Global climate model

A general circulation model (GCM) aims to describe geophysical flow by integrating a variety of fluid-dynamical, chemical, or even biological equations that are either derived directly from physical laws (e.g. Newton's law) or constructed by more empirical means. There are both atmospheric GCMs (AGCMs) and ocean GCMs (OGCMs). When coupled together (along with other components such as a sea ice model and a land model) an ocean-atmosphere coupled general circulation model (AOGCM) forms the basis for a full climate model.

A recent trend in GCMs is to extend them to become Earth system models, that would include such things as submodels for economic growth and its effect on carbon dioxide emissions.

Nevertheless, for over a decade the major climate prediction uncertainties have not been reduced at all. Progress has been made, but additional uncertainties and unknowns have been found. There also are so many adjustables in the models, and there is a limited amount of observational data, so the models can always be brought into agreement with the data. [1] (http://www.sciencemag.org/cgi/content/summary/292/5515/192)

Note that many simpler levels of climate model exist; some are of only heuristic interest; others continue to be scientifically relevant.

Contents

Structure

Three (or more properly, four) dimensional GCMs discretise the equations for fluid motion and integrate these forward in time. They also contain parametrisations for processes - such as convection - that occur on scales too small to be resolved directly. More sophisticated models may include representations of the carbon and other cycles.

A simple general circulation model (SGCM), a minimal GCM, consists of a dynamical core, for example the primitive equations, energy input into the model, and energy dissipation in the form of scale-dependent friction, so that atmospheric waves with the highest wavenumbers are the ones most strongly attenuated. Such models may be used to study atmospheric processes within a simplified framework but are not suitable for future climate projections.

Atmospheric GCMs (AGCMs) model the atmosphere (and typically contain a land-surface model as well) and impose sea surface temperatures. A large amount of information including model documentation is available from AMIP [2] (http://www-pcmdi.llnl.gov/amip/). They may include atmospheric chemistry.

  • AGCMs consist of a dynamical core which integrates the equations of fluid motion, typically for:
    • surface pressure
    • horizontal components of velocity in layers
    • temperature and moisture in layers
  • parametrizations handle other processes, these include :
    • radiation (solar/short wave and terrestrial/infra-red/long wave)
    • convection
    • land surface processes and hydrology

A GCM will contain a number of prognostic variables that are directly integrated (e.g. surface pressure) together with a number of diagnostic variables which are deduced from these (e.g. the 1.5 metre temperature, used to compare with observations, is deduced from the surface and lowest-model-layer temperatures).

Oceanic GCMs (OGCMs) model the ocean (with fluxes from the atmosphere imposed) and may or may not contain a sea ice model. The standard resolutionof HadOM3 is 1.25 degrees in latitude and longitude, with 20 vertical levels, leading to approximately 1,500,000 variables.

Coupled atmosphere-ocean GCMs (AOGCMs) (e.g. HadCM3) combine the two models. They thus have the advantage of removing the need to specify fluxes across the interface of the ocean surface. These models are the basis for sophisticated model predictions of future climate, such as are discussed by the IPCC.

AOGCMs represent the pinnacle of complexity in climate models and internalise as many processes as possible. They are the only tools that could provide detailed regional predictions of future climate change. However, they are still under development. The simpler models are generally susceptible to simple analysis and their results are generally easy to understand. AOGCMs, by contrast, are often nearly as hard to analyse as the real climate system.

Model grids

The method by which AGCMs discretise the fluid equations may be the familiar finite difference method or the somewhat harder to understand spectral method. Typical AGCM resolution is between 1 and 5 degrees in latitude or longitude: the Hadley Centre model HadAM3, for example, uses 2.5 degrees in latitude and 3.75 in longitude, giving a grid of 73 by 96 points; and has 19 levels in the vertical. This results in approximately 500,000 "basic" variables, since each grid point has four variables (u,v,T,Q), though a full count would give more (clouds; soil levels). HadGEM1 uses a grid of 1.25 in latitude and longitude.

For a standard finite difference model, the gridlines converge towards the poles. This would lead to computational instabilities (see CFL) and so the model variables must be filtered along lines of latitude close to the poles. Ocean models suffer from this problem too, unless a rotated grid is used in which the North Pole is shifted onto a nearby landmass. Spectral models do not suffer from this problem. There are experiments using geodesic grids [3] (http://unisci.com/stories/20013/0924011.htm) and others.

Variable resolution grids can be used. The "LMDz" model can be arranged to give high resolution over any given section of the planet. HadGEM1 (and other models) use a grid with higher resolution in the tropics to help resolve processes believed to be important for ENSO.

Flux correction

Early generations of AOGCMs required a somewhat ad hoc process of "flux correction" to achieve a stable climate. More recent models do not require this. "Flux correction" was always felt to be an undesirable feature of the models by those that wrote them (as well as by those that did not like them) and was resorted to out of necessity. One of the principle (valid) objections to flux corrections was that they amounted to a "tuning" of the models towards the current climate and made future projections less reliable. The model improvements that now make flux corrections unnecessary are various, but include improved ocean physics, improved resolution in both atmosphere and ocean, and a better fit between atmosphere and ocean models. Most recent simulations show "plausible" agreement with the measured temperature anomalies over the past 150 year, when forced by observed changes in "Greenhouse" gases and aerosols, but better agreement is achieved when natural forcings are also included [4] (http://www.grida.no/climate/ipcc_tar/wg1/figspm-4.htm) [5] (http://www.hadleycentre.gov.uk/research/hadleycentre/pubs/talks/sld017.html).

Convection

In the real world, the earths atmosphere is heated from below by solar radiation, and this becomes unstable. Convection occurs, in which the warm air rises; if cloud condenses latent heat is released and can lead to a positive feedback. This process occurs on too small a scale to be resolved by climate models, and hence must be parametrised. This has been done since the earliest days of cliamte modelling, in the 1950s. Akio Arakawa did much of the early work and variants of his scheme are still used [6] (http://www.aip.org/history/climate/arakawa.htm) although there are a variety of different schemes now in use [7] (http://grads.iges.org/reps/rep27/colarep27.html) [8] (http://www-pcmdi.llnl.gov/projects/modeldoc/amip/10Tbl2.10.html) [9] (http://rainbow.llnl.gov/projects/modeldoc/cmip/table4.html). The behavior of clouds is still poorly understood and is parametrized. [10] (http://www.aip.org/history/climate/GCM.htm). Convection velocity and enstrophy conserving parametrization is in use in the UCLA VI AGCM. [11] (http://www.atmos.ucla.edu/~mechoso/esm/agcm.html) [12] (http://www-pcmdi.llnl.gov/projects/modeldoc/amip/33ucla.html#RTFToC25)

IPCC scenarios

Coupled ocean-atmosphere GCMs are used to project/predict future temperature changes under various scenarios. The IPCC TAR figure 9.3 (http://www.grida.no/climate/ipcc_tar/wg1/fig9-3.htm) shows the global mean response of 19 different coupled models to an idealised experiment in which CO2 is increased at 1% per year [13] (http://www.grida.no/climate/ipcc_tar/wg1/348.htm#fig93). Figure 9.5 (http://www.grida.no/climate/ipcc_tar/wg1/fig9-5.htm) shows the response of a smaller number of models to more realistic climate forcing - although the forcings used depend on projections of future CO2 emissions, which are themselves uncertain.

According to the IPCC, the majority of climatologists agree that important climate processes are incorrectly accounted for by the climate models but don't think that better models would change the conclusion. Critics point out that there are unspecified flaws in the models and unspecified external factors not taken into consideration that could change the conclusion above.

Some solar effects may be very important and are not currently accounted for by temperature-prediction climate models, such as the feedbacks due to direct changes to water vapor caused by solar variation (Sonnemann and Grygalashvyly, Journal of Atmospheric and Solar-Terrestrial Physics, 2005), or feedbacks due to complex changes to the scattering and absorption of cirrus clouds (Baran, Journal of Quantitative Spectroscopy and Radiative Transfer, 2004).

There are areas in which current climate models due a significantly poor job of predicting feedback due to solar forcing of clouds and the greenhouse effect of clouds. In 2003, CCM3 was found to differ from observation by 10.5 W/m2 in the pacific cold tongue region due to an underestimate of the negative feedback due to solar forcing of clouds, and an overestimate of the positive feedback due to the greenhouse effect of clouds. (Sun et. al., Journal of Climate, 2003)

Accurate predictions of climate effects due to solar forcing and its associated feedbacks are important to prediction of effects due to anthropogenic greenhouse gas emissions, because models which fit observed temperature data but underestimate effects due to solar forcing will overestimate effects due to anthropogenic greenhouse gases, and vice versa.

Current climate model predictions match observed recent temperature fluctuations to within a four or five degree of freedom fit [14] (http://seamonkey.ed.asu.edu/~alex/computer/sas/df.html) [15] (http://math.cl.uh.edu/~thompsonla/5537/Model_Assessment_and_Validation.html). Research is continuing to improve the degree of fit to observed data, and to improve certainty and confidence in the predictive power of climate models.

Accuracy of models that predict global warming

Missing image
Hadcm3-era-sst-annual.png
SST errors in HadCM3
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GCM_temp_anomalies_3_2000.jpg
Mean global temperatures from observations and two climate models.

Whether these models are sufficiently "correct" to be useful or not is a matter of debate. GCMs are capable of reproducing the general features of the observed global temperature over the past century [16] (http://www.grida.no/climate/ipcc_tar/wg1/figspm-4.htm).

Thousands of climate researchers around the world use climate models to understand the climate system. There are thousands of papers published about model-based studies in peer reviewed journals - and a part of this research is work improving the models. Improvement has been difficult but steady (most obviously, state of the art AOGCMs no longer require flux correction), and progress has sometimes led to discovering new uncertainties.

In 2000, a comparison between measurements and dozens of CGM simulations of ENSO-driven tropical precipitation, water vapor, temperature, and outgoing longwave radiation found a significant difference. Although there is similarity between measurements and simulation of most factors, the simulated change in precipitation was about one-fourth less than what was observed. Because the behavior of water and energy are closely connected, the precipitation difference should not have been present. If the simulated precipitation is in error, this implies there is another error which causes the simulations of the other factors to produce the observed values. The other possibility is that the satellite-based measurements are in error. Either indicates considerable progress is required in order to monitor and predict such changes. [17] (http://ams.allenpress.com/amsonline/?request=get-abstract&doi=10.1175%2F1520-0442(2000)013%3C0538:TSOTTH%3E2.0.CO%3B2) [18] (http://www.co2andclimate.org/climate/previous_issues/vol5/v5n10/cutting1.htm)

A rather more complete discussion of climate models is provided by the IPCC TAR chapter 8, Model Evaluation (http://www.grida.no/climate/ipcc_tar/wg1/308.htm) (2001).

  • The model mean exhibits good agreement with observations.
  • The individual models often exhibit worse agreement with observations.
  • Many of the non-flux adjusted models suffered from unrealistic climate drift up to about 1C/century in global mean surface temperature.
  • The errors in model-mean surface air temperature rarely exceed 1C over the oceans and 5C over the continents; precipitation and sea level pressure errors are relatively greater but the magnitudes and patterns of these quantities are recognisably similar to observations.
  • Surface air temperature is particularly well simulated, with nearly all models closely matching the observed magnitude of variance and exhibiting a correlation > 0.95 with the observations.
  • Simulated variance of sea level pressure and precipitation is within ±25% of observed.
  • All models have shortcomings in their simulations of the present day climate of the stratosphere, which might limit the accuracy of predictions of future climate change.
    • There is a tendency for the models to show a global mean cold bias at all levels.
    • There is a large scatter in the tropical temperatures.
    • The polar night jets in most models are inclined poleward with height, in noticeable contrast to an equatorward inclination of the observed jet.
    • There is a differing degree of separation in the models between the winter sub-tropical jet and the polar night jet.
  • For nearly all models the r.m.s. error in zonal- and annual-mean surface air temperature is small compared with its natural variability.
    • There are problems in simulating natural seasonal variability.( 2000) (http://pubs.giss.nasa.gov/abstracts/2000/CoveyAbeOuchi.html)
      • In flux-adjused models, seasonal variations are simulated to within 2 K of observed values over the oceans. The corresponding average over non-flux-adjusted models shows errors up to ~6 K in extensive ocean areas.
      • Near-surface land temperature errors are substantial in the average over flux-adjusted models, which systematically underestimates (by ~5 K) temperature in areas of elevated terrain. The corresponding average over non-flux -adjusted models forms a similar error pattern (with somewhat increased amplitude) over land.
      • In Southern Ocean mid-latitudes, the non-flux-adjusted models overestimate the magnitude of January-minus-July temperature differences by ~5 K due to an overestimate of summer (January) near-surface temperature. This error is common to five of the eight non-flux-adjusted models.
      • Over Northern Hemisphere mid-latitude land areas, zonal mean differences between July and January temperatures simulated by the non-flux-adjusted models show a greater spread (positive and negative) about observed values than results from the flux-adjusted models.
      • The ability of coupled GCMs to simulate a reasonable seasonal cycle is a necessary condition for confidence in their prediction of long-term climatic changes (such as global warming), but it is not a sufficient condition unless the seasonal cycle and long-term changes involve similar climatic processes.
Missing image
Climate_model_NA_annual_precipitation_2002.jpg
North American precipitation from various models.
  • Coupled climate models do not simulate with reasonable accuracy clouds and some related hydrological processes (in particular those involving upper tropospheric humidity). Problems in the simulation of clouds and upper tropospheric humidity, remain worrisome because the associated processes account for most of the uncertainty in climate model simulations of anthropogenic change.

There is a debate over how to reconcile climate model predictions that upper air (tropospheric) warming should be greater than surface warming, with observations some of which appear to show otherwise (see also satellite temperature record) [19] (http://www4.nationalacademies.org/news.nsf/isbn/0309068916?OpenDocument). Possible explanations include errors in the surface or upper-air records; a problem with the model; or just the shortness of the observed record. This problem is no longer as intense as it used to be a few years ago, because (1) all versions of the satellite record now show warming; (2) there are now multiple versions of the satellite temperature record, some of which show warming greater than that observed at the surface.

Missing image
GCM_temp_forecasts_10.jpg
Temperature trends from some climate models.

The precise magnitude of future changes in climate is still uncertain [20] (http://www.grida.no/climate/ipcc_tar/wg1/339.htm); for the end of the 21st century (2071 to 2100), for SRES scenario A2, the change of global average SAT change from AOGCMs compared with 1961 to 1990 is +3.0C and the range is +1.3 to +4.5C. There uncertainty about the accuracy of climate models, chiefly in the areas of clouds and aerosols which have the potential significantly change the net effect of CO2, although the uncertainty is such that it is not known if they under- or overpredict future climate change. The paleo climate data, suggests that the predicted impact of CO2 should be lower than the models predict, although the paleo data reflects long term equilibria and cannot rule out higher temperature increases within the lifespans of humans living today.

Forecasts of climate change are inevitably uncertain. A basic problem with all such predictions to date has been the difficulty of providing any systematic estimate of uncertainty, a problem that stems from the fact that these [climate] models do not necessarily span the full range of known climate system behavior. [21] (http://epw.senate.gov/repwhitepapers/ClimateChange.pdf)

Relation to weather forecasting

The global climate models used for climate projections are very similar in structure to (and often share computer code with) numerical models for weather prediction but are nonetheless logically distinct: see climate vs weather for details.

Most weather forecasting is done on the basis of interpreting the output of GCM data. Since forecasts are short - typically a few days or a week - such models do not usually contain an ocean model but rely on imposed SSTs. They also require accurate initial conditions to begin the forecast - typically these are taken from the output of a previous forecast, with observations blended in. Because the results are needed quickly the predictions must be run in a few hours; but because they only need to cover a week of real time these predictions can be run at higher resolution than in climate mode. Currently ECMWF runs at 40 km resolution [22] (http://www.ecmwf.int/index_forecasts.html) as opposed to the 100-200 km scale used by typical climate models. Nested models can be run forced by the global models for boundary conditions, to achieve higher local resolution: the Met Office runs a mesoscale model with an 11 km resolution [23] (http://www.metoffice.gov.uk/research/nwp/numerical/operational/index.html) covering the UK.

Using the output from these models, together with satellite pictures and conventional data, weather forecasting may examine the effects of a single storm front moving in several different ways across part of a continent.

Formerly, weather forecasting also used methods which have less similarity to climate studies. Simply searching past records for situations similar to current conditions upwind of a city can produce a forecast based upon what usually happens in that city, but this "analogues" approach is now less common. More often, an experienced forecaster will use local knowledge to interpret the model output. A river valley or lake may produce local effects which local forecasting is interested in, but the effects are too small to affect continental-scale patterns.

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