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Weather and climate modelling expands to cover the globe Tony Slingo, ESSC University of Reading “The past, the present and the future of global weather.

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Presentation on theme: "Weather and climate modelling expands to cover the globe Tony Slingo, ESSC University of Reading “The past, the present and the future of global weather."— Presentation transcript:

1 Weather and climate modelling expands to cover the globe Tony Slingo, ESSC University of Reading “The past, the present and the future of global weather and climate modelling” Royal Meteorological Society meeting, University of Reading, 25 April 2007 Scope: from the 1950s to the 1990s Emphasis: NWP and climate models mainly atmospheric models (not ocean models or data assimilation) quite a bit about parametrizations (not surprisingly!)

2 Early developments in the USA 1950: Charney, Fjortoft and von Neumann 1956: Phillips (first general circulation experiment) The start of NWP and climate modelling –1954: Joint Numerical Weather Prediction Unit 1958: National Meteorological Center (NMC) 1974: NMC ran the first global grid-point model –Geophysical Fluid Dynamics Laboratory (GFDL) originally (1955) a section of the US Weather Bureau led by Smagorinsky, with Manabe, Miyakoda, Bryan, … 1963: 9 level primitive equation grid-point model many firsts (hydrological cycle, coupled ocean-atmosphere, CO 2 ) –University of California Los Angeles (UCLA) grid-point model (Mintz/Arakawa) Goddard Institute for Space Studies (GISS), GSFC and others –National Center for Atmospheric Research (NCAR) grid-point model (Kasahara/Washington)

3 Several countries developed NWP and climate models –e.g. Sweden (1954), UK, France, Germany, Australia, Canada –more on the UK Met Office in a moment First spectral model developed by Bourke (1972, 1974) –was exported to GFDL, where it replaced the grid-point model, and to NCAR, where it replaced the Kasahara/Washington model and became the Community Climate Model (CCM) ECMWF was founded in 1975 –first model was global, grid-point (August 1979) –replaced by a spectral model in 1983 –exported to create the climate model at the Max Planck Institute for Meteorology, in Hamburg Early developments outside the USA

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5 1957-58: IGY – International Geophysical Year 1967: GARP –Global Atmospheric Research Programme 1974: GATE – GARP Atlantic Tropical Experiment – the first large-scale tropical experiment 1978-1979: FGGE – First GARP Global Experiment – global weather observations for an entire year – coincided with the launch of Tiros-N Some other key international developments

6 NWP –1959 (Ferranti Mercury): experimental 2-level limited area model –1965 (KDF 9): 3-level quasi-geostrophic model operational  –1972 (IBM 360/195): 10-level primitive equation model (Bushby) Northern Hemisphere, and embedded European “rectangle” –1982 (CDC Cyber 205): 15-level, 150km, 144h global forecasts Climate –5-level model (Corby, Gilchrist and Newson, 1975) –1972: 11-layer model, used as a tropical model for GATE by Peter Rowntree’s group –stratospheric model for the Comesa project –1990: Hadley Centre for climate prediction and research Unified Forecast/Climate Model –1991 (Cray Y-MP): first version had 19 levels –2002: New Dynamics All of the above were/are grid-point models NWP and climate modelling in the Met Office

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8 Phillips (1956) “Certain of the assumptions in this particular numerical experiment can be eliminated in a rather straightforward manner, e.g. the geostrophic assumption and the simplified geometry. However, a further refinement of the model will soon run into the more difficult physical problems of small-scale turbulence and convection, the release of latent heat, and the dependence of radiation on temperature, moisture and cloud. Progress in the past in developing an adequate theory of the general circulation has had as its main obstacle the difficulty of solving the non-linear hydrodynamical equations. High-speed computing machines have to some extent eliminated this problem, and further progress in understanding the large-scale behaviour of the atmosphere should come to depend more and more on a fuller understanding of the physical processes mentioned above.”

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10 Parametrization highlights Convection –early models: simple convective adjustment –more advanced: mass-flux convection schemes Arakawa and Schubert (1974) Rowntree scheme: Lyne and Rowntree (1976), Gregory and Rowntree (1990). Modified to include saturated downdraughts, convective momentum transfer Betts and Miller (1986); convective adjustment scheme, ECMWF Tiedtke (1989), ECMWF

11 Arakawa and Schubert (1974)

12 Gregory and Rowntree (1990)

13 Representation of orography The upper figure shows the surface orography over North America at a resolution of 300km, as in a low resolution climate model. The lower figure shows the same field at a resolution of 60km, as in a weather forecasting model.

14 Parametrization highlights Orographic gravity wave drag –As the horizontal resolution of climate models improved, by the 1980s some models showed evidence of anomalously strong westerly winds at mid-latitudes –This was particularly noticeable in the Met Office 11- layer model and was known as the “westerly problem” –The problem was solved by Palmer, Shutts and Swinbank (1986), who developed a parametrization for the drag produced by gravity waves excited by unresolved orography –A similar parametrization was developed by McFarlane (1986) and used in the Canadian climate model

15 Slingo and Pearson (1987)

16 Parametrization highlights Radiation –early models: prescribed from climatological calculations –more advanced: interactive radiation, clouds Manabe and Strickler (1964) 11-layer model (Walker 1977) Lacis and Hansen (1974), which anticipated; –even more advanced: full scattering codes Edwards and Slingo (1996), used in Unified Model Mlawer et al. (1997), used in ECMWF model

17 Manabe and Strickler (1964)

18 Walker (1977)

19 Lacis and Hansen (1974)

20 Turner et al. (2004)

21 Parametrizations and model resolution Many of the parametrizations used in GCMs fall within the ambit of Phillips’ comments on the non-linear hydrodynamical equations Radiation does not, but convection, boundary layer and wave drag processes do For many of these processes, we have made little progress in understanding how to parametrize them, or even whether they can be parametrized at all This suggests that we need to increase the resolution of GCMs substantially, either to resolve these motions explicitly or at least to give parametrizations a chance to work properly on scales that can be parametrized Have climate modellers done this?

22 GATE Tropics 1974 Global 11-level 1980 HadCM2 1994 HadCM3 1998 HadGEM1 2004 Atmosphere~200km 11 levels ~300km 11 levels ~300km 19 levels ~300km 19 levels ~150km 38 levels Ocean--2.5 0 x 3.75 0 20 levels 1.25 0 x 1.25 0 20 levels 1 0 x 1 0 (1/3 0 ) 40 levels Flux Adjustment? --YesNo Computing??1440 Progression of Met Office climate models from the original 11-layer model onwards

23 Why haven’t climate modellers increased the resolution of their models? Because there have been other priorities: –standard runs of the 11-layer model on the IBM 360/195 were 50 days in length –but climate integrations (e.g. for global warming predictions) need complex models run on decadal to century timescales –so, all of the extra computing power has had to be directed towards longer integrations of more complex models, with ensembles to investigate different scenarios and to provide better signal to noise In contrast, every time that more computing resources have become available, the resolution of NWP models has been increased –because high resolution is needed to assimilate the initial data properly and to provide regional detail in the forecasts –and of course weather forecasts are run for days, not years, and the models do not need to be quite so complicated

24 Duration and/or Ensemble size Resolution Computing Resources Complexity 1/12 0 Resolution, complexity, duration/ensemble size

25 Conclusion It is time to start running climate models at much higher resolution, not for all applications of course, but at least to try to make progress with the parametrization problem and to meet the challenge articulated by Phillips in 1956

26 Sources of information Don’t bother to copy all this down, go to http://www.nerc-essc.ac.uk/~as/http://www.nerc-essc.ac.uk/~as/ Randall, D.A. (Ed.) 2000. General circulation model development. Academic Press Washington, W.M. and Parkinson, C.L., 2005. An introduction to three dimensional climate modeling. University Science Books Trenberth, K.E.,1995. Climate system modeling. Cambridge University Press Web pages: –http://wwwt.ncep.noaa.gov/nwp50/ (meeting on 50 th anniversary of NWP)http://wwwt.ncep.noaa.gov/nwp50/ –http://www.aip.org/history/sloan/gcm/intro.html(history of GCM modelling)http://www.aip.org/history/sloan/gcm/intro.html –http://www.metoffice.gov.uk/research/nwp/publications/nwp_gazette/sep02/ history_nwp.html(Met Office website)http://www.metoffice.gov.uk/research/nwp/publications/nwp_gazette/sep02/ history_nwp.html –http://celebrating200years.noaa.gov/historymakers/Smagorinsky/welcome. html(general website; this one about Joseph Smagorinsky)http://celebrating200years.noaa.gov/historymakers/Smagorinsky/welcome. html –http://www.bom.gov.au/bmrc/basic/wksp16/papers/papers.shtmlhttp://www.bom.gov.au/bmrc/basic/wksp16/papers/papers.shtml (BMRC Workshop November 2004; several excellent talks) –http://www.ecmwf.int/newsevents/training/(ECMWF website)http://www.ecmwf.int/newsevents/training/


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