in Table of EMICS, edited by Martin Claussen

Toward a Planet Simulator: PUMA - LSG

Principal Investigators

G. Lohmann ( gerrit.lohmann@dkrz.de)

F. Lunkeit ( lunkeit@dkrz.de)

E. Maier-Reimer

E. Kirk

M. Latif

K. Fraedrich

Max-Planck-Institute for Meteorology, Hamburg, Germany

 

Meteorologisches Institut, Universität Hamburg, Germany

 

A Scope of the model

An Earth system model of intermediate complexity is developed for the study of climate dynamics on decadal and millennial time-scales. The main task is to identify the driving mechanisms and potential thresholds responsible for climate transitions. Emphasis is placed on the multiple states of the system and the interaction of the dominant pattern of atmospheric variability with the ocean and land surface. In contrast to conventional time-slice experiments, the present approach is not restricted to equilibrium transitions and is capable to utilise all available data for validation. Transient simulations for the past and future climate will examine feedback mechanism in the climate system. Pathways of orbital forcing into climate response will reveal the understanding of climate records. The model explicitely resolves the three-dimensional atmospheric and oceanic dynamics and is therefore conceptual different from statistical dynamical models.

At time-scales comparable to the glacial-interglacial cycles, the importance of each Earth system component has not been estimated. At this early stage of exploration for the coupled system, it is necessary to be able to carry out a large number of sensitivity experiments. It is expected that, compared to e.g. scenario calculations for the next century, different processes will dominate Earth system interactions at such long time scales. This has to be accounted for a suitable modelling framework in order to allow cooperation between expert groups of different focus. The Earth system model shall have a modular structure with portable Fortran code. The modular structure of the model enables the user to modify model configurations according to the application. New schemes and model components can be included with a minimum of technical expense which is particularly useful for paleoclimatic applications.

 

 

B Model components

Atmosphere

The Portable University Model of the Atmosphere (PUMA) [Fraedrich et al., 1998] is based on the Reading multi-level spectral model described by Hoskins and Simmons [1975]. The model solves the primitive equations using terrain following-coordinates in the vertical. The PUMA model has been extended by relatively simple radiation and precipitation schemes. A snow model following Loth [1995] has been implemented.

Ocean

The atmospheric model has been coupled to the ocean model LSG [Maier-Reimer et al., 1993] designed especially for long-term climate studies (time step of one month). This model contains a parameterization for the bottom boundary layer [Beckmann and Döscher, 1997] which drastically improves the density-driven downslope flows [Lohmann, 1998] and is essential for the interpretation of paleoclimatic records [Lohmann and Schulz, 2000].

Sea ice model

Thermodynamic sea ice model including a simple momentum balance for advection of sea ice.

Carbon Cycle

In the LSG ocean model , the HAMOCC carbon cycle model [Maier-Reimer, 1993] is included. First experiments exist for the terrestrial biosphere model LPJ (Lund-Potsdam-Jena) [Sitch et al., 2000], which is forced with the PUMA-LSG climate. The LPJ model is a dynamic global vegetation model combining mechanistic treatments of terrestrial vegetation dynamics, carbon and water cycling.

Coupling

The present version of the model uses a T21/L5 resolution for the atmosphere and 11 vertical levels with horizontal resolution of 5 degrees for the ocean. The model contains representations of sub-grid scale fluxes over land, ice, and open sea. The coupled atmosphere-ocean-sea ice model does not require flux adjustments.

Miscellaneous

 

C Limitations

Limitation of the current model version is due to the missing feedbacks by cryosphere and vegetation. Further limitations are due to the simplified radiation codes used (chemistry and dust). The coarse resolution and the neglected non-linear terms in the oceanic momentum balance restrict studies to spatial scales of more than a thousand kilometers, the model cannot adequately resolve interannual climate variability in the tropical Pacific.

 

D Performance

The required CPU time for the coupled atmosphere-ocean model is less than 8 min per year on the present Cray in Hamburg, i.e. approximate two orders of magnitude faster than complex GCMs. In the asynchronously coupled mode, where atmosphere and ocean model components take even parts in computing time, about 1000 years of model integration can be performed on one day.

 

Atmosphere model PUMA

7 years/1 h CPU

2 MW

Fraedrich et al., 1998

Ocean model LSG

200 years/1 h CPU

5 MW

Maier-Reimer et al., 1993

Marine carbon cycle HAMOCC3

200 years/1 h CPU

10 MW

Maier-Reimer, 1993

Planed:

Terrestrial biosphere LPJ

200 years/1 h CPU

1 MW

Sitch et al., 2000

 

 

E Applications

The model components have been extensively tested in studies of paleoclimate [Winguth et al., 1999], future climate change scenarios for the next century [Lunkeit et al., 1998], and storm track variability [Frisius et al., 1998]. The model is flexible enough to turn various feedback processes off and on, to study the cause and relationships of the climate components. Simulations and sensitivity studies will focus on the following topics:

 

F References

Bagliani, F. Fraedrich, J. Hardenberg, F. Lunkeit, 2000: Lagrangian tracer homogenization and dispersion in a simplified atmospheric GCM. Il Nuovo Cimento (in press).

Beckmann, A., and R. Döscher, 1997: A method for improved representation of dense water spreading over topography in geopotential-coordinate models. J. Phys. Oceanogr., 27, 581-591.

Fraedrich, K., E. Kirk, and F. Lunkeit, 1998: Portable University Model of the Atmosphere, DKRZ Report 16. ( http://dome.dkrz.de/kirk/puma/puma.html )

Frisius, T, Lunkeit, F., Fraedrich, K., and James, I. N., 1998: Storm-track organization and variability in a simplified atmospheric global circulation model. Q. J. R. Meteorol. Soc., 124, 1019-143.

Hardenberg, J., K. Fraedrich, F. Lunkeit, A. Provenzale, 2000: Transient chaotic mixing during a baroclinic life cycle. CHAOS, 10, 122-134.

Heinze, C., E. Maier-Reimer, A. M. E. Winguth, and D. Archer, 1999: A global oceanic sediment model for long-term climate studies. Global Biogeochemical Cycles, 13, 221-250.

Hoskins, B. J., and A. J. Simmons, 1975: A multi-layer spectral model and the semi-implicit method. Q. J. R. Meteorol. Soc., 101, 1231-1250.

Lohmann, G., 1998: The Influence of a near-bottom Transport Parameterization on the Sensitivity of the Thermohaline Circulation. J. Phys. Oceanogr., 28, 2095-2103.

Lohmann, G., and Schulz, M., 2000: Reconciling Bølling warmth with peak deglacial meltwater discharge. Pale- oceanography, (in press).

Loth, B., 1995: Die Schneedecke als Komponente des Klimasystems und ihre Modellierung. Max-Planck-Institut für Meteorologie. Examensarbeit Nr. 32.

Lunkeit, F., S. E. Bauer, and K. Fraedrich, 1998: Storm tracks in a warmer climate: Sensitivity studies with a simplified global circulation model. Clim. Dyn., 14, 813-826.

Maier-Reimer, E., 1993: Geochemical cycles in an ocean general circulation model. Preindustrial Tracer Distributions. Global Biogeochemical Cycles, 7, 645-677.

Maier-Reimer, E., U. Mikolajewicz, and K. Hasselmann, 1993: Mean circulation of the Hamburg LSG OGCM and its sensitivity to the thermohaline surface forcing. J. Phys. Oceanogr., 23, 731-757.

Sitch, S., Prentice, I. C., Smith, B., and LPJ consortium members, 2000: A coupled model of vegetation dynamics and the terrestrial carbon cycle. in: S. Sitch, The role of vegetation dynamics in the control of atmospheric CO2 content. Lund, Sweden.

Winguth, A., D. Archer, E. Maier-Reimer, U. Mikolajewicz, and J.-C. Dupplessy,1999: Sensitivity of the paleonutrient tracer distribution and deep-sea circulation to glacial boundary conditions. Paleoceanogr., 14, 304-323.