Ensemble Data Assimilation at DWD - University of Bonn...Ensemble Data Assimilation at DWD System...
Transcript of Ensemble Data Assimilation at DWD - University of Bonn...Ensemble Data Assimilation at DWD System...
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Ensemble Data Assimilation at DWD
System and Selection of Research Projects
Andreas Rhodin,
Ana Fernandez,
Roland Potthast,
Christoph Schraff,
Hendrik Reich,
Harald Anlauf,
Anne Walter,
Alex Cress,
u.v.m
DWD, Germany & University of Reading, UK
Bonn Sept 2016
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Global NWP Modelling
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ICON Model 13km + Nest over Europe (6.5km)
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3
4. ICON Ensemble Datenassimilation
We are running ICON EDA in our
Routine since Jan 2016
• 40 Members each with 40km global
resolution and 20km NEST over Europe
• 1 deterministic 13km member
• EPS forecasts 40 Members 7 Days + 1
Deterministic
• Output for convective-scale EDA/EPS
• Hybrid System
Grafics by ICON EDA Head
Dr. Andreas Rhodin, FE12
Operational since January 2016 : Rhodin, Fernandez, Cress, Anlauf, etc.
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Roland Potthast
ICON EnVar
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Roland Potthast
ICON EnVar
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Hybrid Methods: EnVAR Scores
ICON EDA
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Hybrid Methods: EnVAR Scores
ICON EDA
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Particle Filter
• Localized version of Particle Filter Classical Particle Filter PF and Localized Markov Chain Particle Filter LMCPF
(See book of Nakamura and Potthast)
• Hybrid Ensemble Var Particle Filter Particle filter coupled with Variational Method (3D-VAR)
Global NWP with ICON Model 40 Particles 40km global resolution, Deterministic run 13km
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You get a prior distribution p(x) by some prior ensemble
Measurements define a data distribution p(y|x)
Bayes theorem defines a posterior distribution by
p(x|y) = c p(x) p(y|x)
The core game is how to get an analysis ensemble from p(x|y).
Particle Filter
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PRIOR
DATA
Posterior
Analysis
Ensemble
BAYES Data Assimilation
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Following the LETKF philosophy
Replacing the LETKF square root filter by a particle selection which works for non-Gaussian distributions
Localizing the EDA part in Observation space
Localizing the coupled variational part in state space.
Using standard tools for spread control from EnKF, i.e. multiplicative and additive covariance inflation, relaxation towards prior perturbations, …adaptively.
Preventing particle filter collapse by a pseudo-random draw in each analysis step around the particles with non-zero weight.
Particle Filter Details
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Roland Potthast 2016
EnKF T on level 85
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Roland Potthast 2016
PF T on level 85
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
TEMP T 3h, 5 days
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
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Roland Potthast 2016
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Summary
• Implemented a localized particle filter for the ICON EDA global assimilation
• Implemented a hybrid EnVar Particle Filter for the deterministic run • Testing the system in a case study • In principle we see that the system is functioning • The behaviour of the forecasts in the case study was useful • The 3h o-f scores of the PF were worse than for the LETKF • The 3h o-f scores of the Hybrid PF were better than for the EnVAR • The forecasts scores were comparable between EnVar-LETKF and
EnVar-PF, the comparison is not yet significant • We need some adaptive spread control in our particle filter, this is
ongoing work. • Further studies and investigation of many details are ongoing.
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Convective Scale EDA
Use an approprite fast update cycle (e.g. 1h)
Deliver probabilistic (pdf) rather than
deterministic forecast
Need ensemble forecast and ensemble data
assimilation system
http://opt-prod.s3.amazonaws.com/traject/files/content_items/relateds/000/045/077/original/5272aa3d07121c9422d6af52-convection_20in_20atmosphere.jpg?1446064102
Roland Potthast - September 2016
Convection-permitting NWP: Convection!
Fast processes, a few hours is „long term“!
Much uncertainty in processes, surface, physical
parametrizations
High-resolution data needed, indirect measurements,
sparse data not resolving all processes
Strong non-linearities in the processes
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Convective Scale EDA
Goal is the prediction of convection and subsequent precipitation,
here model grid (left) and upscaled probability (right)
(Courtesy: FE15)
Upscaling/downscaling of statistics is non-trivial! Roland Potthast - September 2016
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Convective Scale EDA
Design of a convective scale EDA System
(Image: A. Rhodin and C. Schraff)
Roland Potthast - September 2016
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Convective Scale EDA+EPS Design of a convective scale EPS System 1
LBC + IC + Physics
ICON, IFS, GFS, GSM
perturb.
COSMO-DE EPS
Construction of atmospheric Probability Distribution by very different Perturbation Techniques
Roland Potthast - September 2016
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Convective Scale EDA+EPS
Design of a convective scale EPS System 2
LBC + IC + Physics
ICON EPS
perturb.
COSMO-DE EPS
Construction of atmospheric Probability Distribution by very different Perturbation Techniques
Roland Potthast - September 2016
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Convective Scale EDA
Snow Analysis Deterministic analysis The snow analysis for COSMO-DE deterministic runs every 6 hours using observations from snow depth, precipitation combined with 2m temperature, and weather observations ww to analyse snow depth. Background field is the previous analysis. Ensemble system For the ensemble system no explicit snow depth perturbations are applied, differences result from free running snow variables for each member. The ensemble is adjusted after each deterministic analysis to ensure the ensemble mean matches the deterministic analysis. Collocation Method with radial basis functions = Cressman Method, Successive Correction
http://media.gettyimages.com/videos/high-angle-wide-shot-time-lapse-clouds-moving-across-the-snow-covered-video-id996-6?s=640x640
NOAA snow depth analysis previous day Roland Potthast - September 2016
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Convective Scale EDA
Sea Surface Temperature (SST) Deterministic System SST analysis for COSMO-DE deterministic runs daily at 0:00 UTC using background fields from ICON which are based on NCEP input data. Sea ice is updated using the BSH ice mask.
Ensemble System The SST analysis for the ensemble system is based on the analysis from COSMO-DE deterministic. Perturbations are generated by a stochastic method with random perturbations and a localization based on Gaspari Cohn functions.
Roland Potthast - September 2016
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Convective Scale EDA Sea Surface Temperature (SST) and Soil Moisture (w_SO) Perturbations Random algorithm with two scales Surface temperature differences from soil moisture perturbations and model
dynamics
Difference Member 3 – Mean (left) or Member 1 – Mean (right) of T_SO Roland Potthast - September 2016
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Convective Scale EDA Sea Surface Temperature (SST) and Soil Moisture (w_SO) Perturbations Random algorithm with two scales Surface temperature differences from soil moisture perturbations and model
dynamics
Difference Member 3 – Mean (left) or Member 1 – Mean (right) of W_SO Roland Potthast - September 2016
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Hourly Analysis of Atmospheric Fields No Soil-Moisture Analysis, but hourly soil-
moisture perturbations (with spread control) and relaxation of soil moisture towards the deterministic run
Snow Analysis every 6 hours at 0, 6, 12, 18 UTC
SST once per day at 0 UTC
EDA Component Schedule
Roland Potthast - September 2016
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Distributions EPS Members
Histogram T50 Full temperature Distribution Of COSMO Model, 1 time slice
Histogram ΔT50 With subtraction of mean for each point
Roland Potthast - September 2016
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• Talagrand Rank Histogram
• Checks the distribution of observations compared with the distribution of the ensemble
Distributions EPS Members
T2m is underdispersive
ensemble
obs
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Verification Scores Survey
Upper Air Verification
Surface Verification
Precipitation Verification
Satellite Data Verification
Scores Metrics Bias Field Properties Spectral Distributions
Roland Potthast - September 2016
High Impact Weather Verification
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Verification Scores Survey 1
bias RMSE
Nudging + LHN vs. LETKF + LHN
T [K] RH wind [m/s]
bias RMSE RMSE RMSE
Verification of 6-h forecasts against radiosondes , 28 days (18.05. – 15.06. 2014)
Roland Potthast - September 2016
(Courtesy: C. Schraff and H. Reich)
LETKF: smaller wind errors, larger humidity errors
LEKTF less able to correct (model) biases
Temperature neutral
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Verification Scores Survey 2
KENDA: neutral (similar results for convective period)
reduction of variance [%] rmse
pre
ssu
re [h
Pa
]
KENDA-LETKF vs. nudging rmse
(averaged over
lead times &
initial times) T
wind speed
wind direct.
RH Differences are not significant Differences are
not significant
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Verification Scores Survey 3 p
ressure
[hP
a]
KENDA-LETKF vs. nudg./multi-model CRPS
(averaged over
lead times &
initial times) T
zonal wind
merid. wind
RH
(Courtesy: C. Schraff and H. Reich)
Roland Potthast - September 2016
KENDA: much
better CRPS
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Verification Scores Survey 4 le
ad
tim
e [h
]
KENDA-LETKF vs. nudg./multi-model
Roland Potthast - September 2016
KENDA: much better
CRPS in all variables
except surface pressure
(Courtesy: C. Schraff and H. Reich)
CRPS
(averaged over
lead times &
initial times)
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Verification Scores Survey 5
Roland Potthast - September 2016
28 days 18.05. –
15.06.
2014
with LHN: small difference in first 4 hours due to dominating
influence of LHN, thereafter, advantage of KENDA over nudging tends
to be larger than without LHN
1 mm/h
0-UTC
runs
12-UTC
runs
0.1
mm/h
1-hrly
precip
FSS
( 30 km )
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Verification Scores Survey 6
Roland Potthast - September 2016
0-UTC runs
12-UTC runs
Brier skill score , 14 m/s spread / rmse
10-m wind gusts
KENDA: better spread + skill + BSS (for 14 m/s + 18 m/s, due to improved reliability)
KENDA-LETKF nudg./multi-model
(Courtesy: C. Schraff and H. Reich)
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Convective Scale EDA
Roland Potthast - September 2016
• Observe!
RADAR Reflectivity
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GPS/GNSS Tomography
GNSS (GPS) Slant Path Delay : humidity integrated over path
from ground station to GNSS (GPS) satellite, all weather obs
(45) GPS obs from 1 station / 9 satellites in 15 min.
many stations 3-D information on humidity, but !
at 5° (7°), path reaches height of 10 km at ~ 100 (80) km distance
vert. + horiz. non-local obs (not point measurements)
Roland Potthast - September 2016
(Courtesy: M. Bender, A. Rhodin, C. Schraff, R. Potthast)
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GPS/GNSS Tomography
Slant Total Delay :
humidity integrated over path
from ground station to satellite
elevation angles 90° - 5
vert. + horiz. non-local obs
difficult to use in LETKF:
explicit localization (doing separate analysis at every analysis grid point,
select only obs in vicinity and scale R-1)
analysis grid points
used obs
discarded obs
non-local obs
(Courtesy: Michael Bender, Rhodin, Schraff) Roland Potthast - September 2016
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GPS/GNSS Tomography
8 days 17. – 24.06.
2014
spread reduced particularly in lower atmosphere
RH -TEMP T -AIREP wind -AIREP
spread
LETKF settings:
• STD localised 1000 m above the GNSS station
• vertical localisation length : 125 hPa ≈ 1000 m (v_loc = 0.15)
• horizontal localisation length : 30 km (h_loc = 30)
(Courtesy: M. Bender, A. Rhodin, C. Schraff, R. Potthast) Roland Potthast - September 2016
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GPS/GNSS Tomography
8 days 17. – 24.06.
2014
RH -TEMP T -AIREP wind -AIREP
std dev
low level degraded
upper levels improved
T –AIREP
bias
(Courtesy: M. Bender, A. Rhodin, C. Schraff, R. Potthast) Roland Potthast - September 2016
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GPS/GNSS Tomography
1-hrly precip
FSS ( 30 km )
8 days 17 – 24 May 2014
0.1 mm/h
0.1 mm/h : slightly worse for 0-UTC runs, slightly better for 6-, 18-UTC runs
CONV only CONV + GNSS CONV + LHN CONV + LHN + GNSS
(Courtesy: M. Bender, A. Rhodin, C. Schraff, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
Roland Potthast - September 2016
• Observe!
RADAR Reflectivity
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Convective Scale EDA
51
• mature convection: precipitation
radar: 3-dim. reflectivity
3-dim. radial velocity
Therea Bick left Axel Seiffert
Elisabeth Bauernschubert (DWD/IAFE),
Virginia Poli (ARPAE): (1 week DA exp).
Assimilation of Radial Velocities Based on the Ensemble Data Assimilation KENDA
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
1-hrly precip
FSS ( 30 km ) 12-UTC forecast runs
2 mm/h
8 days 21 – 29 May 2014
0.1 mm/h
CONV only CONV + RAD Vr RAD Vr only
preliminary tuning experiments (4 radars used)
moderate sensitivity, optimal values: obs error 3 m/s (better than 5 m/s),
superobbing 10 km (5 km, 20 km), horizontal localisation 32 km (16 km)
generally positive impact on first few hours of forecasts (upper-air + surface verif)
CONV only CONV + RAD Vr RAD Vr only
• only 1 radar used (Boostedt in Northern Germany)
• obs error 5 m/s, superobbing 10 km, h-loc 16 km
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
1-hrly precip
FSS ( 30 km ) 12-UTC forecast runs
2 mm/h
8 days 21 – 29 May 2014
0.1 mm/h
CONV only CONV + RAD Vr RAD Vr only
preliminary tuning experiments (4 radars used)
moderate sensitivity, optimal values: obs error 3 m/s (better than 5 m/s),
superobbing 10 km (5 km, 20 km), horizontal localisation 32 km (16 km)
generally positive impact on first few hours of forecasts (upper-air + surface verif)
CONV only CONV + RAD Vr RAD Vr only
• only 1 radar used (Boostedt in Northern Germany)
• obs error 5 m/s, superobbing 10 km, h-loc 16 km
(Courtesy: Bauernschubert, K. Stephan, C. Schraff, H. Reich, R. Potthast) Roland Potthast - September 2016
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Convective Scale EDA
Convective Scale Data Assimilation is a key challenge for the upcoming years
We need Algorithms to deal with Uncertainty, Nonlinearity, Predictability Questions
We need many temporally and spatially high-resolution observations
We need to bring together process understanding and measurement data
Within an Integrated Forecasting System we merge Nowcasting and NWP
Roland Potthast - September 2016
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Many Thanks!
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Spread EnKF T on level 85
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Spread PF T on level 85
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Roland Potthast 2016
Ens 01-Mean, PF T 90
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Roland Potthast 2016
Ens 01-Mean, EKF T 90
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Roland Potthast 2016
Ens 01- Ens 01, PF1 vs PF2 T 90