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Transcript of Introduction to parametrization Introduction to Parametrization of Sub-grid Processes Anton Beljaars...
Introduction to parametrization
Introduction to Parametrization of Sub-grid Processes
Anton Beljaars
([email protected] room 114)
• What is parametrization?
• Processes, importance and impact.
• Testing, validation, diagnostics
• Parametrization development strategy
Introduction to parametrization
Why parametrization
•Small scale processes are not resolved by large scale models, because they are sub-grid.•The effect of the sub-grid process on the large scale can only be represented statistically. •The procedure of expressing the effect of sub-grid process is called parametrization.
Introduction to parametrization
•The standard Reynolds decomposition and averaging, leads to co-variances that need “closure” or “parametrization”
•Radiation absorbed, scattered and emitted by molecules, aerosols and cloud droplets play an important role in the atmosphere and need parametrization.
•Cloud microphysical processes need “parametrization”
•Parametrization schemes express the effect of sub-grid processes in resolved variables.•Model variables are U,V,T,q, (l,a)
What is parametrization and why is it needed
Introduction to parametrization
Reynolds decomposition
e.g. equation for potential temperature:
)(2
2
2
2
2
2
zyxQ
xw
yv
xu
t
advection source molecular diffusion
Reynolds decomposition:'.,'
,','
wwW
vvVuuU
Averaged (e.g. over grid box):
)''()''()''(z
wzy
vyx
ux
Q
xw
yv
xu
t
: source term (e.g. radiation absorption/emission or condensation)Q
''w : subgrid (Reynolds) transport term (e.g. due to turbulence, convection)
Introduction to parametrization
Space and time scales
Introduction to parametrization
Space and time scales
1 hour100 hours 0.01 hour
Introduction to parametrization
• Climate models 200 km 500 m 100 years• Global weather prediction 20 km 200 m 10 days • Limited area weather pred. 10 km 200 m 2 days• Cloud resolving models 500 m 500 m 1 day• Large eddy models 50 m 50 m 5 hours
Hor. scales Vert. Scales time range
Different models need different level of parametrization
Numerical models of the atmosphere
Introduction to parametrization
Parametrized processes in the ECMWF model
Introduction to parametrization
Applications and requirements
• Applications of the ECMWF model– Data assimilation T1279L91-outer and T95/T159/T255-inner loops: 12-hour
4DVAR.– Medium range forecasts at T1279/L91 (16 km): 10 days from 00 and 12 UTC.– Ensemble prediction system at T639L62 (32 km) for 10 days, and T319 (65
km) up to day 15; 2x(50+1) members. – Short range at T1279L91 (15 km): 3 days, 4 times per day for LAMs.– Seasonal forecasting at T95L40 (200 km): 200 days ensembles coupled to
ocean model.– Monthly forecasts (ocean coupled) at T159L61: Every week, 50+1 members.– Fully coupled ocean wave model.– Interim reanalysis (1989-current) is under way (T255L60, 4DVAR).
• Basic requirements– Accommodate different applications. – Parametrization needs to work over a wide range of spatial resolutions.– Time steps are long (from 10 to 60 minutes); Numerics needs to be efficient
and robust. – Interactions between processes are important and should be considered in the
design of the schemes.
Introduction to parametrization
Importance of physical processes
•General
•Tendencies from sub-grid processes are substantial and contribute to the evolution of the atmosphere even in the short range.
• Diabatic processes drive the general circulation.
•Synoptic development
•Diabatic heating and friction influence synoptic development.
•Weather parameters
•Diurnal cycle
•Clouds, precipitation, fog
•Wind, gusts
•T and q at 2m level.
•Data assimilation
•Forward operators are needed for observations.
Introduction to parametrization
Global energy and moisture budgetsEnergy
Net atmospheric radiative heating
Heating due to latent heat release
Surface sensible heat flux
Horizontal energy flux divergence
a a
a
a
R LP SH FRLPSHF
Moisture
5 mm/day
=P-E
Runofff
Hartman, 1994. Academic Press. Fig 6.1 and 5.2
Introduction to parametrization
Sensitivity of cyclo-genesis to surface drag
control Pcentre=918 hPa
analysis Pcentre=925 hPa difference
1.2 DC Pcentre=923 hPa
Introduction to parametrization
T-tendencies
Introduction to parametrization
T-Tendencies
Introduction to parametrization
T-Tendencies
Introduction to parametrization
T-Tendencies
Introduction to parametrization
T-tendencies
Introduction to parametrization
T-Tendencies
Imbalance (physics – dynamics) due to: (a) Fast adjustment to initial state (“data assimilation problem”); (b) Parametrization deficiencies
Introduction to parametrization
Validation and diagnostics
•Compare with analysis
•daily verification
•systematic errors e.g. from monthly averages
•Compare with operational data
•SYNOP’s
•radio sondes
•satellite
•Climatological data
•CERES, ISCCP
•ocean fluxes
•Field experiments
•TOGA/COARE, PYREX, ARM, FIFE, ...
Introduction to parametrization
Day-5, T850 errors
Viterbo and Betts, 1999. JGR, 104D, 27,803-27,810
Introduction to parametrization
History of 2m T-errors over Europe in the ECMWF model
(step60/72)
•Model temperature errors are influenced by many processes. •Observations at process level are needed to disentangle their effect
Bias (day/night)
RMS (day/night)
LESS STABLE BL DIFFUSION
Introduction to parametrization
TSR: JJA 24 hour forecasts (CY31R1/23R4 - CERES)
CY31R1 - CERES
CY23R4 - CERES
Introduction to parametrization
Lat. Heat Flux-DJF (ERA_40_Step_0_6 vs. DaSilva climatology)
ERA40 model
Introduction to parametrization
PYREX experiment
Introduction to parametrization
PYREX mountain drag (Oct/Nov 1990)
Lott and Miller, 1995. QJRMS, 121, 1323-1348
Introduction to parametrization
Latent heat flux: ERA-40 vs. IMET buoy
Introduction to parametrization
Cloud fraction (LITE/ECMWF model)
Model
LITE
Cross section over Pacific 45N/120E – 45S/160W (16-09-1994)
Introduction to parametrization
Parametrization development strategy
-Invent empirical relations (e.g. based on theory, similarity arguments or physical insight)
To find parameters use:
–Theory (e.g. radiation)
–Field data (e.g. GATE for convection; PYREX for orographic drag; HAPEX for land surface; Kansas for turbulence; ASTEX for clouds; BOREAS for forest albedo)
–Cloud resolving models (e.g. for clouds and convection)
–Meso scale models (e.g. for subgrid orography)
–Large eddy simulation (turbulence)
–Test in stand alone or single column mode
–Test in 3D mode with short range forecasts
–Test in long integrations (model climate)
–Consider interactions
Introduction to parametrization
Measure diffusion coefficients
)/(*
Lz
zuK
mm
stableunstable
Lz /
m
Introduction to parametrization
Convert to empirical function
Diffusion coefficients based on Monin Obukhov similarity:
2
2 )(
''
z
U
z
gRi
Riflz
UK
zKw
Operational CY30R2
MO-scheme (less diffusive)
Operational CY30R2
MO-scheme (less diffusive)
Introduction to parametrization
Column test
Cabauw: July 1987, 3-day time series Observations versus model (T159, 12-36 hr forecasts)
Introduction to parametrization
Test in 3D model: Data assimilation + daily forecasts over 32 days March 2004
Effect of MO-stability functions
Introduction to parametrization
Concluding remark
Enjoy the course
and
Don’t hesitate to ask questions