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4.2 J. Masek: Idealized tests of ALADIN-NH dynamical kernel at very high resolution 168
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NEWSLETTER of the 28 th EWGLAM and
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Newsletter of the 28th EWGLAM and 1
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6.2 P. Clark et al.: The Convective
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1.1 Foreword In 2006, MeteoSwiss ha
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Cornel Soci National Meteorological
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16:15 - 16:45 Filip Vana general Dy
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2 Consortia and ECMWF reports 12
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Research Progress at ECMWF 2005-200
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ocean data assimilation system for
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Physical Aspects 1) The introductio
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either with a 1-dimensional observa
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2.2 ALADIN 22
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Another important event happened, i
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• However inspection of T2m forec
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Figure 4: One case of intercomparis
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The COSMO Consortium in 2005-2006 T
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2. Model system overview The key fe
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Data Assimilation for LM Method: Nu
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2. LM performance known, critically
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expected to result in an improved r
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Schrodin, R. and H. Heise, 2002: Th
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HIRLAM-A activities in 2006 Jeanett
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addition, research on the construct
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HIRLAM Reference System development
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Fig. 2: Case study for 10 June 2006
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Unified Model Developments 2006 Met
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Figure 4: Noise in increments from
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Cycle Date Model change and impact
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1.5km On-demand model Figure 8: 1.5
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3.1 Belgium 59
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• A prognostic mass-flux scheme f
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Perspectives The integrated package
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3.2 Croatia 65
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New computer Core of the new comput
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3.3 Czech Republic 69
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ÏÄÅ ÊÔÓÖØ ¾¼¼ ÖÓÑ Ø
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ÙÖ ¿ ËÙÖ ÔÖÑØÖ× ÖÓÑ
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LAM efforts at Estonian Meteorologi
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grid is 186x170 points in horizonta
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McDonald, A., and J. E. Haugen, 199
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Operational NWP Activities at the F
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Model Forecast model Limited area g
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3.7 France 87
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Fig.1. The ALADIN-France domain, wi
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Towards AROME, A first try of a Rap
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Status Report of the Deutscher Wett
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In August 2006 production with the
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3.9 Hungary 97
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• LBC coupling at every 3 hours O
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IFS as driving model for ALADIN. Th
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3.10 Ireland 103
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Filtering: Fourth order implicit ho
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The next chart shows wind arrows at
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Italian Meteorological Service Stat
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Fig.3 Integration domain for LM- EU
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3.12 Netherlands 113
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esults with fixed entrainment and d
Page 119 and 120: simulation. In order to allow a goo
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Page 125 and 126: Limited Area Modelling Activities a
Page 127 and 128: (a) Figure 2 ALADIN/Portugal geogra
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Page 131 and 132: LAM ACTIVITIES IN ROMANIA Cornel SO
Page 133 and 134: Fig.3 HRM domain, 78 cumulated prec
Page 135 and 136: - Experiments : variation of the fr
Page 137 and 138: NWP activities at Slovak Hydrometeo
Page 139 and 140: Operational suite upgrades • 23/0
Page 141 and 142: 3.16 Slovenia 139
Page 143 and 144: First experiments with new physical
Page 145 and 146: • resolution of meteorological fi
Page 147 and 148: NWP activities in INM Bartolomé Or
Page 149 and 150: 1 System definition • Creation of
Page 151 and 152: MSLP June-August 2006 Geopotential
Page 153 and 154: NATIONAL STATUS REPORT on Operation
Page 155 and 156: Model input The observations used f
Page 157 and 158: Numerical Weather Prediction at Met
Page 159 and 160: The setup is based on a new numeric
Page 161 and 162: weight of importance in the voting
Page 163 and 164: 4.1 F. Vana: Dynamics & Coupling, A
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Page 181 and 182: 5 Scientific presentations on data
Page 183 and 184: COSMO: Overview and Strategy on Dat
Page 185 and 186: Meteorology in Hamburg (MPI-M). The
Page 187 and 188: temperature forecasts, this had a s
Page 189 and 190: 5.2 D. Leuenberger et al.: The Late
Page 191 and 192: scaling factor α and of the latent
Page 193 and 194: a) b) RAD 1 2 3 4 5 6 7 8 9 10 det
Page 195 and 196: 5.3 C. Fischer and A. Horanyi: Alad
Page 197 and 198: Figure 1: analysis increments of wi
Page 199 and 200: 3) Averaged emissivities + dynamica
Page 201 and 202: In parallel, a direct radar observa
Page 203 and 204: ►Algorithms: • FGAT (with Hunga
Page 205 and 206: Data assimilation activities in LAC
Page 207 and 208: Fig.3 RMSE difference (WDEF-NAM2).
Page 209 and 210: 6 Scientific presentations on physi
Page 211 and 212: Physics improvements in the NAE mod
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Page 217 and 218: Relaxation term Due to these proble
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Buncefield oil depot fire Figure 15
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6.2 P. Clark et al.: The Convective
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y the model (e.g. streaks of gradua
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the Met Office Large Eddy Model (LE
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Figure 4 Domains used in high resol
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1.0 95th percentile threshold Fract
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Figure 10 Surface precipitation rat
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HIRLAM Physics developments Sander
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strong winds. This causes a too lar
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epresenting the weather in the case
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×ÖÔØÓÒ Ó Ð ÑÓÐº Ìº
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ALARO-0 Physics developments at LAC
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eflectance for sample of 3-layer in
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2.1 Pseudo prognostic turbulent kin
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TKE and the integral buoyancy of th
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7 Scientific presentations on predi
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LAMEPS Development of ALADIN-LACE Y
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The more iterations performed, the
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uncertainty in the model physics, t
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In Budapest, dynamical downscaling
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7.2 J. García-Moya et al.: Recent
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Currently the size of the super ens
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Palmer, T.N., Alessandri, A., Ander
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Figure 4 Example of probability map
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More than 15 mm/6 hours Figure 6 Re
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7.3 C. Marsigli et al.: The COSMO S
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ÔÓ××Ð Ù×× Ó ÓÖ×Ø ÖÖ
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ÇËÅÇßËÊÈË × ½ßÑÑÖ
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¾℄ ÅÖ×Ð¸ º¸ ÅÓÒØÒ¸
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Overview COSMO ensemble systems Pie
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COSMO-LEPS 16-MEMBER EPS An objecti
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The used models are LAMI (Italy), a
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28th EWGLAM Meeting 9-11 October 20
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9 SRNWP business meeting report 293
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Minutes of the Meeting Participatio
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Training and Education Activities i
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These reports were very divers, fro
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Contacts with the Academia In his d
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