Atmospheric Composition Data Assimilation: Selected topics(Robichaud et al. 2015, Air Qual Atmos...
Transcript of Atmospheric Composition Data Assimilation: Selected topics(Robichaud et al. 2015, Air Qual Atmos...
Atmospheric Composition Data Assimilation:
Selected topics
Richard Ménard, Martin Deshaies-Jacques Air Quality Research Division, Environment and Climate Change Canada
Simon Chabrillat, Quentin Errera, and Sergey Skachko Belgium Institute for Space Aeronomy
International Symposium on Data Assimilation, Munich , March 2018
Atmospheric composition : A strongly constrained system
• Coupling with the meteorology is in each 3D grid volume
(winds, temperature, humidity, clouds/radiation)
• Chemical solution is also controlled by chemical sources and sinks
Boundary layer O3
Forecast verification after O3 assimilation
no O3 assimilation
with O3 assimilation
bia
s
sta
ndard
devia
tion
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Atmospheric composition
as a slaved /controlled system
• As coupled system have to consider the Information content:
– Chemical model
– Chemical observations
– Meteorology
• Favors online chemistry-meteorology models
• No for Incremental formulation with a lower resolution chemistry
• Because the control of meteorology on chemistry is so strong,
the feedback of chemistry on meteorology is small
• Except for long-lived species, chemical forecast is not the most
useful product, but analyses are
• Forecast improvement is better addressed with parameter
(e.g. sources) estimation
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Notation and definitions
Continuity equation; dry air density
Eulerian0)(;Lagrangian01
VV
tDt
D
Mixing ratio ci of constituent i is defined as
iic
Eulerian0;Lagrangian0
i
ii ct
c
Dt
DcV
The consistency between the wind field V used for the continuity equation and
the wind field V used for the transport of the constituent i is called the mass consistency
CTM (Chemical Transport Models) are offline (from meteorology) models that uses
different V and often at different resolution: they were introduced to use met analyses
Online chemical models have mass consistency and same resolution as the meteorology
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GEM-BACH online with meteo model /
BASCOE CTM offline model driven by 6-hourly meteorological analyses
TOMS
observation
CTM-BIRA
4DVar assim
resolution
3.75º x 5º
CTM-BIRA
simulation
1.875º x 2.5º
Online
GEM-BIRA
simulation
1.5º x 1.5º
Total column ozone (DU) for September 30th, 2003: Grey areas represent pixels where the ozone column is smaller than 100 DU.
Validation with MIPAS OFL 20030825-20030904, 60°N-90°N
BASCOE CTM, ECMWF (d2003G)
BASCOE CTM, EC 3D-VAR (v3s85)
GEM-BACH, EC 3D-VAR (K3BCS304)
GEM-BACH, EC 4D-VAR (K4BCS304)
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Coupled Assimilation
O3/meteorology
Assimilation of limb sounding
MIPAS observations of O3
with AMSU-A
MIPAS vertical resolution 1-3 km
solid lines
no radiation feedback
dashed lines
assim O3 used in radiative
scheme (k-correlated method)
de Grandpré et al., 1997, MWR
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Operational air quality analysis
experimental since 2002, operational since Feb 2013
ozone fine particles
Analysis of O3, NO2, SO2, PM2.5, PM10 each hour
History
• O3, PM2.5 – using CHRONOS
2002-2009
• O3, PM2.5 – using GEM-MACH
2009-2015
• O3, PM2.5 , NO2, SO2, PM10
since April 2015
(Robichaud et al. 2015,
Air Qual Atmos Health)
• Multi-year data set (2002-2012)
Robichaud and Ménard 2014, ACP)
What does the medicine has to say about air pollution ? • Interact with many groups (e.g. Health Canada, Environmental Cardiology )
• In terms of mass, we breathe-in
per day about 20 kg of air,
2 kg of liquid
and 1 kg of solid food
12-25 breath per minutes each is about 1 liter
≈ 20,000 liter of air/day
• Pulmonology and cardiology
are strongly linked
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Mean 15 mg/m3
Sun et al., JAMA 2005
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Canadian Census Health and Environmental Cohort
(CanCHEC) and the Canadian Urban Environmental
Health Research Consortium (CANUE)
www.canue.ca
Brook et al. BMC Public Health (2018) 18:114
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Evaluation of analysis
by cross-validation
(or leave-out observations)
Ménard, R and M. Deshaies-Jacques Part I: Using verification metrics. Atmosphere 2018, 9(3), 86,
doi:10.3390/atmos9030086
Ménard, R and M. Deshaies-Jacques Part II: Diagnostic and optimization of analysis error covariance.
Atmosphere 2018, 9(2), 70; doi:10.3390/atmos9020070
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3 spatially random distributed set of observations
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)),(var(
)),(var(
)),(var(
213
312
321
OOAO
OOAO
OOAO
))(var(
))(var(
))(var(
33
22
11
OAO
OAO
OAO
Passive /independent obs.
Active obs.
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Estimation of error covariances in observation space
(HBHT , R)
Theorem on estimation of error covariances in observation space
Assuming that observation and background errors are uncorrelated,
the necessary and sufficent conditions for error covariance estimates to be
equal to the true observation and background error covariances are:
yconsistenc covariance InnovationBOBO TTRHBH~~
]))([()1 E
A scalar version of this condition is
pTTT Ntrtr ][])
~~([)
~~(][ 211 EEE dRHBHdRHBHdd
or
2/min pNJ
conditiongain Kalman TheKHHK~
)2
Ménard, 2016, QJRMS
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conditiongain Kalman TheKHHK~
)2
Diagnostic of the Kalman gain condition
• Daley 1992 (MWR) suggested that the time lag-innovation covariance
to be equal zero (assuming observation errors are serially uncorrelated)
• Here we suggest to use cross-validation
Simple interpretation with a scalar problem
1) Innovation consistency says that the sum of observation and background
error variances is the sum of the true error variances
2) Kalman gain condition says that the ratio of observation to background
error variance is the ratio of the true error variances
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17
Hilbert spaces of random variables
Define an inner product of two (zero-mean) random variables X , Y as
YXY,X E
Can defined a metric as
2
2XX E
Verification of analysis by cross-validation:
A geometric view
Uncorrelated random variables X , Y would be orthogonal 0Y,X
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Verification of analysis by cross-validation:
A geometric view
TTBOBO HBHR ]))([(E
0])([ Toc
o E
0H ])([ Tfo E
0Η ]))([( Toc
ac E
obs and background errors are uncorrelated
active and independent obs. errors are uncorrelated
0H ])([ Toc
f E
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Verification of analysis by cross-validation:
A geometric view
Tccc
Tcc AOAO AHHR ])()[(E0Η ]))([( To
ca
c E
true measure of the analysis error covariance
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Verification of analysis by cross-validation:
A geometric view c
by varying the observation weight while
we can find a true optimal analysis
TTBOBO HBHR ]))([(E
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Verification of analysis by cross-validation:
A geometric view
THL
TAOAO HAHR ˆ])ˆ)(ˆ[( E
Hollingsworth-Lönnberg 1989
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Verification of analysis by cross-validation: A geometric view
TMDJ
TTBABA HAHHBH ˆ])ˆ)(ˆ[( E
Ménard-Deshaies-Jacques 2018
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Verification of analysis by cross-validation:
A geometric view
TD
TBAAO HAH ˆ])ˆ)(ˆ[( E
Desroziers et al. 2005
Geometrical proof given in
Ménard and Deshaies-Jacques 2018
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Verification of analysis by cross-validation:
A geometric view
TcMDJc
Tcc
Tcc BABA HAHBHH ˆ])ˆ()ˆ[( E
Diagnostic in passive observation space we get
The yellow triangle we have
])ˆ()ˆ[(
])ˆ()ˆ[(])()[(
Tcc
Tcc
Tcc
AOAO
BABABOBO
E
EE
and using we get the relation above
cTcc
Tcc
cTcc
Tcc
BOBO
AOAO
RBHH
RHAH
])()[(
ˆ])ˆ()ˆ[(
E
E
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Experiment cL (km) 2)( BO 22 ˆ/ˆˆbo
2ˆo 2ˆ
b pN/2
O3 iter 0 124 101.25 0.22 18.3 83 2.23
O3 iter 1 45 101.25 0.25 20.2 81 1.36
1
Experiment Passive
)ˆ( TcMDJcdiag HAH
Passive 2])ˆvar[( occAO
O3 iter 0 26.03 32.72
O3 iter 1 28.95 28.75
Experiment Active
)ˆ( TMDJdiag HAH
Active
)ˆ( TDdiag HAH
Active
)ˆ( THLdiag HAH
Active
)ˆ( TPdiag HAH
O3 iter 0 22.69 9.61 -6.03 5.77
O3 iter 1 13.32 13.68 8.94 11.60
Input error statistics
Estimate of analysis error variance at passive observation sites
Estimation of active analysis error variance
Application to O3 surface analysis
iter 0 (first guess error correlation)
Iter 1 (Maximium Likelihood estimation of correlation length)
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Verification of analysis by cross-validation:
when active observation and background errors are correlated
1)()(
])([
HXHXRHBHXBHHHxHx
X
TTTTfa
Tof E
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1222 )2()()-(
X
obobobb
ob
BA
The HL and MDJ diagnostic continue to be valid
but not the D diagnostic
Verification of analysis by cross-validation:
when active observation and background errors are correlated
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)()-(
/when
)()-(
0Xwhen
o
BOBA
BOBA
b
T
O
o
b B
q
b
o
q cos
Verification of analysis by cross-validation:
when active observation and background errors are correlated
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Lognormal
Kapteyn’s analogue machine, replicate
)1(1 iii XX
where i is simply specified by
Huize de Wolf laboratory University of Groningen
2/1)(
2/1)(
aP
aP
i
i
Simple model: Random proportional tendencies
11
ii
ii ct
cc
where is random parameter. Suppose we
divide a time inverval [0,1] into K intervals
K
ii
K
i i
ii tc
cc
11 1
1
t
)(log)(log 0
)(
)(1 1
1
0
tctcc
dc
c
ccK
tc
tc
K
i i
iiK
we can approximate
and by central limit theorem
),(~1 2
11
m NK
KttK
ii
K
ii
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),(~)(
)(log 2
0
mNtc
tc K
then
),(~)(
)( 2
0
mLNtc
tc K
is lognormally-distributed.
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Letting w = log c , the analysis equation is then of the form
)( bHwwKww fofa
1 oTfTf
BHBHHBK
where the s are the error covariances defined in log space.
b is an observational correction, and has different form whether we consider that:
a) the measurement in log space that is unbiased (in which case b = 0)
b) the measurement in physical space is unbiased
2/iii Bb
Transformation of mean and covariance between log and physical quantities
1)exp(
2
1exp
ijjiij
iiii
BccP
Bwc
31
Analysis step
Positive analysis (lognormal formulation) (Cohn 1997, Fletcher and Zupanski 2006 )
B
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32
ji
fij
ijcc
PB 1logInverse transformation and with
fij
fj
fiij CP
and a relative standard deviation then c
fij
fj
fi
fij
fj
fiij CCB 1log for 1.0
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Data assimilation with a relative error formulation
If the state-dependent observation error is dependent on the forecast instead
of the truth, i.e.
and that the state-dependent model error is dependent on the analysis
instead of the truth
Then the Bayesian update, and KF propagation using the proper conditional
expectation can be derived and give the standard KF with
Ménard et al., 2000. MWR
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4.4 Lognormal KF • KF relative error formulation
34
qaq
ofo
~
~
με
με
• KF lognormal formulation
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Lognormal distributions:
Observation errors is not lognormally distributed
35
)1(exp 222 wc c
model values at observation sites observations
Observations at low concentrations can have negative values, because
there are detection limits, or because of the retrieval
ctecc bctecc
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Lognormal or something else ?
Process of random dilution
n is the number density (number of molecules per unit volume), v is the volume,
and q is total number of molecules
vnq
If all these molecules found themselves into a larger volume V, then the new
number density is VNq
thus n
V
vnN
where is a dilution factor 10
And after k dilutions,
k
iik
k
iik nnnn
10
10 lnlnlnor
If then and )1,0(~ Ui )1(~log EXPi )1,(~log1
kGammaK
ii
i
so nk ~ Log-Gamma distribution
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Thanks