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A NUMERICAL PREDICTION OF LOCAL ATMOSPHERIC PROCESSES

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Title: A NUMERICAL PREDICTION OF LOCAL ATMOSPHERIC PROCESSES


1
A NUMERICAL PREDICTION OF LOCAL ATMOSPHERIC
PROCESSES
  • A.V.Starchenko
  • Tomsk State University

2
Introduction
Nowadays a broad range of problems of atmospheric
physics, climate and environment protection is
solved with application of mathematical
modelling approach. Modelling systems, developed
at large centres of atmospheric research, are
applied for scenario analysis, weather
prediction, air quality investigation. For
example, CMAQ, Community Multiscale Air Quality
Chemical Transport Modelling System EURAD,
EURopean Acid Deposition model, EZM, European
Zooming Model. Dynamic core of such systems are
or well-known models (e.g. MM5) either original
models.
3
MM5 (Mesoscale Model 5)
The PSU/NCAR mesoscale model is a limited-area,
nonhydrostatic or hydrostatic, terrain-following
sigma-coordinate model designed to simulate or
predict mesoscale and regional-scale atmospheric
circulation. It has been developed at Penn State
and NCAR as a community mesoscale model. The
Fifth-Generation NCAR / Penn State Mesoscale
Model (MM5) includes a multiple-nest capability,
nonhydrostatic dynamics, which allows the model
to be used at a few-kilometer scale, multitasking
capability on shared- and distributed-memory
machines, a four-dimensional data-assimilation
capability, more physics options.
4
Mesoscale Model 5
MM5 generates meteorological fields -
horizontal and vertical wind components, -
pressure, - temperature, - air humidity, -
cloudiness and precipitation parameters, - heat,
moisture and momentum fluxes, - short-wave and
long-wave radiation.
5
Mesoscale Model 5
Modeling system MM5 includes a lot of
parameterization schemes of subgrid physical
processes, which are chosen in correspondence
with scales of investigated processes - 8
cumulus parameterization - 7 PBL schemes - 5
radiation schemes - 8 explicit moisture
schemes - 4 surface schemes.
6
The Weather Research and Forecast Model is a
next-generation mesocale numerical weather
prediction system designed to serve both
operational forecasting and atmospheric research
needs. It features multiple dynamical cores, a
3-dimensional variational (3DVAR) data
assimilation system, and a software architecture
allowing for computational parallelism and
system extensibility. The WRF model is a fully
compressible, nonhydrostatic model. Its vertical
coordinate is a terrain-following hydrostatic
pressure coordinate. Model uses the Runge-Kutta
2nd and 3rd order time integration schemes, and
2nd to 6th order advection schemes in both
horizontal and vertical directions. The dynamics
conserves scalar variables.
7
The WRF model is designed to be a flexible,
state-of-the-art atmospheric simulation system
that is portable and efficient on available
parallel computing platforms. WRF is suitable for
use in a broad range of applications across
scales ranging from meters to thousands of
kilometres, including - Idealized simulations
(e.g. LES, convection, baroclinic waves) -
Parameterization research - Data assimilation
research - Forecast research - Real-time NWP -
Coupled-model applications - Teaching
8
WRF includes a lot of physic options, which can
be combined. Options are varied from simple and
effective to complicate, required additional
computations - 8 schemes of microphysics
(Kessler, Lin, NCEP simple ice, NCEP mixed phase,
Eta mycrophisics, ...) - 3 schemes of convection
(KF, BMJ, New KF) - 2 schemes of long-wave
radiation (RRTM, ETA GFDL) - 3 schemes of
short-wave radiation (Dudhia, Goddard, ETA
GFDL) - 3 schemes of surface layer (none,
Monin-Obukhov, MYJ) - 3 schemes of land-surface
parameterization (simple, OSU, ...) - 3 schemes
of PBL (MRF, MYJ) - 2 schemes of subgrid
diffusion parameterization
9
MM5 WRF
Since the MM5WRF modeling system are primarily
designed for real-data studies/simulations, it
requires the following datasets to run -
Topography, landuse and vegetation (in
categories) (1o - 30 resolution) - Gridded
atmospheric data that have at least these
variables sea-level pressure, wind,
temperature, relative humidity and geopotential
height and at these pressure levels surface,
1000, 850, 700, 500, 400, 300, 250, 200, 150, 100
mb - Observation data that contains soundings
and surface reports (final analysis data NCEP or
ECMWF, global data NCEP)
10
Simulation cases
  • Two temporal periods 16-17 May 2004 20-21
    October 2004
  • Three local nested domains with horizontal sizes
    450?450, 150?150 ? 50?50km2. South of Western
    Siberia, Tomsk (56,5o N, 85o E) is in the centre
    of domains
  • Initial state of atmosphere and lateral boundary
    conditions were set up on the basis of NCEP final
    analysis data

11
Simulation conditions
D1
D1
D2
D2
D3
Tomsk
D3
Kemerovo
Kemerovo
Novosibirsk
Novosibirsk
Three nested domains D1, D2, D3 and distribution
of landuse categories
12
Simulation options
MM5
WRF
  • Grids 52?52?31 for domains D1, D2, D3
  • Horizontal resolution 9 3 1 km for D1, D2, D3
  • Temporal step 27 9 3 sec for D1, D2, D3
  • Vertical size of domains 17km
  • Cluster IAO SB RAS
  • Grids 52?52?31 for domains D1, D2, D3
  • Horizontal resolution 9 3 1 km for D1, D2, D3
  • Temporal step 60 30 10 sec for D1, D2, D3
  • Vertical size of domains 17 km
  • Cluster IAO SB RAS

13
Simulation options
MM5
WRF
  • Mixed phase microphysics by Reisner
  • RRTM scheme for long wave radiation
  • Similarity theory for surface layer
  • Thermal diffusion for soil
  • Blackadar scheme for PBL
  • None cumulus parametrization
  • Eta Grid-Scale Cloud and Precipitation scheme by
    Ferrier
  • RRTM scheme for long wave radiation
  • Dudhia scheme for short wave radiation
  • Similarity theory for surface layer
  • Thermal diffusion for soil
  • MYJ scheme for PBL

14
Comparison of the models
MM5 WRF
Time-200 16 May 2004 Time 024 17 May 2004
Wind velocity and direction at 10m Air
temperature at 2m in Tomsk
15
Wind at 10m for the domain D1
MM5
WRF
16
Wind at 10m for the domain D1
MM5
WRF
17
Air temperature at 2m for D1
MM5
WRF
18
Vertical distribution of air potential temperature
MM5
WRF
17 May 2004, 1400 LST, Domain D1
19
Vertical distribution of air absolute humidity
MM5
WRF
17 May 2004, 1400 LST, Domain D1
20
Wind at 10m for the domain D3
MM5
WRF
21
Wind at 10m for the domain D3
MM5
WRF
22
Comparison of the models
Time-200 20 October 2004 Time 024 21
October 2004
MM5 WRF
Wind velocity and direction at 10m Air
temperature at 2m in Tomsk
23
Wind at 10m for the domain D1
MM5
WRF
24
Wind at 10m for the domain D1
MM5
WRF
25
Wind at 10m for the domain D3
MM5
WRF
26
Wind at 10m for the domain D3
MM5
WRF
27
Generation of cloudness
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Parallel realization of the models
  • Linux cluster IAO
  • 10 nodes, each with 2 processors Pentium III 1GHz
    and RAM 1Gb
  • Communication net 1Gbs Ethernet, star topology
  • 11Gflops on the LINPACK test

MM5 80Mb, WRF 210Mb
54
Ozone concentration, measured by TOR-station IAO
near Tomsk on 16 May 2004
O3, mkg/m3
55
Generic Reaction Set kinetic scheme of ozone
formation
  • Rsmog hv gt RP Rsmog ?APM
  • RP NO gt NO2
  • NO2 hv gt NO O3
  • NO O3 gt NO2
  • RP RP gt RP ?H2O2
  • RP NO2 gt SGN
  • RP NO2 gt APM
  • RP SO2 gt APM
  • H2O2 SO2 gt APM
  • O3 SO2 gt APM

56
Air pollution in Tomsk
Time-200 16 May 2004 Time 024 17 May 2004
57
Conclusion
  • Results of application of mesoscale models MM5
    and WRF for investigation of regional and local
    atmospheric processes over Western Siberia and
    Tomsk Region were presented.
  • A comparison with observation data on 16-17 May
    2004 and on 20-21 October 2004 shows a
    possibility of application of these models for
    solution of air quality problems and an
    atmospheric research. But additional testing of
    MM5 and WRF is necessary to select more
    appropriate land-surface parametrization options.
  • Research is funded by RFBR, grant N 04-07-90219.
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