moslef (mode 2) summer velocity moslef (mode 3) summer velocity promes-moslef: an atmosphere-ocean...
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MOSLEF (MODE 2) SUMMER VELOCITY
MOSLEF (MODE 3) SUMMER VELOCITY
PROMES-MOSLEF: An atmosphere-ocean coupled regional model. Coupling and preliminary results over the Mediterranean basin
MWB02
ABSTRACT
Over the last year, in the frame of the Spanish project MERCATOP, the regional atmospheric climate model PROMES and the finite elements semi-Lagrangian ocean model MOSLEF have been integrated in a unique system named PROMES-MOSLEF. OASIS3 coupler has been used as grid interpolator, inter-model communicator and inter-language communicator to link these two models. Currently, the system can be run in four different modes: atmosphere mode, ocean mode with climatological atmospheric feeding, ocean mode with regional modelling atmospheric feeding, and atmosphere-ocean coupled mode. Following MedCordex specifications, the first simulations using the system PROMES-MOSLEF have been focussed in the Mediterranean basin and the ERA-Interim period. In this work preliminary results obtained by using the system are shown and a comparison of those simulations is also presented.
Clemente Gallardo Andrés, Institute of Environmental Sciences – Universidad de Castilla La Mancha, Toledo, Spain
Pedro Galán del Sastre, Department of Applied Mathematics (ETSAM) – Universidad Politécnica de Madrid, Madrid, Spain
Rodolfo Bermejo Bermejo, Department of Applied Mathematics (ETSII) – Universidad Politécnica de Madrid, Madrid, Spain
MOSLEFMOSLEFPROMESPROMES
OASIS-3OASIS-3
INTERF
ACE
INTERF
ACEINTERFACE
INTERFACE
COUPLING
Semi-Lagrangian Finite Element Ocean ModelSemi-Lagrangian Finite Element Ocean Model
Primite Equations of the OceanPrimite Equations of the Ocean
Time DiscretizationTime Discretization• Implicit scheme for diffusion termsImplicit scheme for diffusion terms• Semi-Lagrangian approach for advection termsSemi-Lagrangian approach for advection terms• Splitting scheme to decouple velocity and pressureSplitting scheme to decouple velocity and pressure
Unconditional stable scheme Unconditional stable scheme ΔΔt = 1h 30 mint = 1h 30 min
Spatial DiscretizationSpatial Discretization Finite Element MethodFinite Element Method
• Unstructured meshesUnstructured meshes• Easy definition of the boundaryEasy definition of the boundary• Easy refinement in regionsEasy refinement in regions
Oasis 3 has been used in our coupled model as:Oasis 3 has been used in our coupled model as:• Grid interpolatorGrid interpolator• Inter-model communicatorInter-model communicator• Inter-language communicatorInter-language communicator
Communication technique: CLIM/MPI1Communication technique: CLIM/MPI1
PROMES uses OASIS Box partition type. PROMES uses OASIS Box partition type.
MOSLEF currently uses a Serial partition typeMOSLEF currently uses a Serial partition type
Recent Improvements in the regional atmospheric Recent Improvements in the regional atmospheric model PROMES:model PROMES:
• ECMWF-based RadiationECMWF-based Radiation
• ORCHIDEE land surface modelORCHIDEE land surface model
Interactive phenologyInteractive phenology
Dynamic vegetationDynamic vegetation
River routingRiver routing
The system can be run in four different modes: The system can be run in four different modes: 1.1. atmosphereatmosphere2.2. ocean with climatological atmospheric forcingocean with climatological atmospheric forcing3.3. ocean with ARCM forcing, and ocean with ARCM forcing, and 4.4. atmosphere-ocean full coupledatmosphere-ocean full coupled
MOSLEF (MODE 2) WINTER VELOCITY
MOSLEF (MODE 3) WINTER VELOCITY
PRELIMINARY RESULTS
Several preliminary simulations have been run in order to test the proper working of the system.
Here some results of two simulations of the ocean model MOSLEF in the mode 2 of the system (atmospheric forcing provided by climatology) and the mode 3 (atmospheric forcing provided by PROMES, but MOSLEF running offline) are shown
In the pictures a correct performance of MOSLEF can be seen. Both in summer and winter the model results have a reasonably good approximation to the main characterictics of the Mediterranean Sea surface circulation (see Roussenov et al., 1997 and its references).
Mode 2 and mode 3 of the system give lightly different results, mainly in the strength of some vortex. This is an expected result because of the larger variability of the ARCM atmospheric forcings.
REFERENCES ACKNOWLEDGMENTSRoussenov, V., E. Stanev, V. Artale and N. Pinardi (1995) A seasonal model of the Mediterranean Sea general circulation. J. Geophys. Res., 100 (C7): 13515 -13538.
Dorado, E. (2009) Estudio de soluciones numéricas de largo plazo de los modelos de ecuaciones primitivas de la circulación general del océano. PhD thesis, Universidad Complutense de Madrid.
Castro M, Fernandez C, Gaertner MA (1993) Description of a meso-scale atmospheric numerical model. In: Diaz JI, Lions JL (eds) Mathematics, climate and environment, Masson (ISBN: 2-225-84297-3), p273.
Valcke, S. (2006) OASIS3 User Guide (oasis3_prism_2-5) PRISM Support Initiative Report No 3. CERFACS, Toulouse, France. 64 pp.
This work has been funded through the Spanish projects CGL2007-66440-C04-01 and CGL2007-66440-C04-02 of the Education and Science Ministry of Spain