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Table of
Contents | Director's Message | Executive
Summary | CGD Achievements |
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Run Length In Years |
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| Scenario | T85_gx1v3 | T42_gx1v3 | T31_gx3v5 |
| 1990 control | 700 | 1000 | 880 |
| 1% increasing CO2 | 150 | 150 | 180 |
| 2xCO2 | 150 | 150 | 150 |
| 4xCO2 | 150 | 150 | 150 |
| 1870 control | 750 | 300 | 150 |
| 20th century | 100 | 100 | 100 |
| The scenarios are: | |
| 1990 control | constant 1990s forcing |
| 1% increasing CO2 | starting from a 1990 control, applies 1% annual increasing CO2 forcing |
| 2xCO2 | starting from where a 1% increasing CO2 reaches 2 times 1990 levels, CO2 held constant |
| 4xCO2 | starting from where a 1% increasing CO2 reaches 4 times 1990 levels, CO2 held constant at 4x levels |
| 1870 control | constant 1870s forcing |
| 20th century | starting from an 1870 control, a time series of 20th century forcing is applied |
The application of CCSM to IPCC represents a multi-institutional, distributed effort by scientists and software engineers at NCAR, Oak Ridge National Laboratory (ORNL), National Energy Research Supercomputing Center (NERSC), Lawrence Berkeley National Laboratory (LBNL), and partners in the Kyosei Consortium using the Japanese Earth Simulator (ES).
This figure shows IPCC CO2 concentrations. In addition to CO2, the simulations are run with solar, volcanoes, sulfate aerosols, ozone, and other greenhouse gases for the period 1870-2000. A spread of CO2 concentrations for future forcing scenarios is used from years 2000-2200 that also include sulfate aerosols and ozone.
CCSM3 (T85 version) has been run to perform a suite of 20th, 21st, 22nd, and 23rd century climate simulations. These simulations are the CCSM contribution to the IPCC AR4. The experimental design and list of experiments was suggested by IPCC Working Group 1 and coordinated by the World Climate Research Program/Climate Variability and Prediction Program (WCRP/CLIVAR) Working Group on Coupled Models (WGCM).
The IPCC scenarios that are being run can be categorized into two groups: a set of "commitment scenarios" and a number of "science scenarios" that explore alternative future emissions outcomes. The IPCC Special Report on Emissions Scenarios (SRES) that were recommended to the global coupled climate modeling groups by IPCC Working Group 1 include B1 (a low forcing scenario), A1B (a medium forcing scenario), and A2 (a large forcing scenario). The A2, A1B, and B1 scenarios consist of eight-member ensembles run from the year 2000 to the year 2100. Then, commitment scenarios are run with the concentrations of all atmospheric constituents in A1B and B1 held constant at year 2100 values, and the model continues to the year 2200 with five-member ensembles. One of the ensemble members from each is continued for an additional 100 years to the year 2300 with constant year 2100 concentrations. There is also a 20th century commitment scenario that freezes concentrations at levels observed in the year 2000, and the model is run to the year 2100. A limited number of experiments performed on the ES examined the implications of future reductions in CO2 concentrations.
This figure shows the CCSM3 IPCC Run Plan: The IPCC scenario runs have been done at NSF/NCAR (blue), DOE/ORNL (green), and DOE/NERSC (red). Parallel runs on the ES (pink) were made with the scientific and technical assistance of the Kyosei Consortium.
The CCSM3 and Parallel Climate Model (PCM) IPCC runs are being performed at NSF/NCAR, DOE/ORNL, and DOE/NERSC supercomputing sites. An additional set of parallel runs, using the same version of CCSM3 with forcing data sets prepared by NCAR, was run on the ES. Focused model development and significant dedicated computing resources provided by NCAR, DOE, and the Kyosei Consortium have kept the IPCC runs on track for completion in time to meet IPCC data submission and paper publication deadlines. Most recently, NERSC consultants assisted the CCSM team in running the NERSC A2 five-member ensemble as one single 1020 processor massively-parallel run.
The data products from CCSM3 and PCM IPCC simulations will be used for climate change impact studies and as boundary conditions to drive regional scale models. To support NSF and DOE regional modeling efforts, we are outputting two additional sub-daily data streams for each of the CCSM IPCC scenarios. By design, the raw and post-processed data products from the different IPCC scenarios are being kept at DOE and NSF sites where they were computed. This large distributed data set is being made freely available to the U.S. climate research and education community via the DOE Earth System Grid (ESG).
This figure shows CCSM3 DOE/NSF IPCC scenario runs as of October 4, 2004. Observed forcings (solar, volcanoes, greenhouse gases, sulfate aerosols, carbon aerosols, and ozone) are used during the historical period, from years 1870-2000. A variety of future forcing scenarios (20th century freeze, B1, A1B, and A2) are used from years 2000-2200 to simulate the most likely range of future climates. Two of the commitment scenarios (A1B and B1) will be executed out to year 2300.
The IPCC experiments are intended to address several outstanding climate simulation issues. First, how well can the CCSM3 simulate 20th century climate if most of the dominant forcings are included over that time period? In this regard, forcings used previously included natural forcings (solar and volcanoes) and anthropogenic forcings (greenhouse gases, sulfate aerosol direct effect, and ozone). It also included an important new forcing by carbon aerosols, using a present-day distribution of carbon aerosols that scaled the geographical pattern over the 20th century by population as an approximation of their varying effect with time. Future experiments already planned will examine the role of carbon aerosols in much more detail. The 20th century simulations with the CCSM3 show that the time evolution of globally averaged temperatures track the observed time series very well, indicating that the forcings we have included are relevant for simulating 20th century climate.
Second, given three SRES's for 21st century climate change, what possible changes could occur by the end of the 21st century? Results show that the global temperature increases are proportional to the forcing as could be expected, with the pattern of temperature changes showing greatest warming at the high latitudes of the Northern Hemisphere and over land areas, with least warming over the North Atlantic and Southern Oceans.
A third major issue is the nature of climate change that is committed by previous
emissions and by emissions occurring during the 21st century. The analysis is based upon
idealized experiments where all concentrations are held fixed, first at year 2000 values,
and then at year 2100 values for the A1B and B1 scenarios. Results show that global
temperatures continue to rise on the order of a couple of tenths of a degree for the next
100 years after concentrations are fixed, but the much greater commitment comes from sea
level rise. Subsequent sea level increases from thermal expansion alone 100 years after
fixing concentrations are on the order of a couple hundred percent. These results
demonstrate that the threat from future climate change after stabilization comes more from
sea level rise we are already committed to, rather than future increases of temperature.
The CCSM3 experiments for the IPCC AR4 involve the most extensive and highest resolution
multi-member ensemble ever performed with a global coupled climate model at NCAR, with
five-member ensembles for all of the experiments. We also have been coordinating a
parallel set of runs with CCSM3 on the ES. Combining the multi-member ensembles run on the
ES, the CCSM3 will have by far the largest multi-member ensemble data set of any of the
international global coupled models run for the IPCC AR4. Thus, the CCSM3 has assumed a
leadership role in the performance and analysis of these high profile climate change
simulations for the AR4. The model simulations have been completed and a subset of
requested model data is being shipped for archival at DOE's Program for Climate Model
Diagnosis and Intercomparison (PCMDI). This data will become part of the largest
multi-model climate analysis project ever attempted, as over 200 researchers from around
the world have registered to analyze the multi-model data set, of which CCSM3 is a part,
for the IPCC AR4. After the deadline for submission of manuscripts for the Journal of
Climate special issue on CCSM3 in fall 2004, the entire CCSM3 data set will become
available for analysis to the CCSM3 community.
The second phase of the Paleoclimate Modeling Intercomparison Project (PMIP2) is coordinating simulations and data syntheses for the Last Glacial Maximum (LGM, 21,000 years before present) to improve the assessment of climate sensitivity. The important forcing for the LGM is not the direct effect of insolation changes, which are minor, but instead results from the large consequential changes in various elements of the climate system, including greenhouse gases, aerosols, ice sheets, and vegetation change. The changes in greenhouse gases are fairly well known but the others are not. Global climate sensitivity can in principle be estimated from the difference between LGM and present, from Q=a; DT, where Q is the radiative forcing, DT; the global average surface air temperature change, and a; the climate feedback parameter. The climate feedback parameter is related to equilibrium climate sensitivity according to D;T2x=Q2x/a;. While Q and DT;are uncertain, fortunately the signal associated with the changes between LGM and present-day conditions are large.
Using measurements from ice cores, atmospheric CO2 concentrations at the LGM are estimated to be 185 ppmv, approximately 50% of present-day values. Global, annual mean surface temperature simulated by the slab ocean version of the CCSM3 shows a cooling of -2.8°C for LGM CO2 levels and a warming of 2.5°C for a doubling of CO2 (see figure below). Slab and coupled CCSM3 simulations that include the reductions of the other atmospheric trace gases and the large ice sheets covering North America and Eurasia at LGM give cooling in agreement with proxy inferences. The simulations indicate that atmospheric CO2 concentration change explains about half of the global cooling at LGM.
This figure shows global, annual surface temperatures as simulated by slab ocean and
fully-coupled versions of CCSM3 for past and future climate states.
Regional signatures of the climate response to changed LGM forcing are also an
important measure of climate sensitivity and are key for understanding the processes
governing global sensitivity. Patterns and amplitudes of annual surface temperature change
are similar but opposite in sign between the LGM CO2 and 2xCO2 simulations with the
CCSM3 slab ocean model (see figure below, top vs. middle). Cloud feedbacks, particularly
feedbacks involving low clouds, play an important role in determining the surface
temperature response in the model and show comparable patterns of change in the 2xCO2
and LGM CO2 simulations. Additionally, a LGM CCSM3 slab ocean simulation that
includes the reductions of the other atmospheric trace gases and the large northern ice
sheets indicates that the cooling over the oceans in the tropics and Southern Hemisphere
subtropics are primarily (~85%) due to the reductions of atmospheric CO2 (see
figure below, middle vs. bottom). Comparisons of PMIP2 model simulations of surface
temperature changes for these regions and paleoclimatic proxy data may allow the LGM to be
used as a metric to identify estimates of climate sensitivity that are outliers. Other
regions of scalable response will also be identified and quantified as part of the PMIP2
model-data comparisons for the LGM.
This figure shows the surface temperature change simulated by the slab ocean version of
CCSM3 for doubled CO2 compared to present (top), LGM CO2 compared to
present (middle), and Full LGM compared to LGM CO2 (bottom).
The ENSO phenomenon is a natural irregular oscillation of the coupled tropical ocean-atmosphere system on interannual time scales. ENSO is manifest primarily as a warming of the equatorial Pacific Ocean and a redistribution of precipitation within the tropics. However, the effects of ENSO are felt worldwide due to the global atmospheric circulation response to tropical rainfall changes.
This figure shows the variance of monthly SST anomalies from (top) observations during 1900-1999 from the Hadley Centre Sea Ice and SST (HadISST) data sets and (bottom) the T85 CCSM3 control run during model years 400-499.
The ENSO phenomenon in the CCSM3 at T85 resolution exhibits a realistic spatial pattern and amplitude of SST variability in the tropical Pacific and Indian Oceans, with maximum variability in the eastern equatorial Pacific and along the South American coast. This represents a considerable improvement over the previous version of the model (CCSM2), which greatly overestimated the amplitude of the SST variability and its zonal extent (not shown). The T42 version of CCSM3 exhibits a similar pattern and amplitude of SST variability as the T85 version (not shown).
A commonly used index of ENSO is the area-averaged monthly SST anomaly (defined as the departure from the long-term monthly mean) in the equatorial eastern Pacific (5ºN-5ºS, 170ºW-120ºW). A power spectrum of this index shows that the ENSO period in the model is approximately 2 to 3 years (also in the T42 version of CCSM3), considerably shorter than the observed period (approximately 3 to 8 years based on years 1900-1999). The peak amplitude of the power spectrum is comparable in the model and observations.

This figure shows the power spectrum of the monthly equatorial eastern Pacific SST index
from observations during 1900-1999 (black curve) and the T85 CCSM3 control run during
model years 400-499 (red curve).
The spatial distribution of the tropical precipitation changes during
December-February for a composite "warm-minus-cold" ENSO event is shown in the
figure below, where "warm" and "cold" years are identified using a one
standard deviation criterion of the equatorial eastern Pacific SST index. In the model,
warm events are accompanied by rainfall increases in the central and western equatorial
Pacific and decreases directly to the north and south; rainfall decreases are also seen in
the tropical Atlantic and eastern Indian Oceans (a similar pattern and amplitude of
precipitation anomalies is seen in the T42 version of CCSM3; not shown). The simulated
rainfall changes show good overall agreement with the observed changes, although nature
exhibits more pronounced rainfall decreases over the western Pacific and maritime
continent.
This figure shows the warm-minus-cold ENSO composite of precipitation anomalies during
December-February from (top) observations during 1979-2000 based on the Xie-Arkin data set
and (bottom) the T85 CCSM3 control run.
The global atmospheric circulation responds to the redistribution of tropical precipitation during ENSO events via Rossby waves and their interaction with the midlatitude storm tracks. The global sea level pressure (SLP) response to ENSO during December-February is well simulated in the model compared to observations (see figure below). Below normal SLP is found in the eastern tropical Pacific, with above normal SLP in the remaining tropical areas. In the extra tropics, a deepening of the Aleutian Low over the North Pacific is well simulated in the model, with maximum values of approximately 8-10 hPa for the warm-minus-cold ENSO composite. SLP teleconnections to the Southern Hemisphere are also well simulated both in terms of location and amplitude. The T42 version of CCSM3 exhibits a similar SLP response to the T85 version over the tropics, but the amplitude of the Aleutian response is considerably weaker (~5 hPa) than the T85 version (not shown).
This figure shows the warm-minus-cold ENSO composite of sea level pressure anomalies during December-February from (top) observations during 1948-2003 based on the National Centers for Environmental Prediction (NCEP)-NCAR Reanalysis and (bottom) the T85 CCSM3 control run.
The boundary between the late Permian and the Early Triassic at 251 Ma is one of the most remarkable time periods in Earth's history. At this point in time, the largest known extinction of life took place, with approximately 95% of species extinguished. Geologic data indicate this was a time of global warming and very low oxygen levels in the oceans. Jeff Kiehl (CCR) and Christine Shields (CCR) have configured the CCSM3 to simulate the climate of this period. To study ocean conditions at depth, the fully coupled model has to be run for thousands of years for the system to come to a new equilibrium state. The Late Permian simulation is forced with a ten-fold increase in present-day CO2 concentrations. The simulation has been run for over 2000 years, the longest integration of CCSM to date.
This figure shows the time series of the net energy flux at the top of the atmosphere (red) and surface (blue) for the Late Permian simulation. The initial forcing to the system was 14.5 Wm-2 due to a 10x increase in atmospheric CO2.
This figure shows the time series of the global mean annual mean energy flux (Wm-2)
into the oceans.
Given the large heat capacity of the ocean, the long time scale for the model to attain equilibrium is governed by the heat uptake of the oceans as shown in the figure above. Note that around year 1900, the energy flux into the system has reached a very small value (-0.04 Wm-2). This flux of energy is proportional to time rate of change of the volume averaged ocean temperature, shown in the figure below.
This figure shows the time series of the volume averaged ocean temperature (°C) from the Late Permian simulation.
The near equilibrium solution indicates a dramatic decrease in the overturning circulation in the deep ocean. The present-day high latitude pathways of deep water formation, i.e., in the North Atlantic and off the coast of Antarctica, are shut off in the warm climate of the Late Permian. This is the first comprehensive coupled simulation of this time period, and it indicates the need for substantial computational resources to study scientific questions involving deep ocean circulations.
A suite of multi-century fully coupled carbon-climate integrations have been performed using a modified version of the Climate System Model version 1.4 (CSM1.4). Several century-long spin-up runs were done to adjust the modeled carbon cycle incrementally to the coupled model climate. These spin-up runs led to a stable multi-century (1000 years) carbon-climate pre-industrial control run.
Additionally, multiple 180-year historical and 100-year future scenario fossil fuel emissions experiments have been completed. These experiments are being analyzed to understand connections and feedbacks between the carbon cycle and the physical climate.
This figure shows the CSM1.0 simulation of atmospheric carbon dioxide in peta grams of
carbon from the pre-industrial to future climate using the SRES A2 scenario. This
simulation includes both ocean and terrestrial carbon response to climate and changes in
carbon dioxide.
The CCSM project will continue to follow a research and development program to enhance the capabilities of the modeling system. The research will be directed toward providing a more complete, more useful, and more accurate CCSM. Representations of new physical and chemical processes will be formulated and tested within the CCSM framework to make the modeling system closer to what is termed an earth system model. Development will take place to provide increased resolution of climate change projections for impact assessment. As well, increased emphasis will be placed on improving the simulations of the hydrological cycle on continents. Software development will be directed to make the modeling system more portable, more reliable, and easier to use. Considerable effort will be put toward making the modeling system more accurate through a concerted attack on the long standing biases and continued examination of the fidelity of the representations of the physical and dynamical processes of the basic components of the model, atmosphere, ocean, ice, and land.
The recently released version of the model, CCSM3, will be used to tackle a large number of interesting scientific questions. One of the most interesting questions has to do with the physical processes that can lead to abrupt climate change (ACC). In general, climate change is viewed as a gradual process taking place over centuries or millennia. However, observations of past climates indicate that large changes can occur over a few decades. There are hypotheses about physical processes involving ice, air, and ocean interaction particularly in the North Atlantic that, when perturbed, appear to have the potential to lead to rapid changes as a new equilibrium is sought by the climate system. CCSM3 will be used to investigate these physical mechanisms from a basic science point of view. The ad hoc CCSM group for ACC will also attempt to reproduce the characteristics of periods of ACC that have been observed in the paleoclimate record.
CCSM3 will be used to address a rather important question about the effects of human-induced land-use change on climate. Most people think of the emission of greenhouse gases as the substance of human effects on climate. However, in the past 150 years human activity has transformed the land surface. For example, farms have replaced forests in most of the eastern half of the U.S. and southern Canada. There is instrumental evidence of the changes in local climates produced by changes in land use. It is important to address the question of the impact on the climate on at least the continental scale by land-use changes in the 19th and 20th centuries.
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