (green) case actually used in the scenarios results in 730
ppmv CO2 by 2100. These concentrations were calculated
from the radiative forcings developed for IPCC from upwelling diffusion
energy balance models (T. Wigley, personal communication), using the
radiative forcing functions in IPCC Technical Paper II (Houghton
et al., 1997).
Figure
1b: Radiative forcing used to derive the concentrations in
Figure 1a.
Figure
1c: The IS92a and IS92d total sulfate emissions scenarios.
Only direct effects of sulfate aerosols have been considered in these
scenarios. These emissions were calculated from the radiative
forcings developed for IPCC from upwelling diffusion energy balance models
(T. Wigley, personal communication) , using the radiative forcing
functions in IPCC Technical Paper II (Houghton et al.,
1997). The HADCM2 experiments used these emission values (TgS =
teragrams of sulphur) in the form of surface albedos.
Figure
2a: The actual equivalent CO2 concentration used in
the HADCM2 experiments. The values from the historical period are
based on the IPCC estimated greenhouse gas forcings from 1765-1990 (Shine
et al., 1990, Table 2.6; Mitchell and Johns, 1997),
calculated as equivalent CO2. After 1990, CO2
is increased at the rate of 1%/year.
Fig ure
2b: Equivalent CO2 radiative forcings computed from
the HADCM2 GCM.
Figure
2c: SO4 (total) radiative forcings
computed from the HADCM2 GCM (note that actual emission values were not
used in HADCM2, which does not have a sulfate chemistry model). The
values from the historical period are scaled from present-day values to
correspond with historical estimates (Mitchell and
Johns, 1997). Present and future sulfate loadings were derived
using the sulfur cycle model of Langner and Rodhe
(1991) and IS92a estimates for the future (Mitchell
and Johns, 1997).
For a complete description of the NCAR CSM forcing
scenarios, go to NCAR
CSM.
Note: The CGCM1 experiments used the same
forcing as the HADCM2 experiments (for the 1% case).
References
Houghton,
J. T., Filho, L. G. M., Griggs, D. J., and K. Maskell, Eds., 1997, An
introduction to simple climate models used in the IPCC second assessment
report, IPCC, 47 pp.
Langner,
J. and H. Rodhe, 1991, "A global three-dimensional model of the
tropospheric sulfur cycle", J. Atmos. Chem., 13, 225-263.
Mitchell,
J. F. B. and T. C. Johns, 1997, "On modification of global warming by
sulfate aerosols", J. Climate, 10(2): 245-267.
Shine, K.
P. , Derwent, R. G., Wuebbles, D. J., and J. J. Morcrette, 1990, "Radiative
forcing of climate", Climate Change. The IPCC Scientific
Assessment, J. T. Houghton, G. J. Jenkins, and J. J. Ephraums, Eds.,
Cambridge University Press, 41-68.
|