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Objective verification results for RK parallel runs

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Presentation on theme: "Objective verification results for RK parallel runs"— Presentation transcript:

1 Objective verification results for RK parallel runs
Lucio Torrisi CNMCA, National Meteorological Center,Italy COSMO General Meeting, Moscow 6-9 September 2010 1

2 CNMCA NWP System Data Assimilation: 2.8 km 50 v.l. 14 km 40 v.l. 7 km
3DVAR PSAS FGAT (T,u,v,qv,ps) every 3h using TEMP, PILOT, SYNOP, SHIP, BUOY, Wind Profiler, AMSUA rad., AMDAR-ACAR-AIREP, MSG/MODIS AMV, METOP/QUIKSCAT/ERS2 scatt. winds + Land SAF snow mask, IFS SST analysis once a day Data Assimilation: COSMO-ME (7km) ITALIAN MET SERVICE 2.8 km 50 v.l. compressible equations explicit convection 14 km 40 v.l. hydrostatic equations parameterized convection 7 km 40 v.l. compressible equations parameterized convection Local Area Modelling: COSMO 2 2 2 2 2 2 2

3 7km RK/LF comparison In March, itype_bbc_w in COSMO-ME RK (with explicit vertical advection) parallel run was switched from 1 to 0 . Option for selecting the lower boundary condition for vertical wind speed (new NL switch itype_lbc_w): 0/1: RK-like method following iadv_order 2/3: Differencing following iadv_order without RK stepping 4/5: Fourth-order centered differences 0/2/4: include extrapolation of horizontal wind to surface 1/3/5: no extrapolation of horizontal wind to surfacee

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8 7km RK/LF comparison RK has a colder bias in stratosphere (Rayleigh damping setting?) RK slightly warmer than LF in the lower levels RK slightly less negative bias in wind speed than LF RK tends to overestimate light precipitation events and underestimate the most intense ones

9 Heat and moisture source term in p equation
Turbulent heat and Radiaton flux Diabatic heating due to cloud microphysical sources Turbulent flux for water constituents Cloud heat sources Turbulent flux for water constituents and Precipitation (gravitational diffusion) fluxes

10 Heat and moisture source term in p equation
The reformulated equations are: If these new terms are added in the p/T equations, the saturation adjustment scheme has to be consistently adapted to the changes in p/T equations. ( in coop. with Ronny Petrik)

11 Heat and moisture source term in p equation
A preliminary version with QT>>QM was already implemented a few years ago (Torrisi, 2008) The full version is almost complete Work in the saturation adjustment is ongoing In cooperation with Ronny Petrik

12 Thanks for the attention!
Any questions?


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