M. Reuter, EMS, Berlin, September 2011 Retrieval of atmospheric CO 2 from satellite near-infrared...
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Transcript of M. Reuter, EMS, Berlin, September 2011 Retrieval of atmospheric CO 2 from satellite near-infrared...
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e
Retrieval of atmospheric CO2 from satellite near-infrarednadir spectra in the frame of ESA’s climate change initiative
M.Reuter , O.Schneising , M.Buchwitz , J.Heymann, H.Bovensmann, J.P.BurrowsInstitute of Environmental Physics, University of Bremen, Germany
EMS, Berlin, September 2011
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e ESA’s GHG-CCI: Aims and Motivation
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e ESA’s GHG-CCI: Road Map
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e Two in-house algorithms
BESD (XCO2) WFMD (XCO2, XCH4)
Inversion Algorithm:Optimal Estimation;
Full Physics
Least-squares;
Light path Proxy
A-priori constraints:
Yes
Constant: CO2(p), aerosol,
cirrus, ...
Per pixel: P, T, H2O, ...
No
(constant atmosphere as
linearization point for RT)
Atmosphere: ECMWF US Standard (sev. H2O)
Aerosols: State vector (APS) Constant; AAI filter (CO2 only)
Clouds:State vector (CWP, CTH);
Filtering: MERIS 1x1 km2
RT cloud free;
Filtering: O2 & PMD (CO2 only)
Fit windows: Merged fit windows Independent fit windows
Radiative Transfer: SCIATRAN on-line SCIATRAN LUT
Speed: Slow (~15 min./pixel) Fast (~2 min./orbit)
Optimized for: Accuracy Compromise accuracy/speed
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e BESD XCO2
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e Validation with TCCON FTS measurements
350km
Park Falls, USA
350km
Bremen, Germany
350km
Darwin, Australia
350km
Lauder, New Zealand
• Restriction to a limited validation data set due to computational costs• Only 4 TCCON sites measured in the full period 2006-2010
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e Comparison with FTS, CarbonTracker, GOSAT
Overall good agreement betweenSCIAMACHY, GOSAT, FTS
and CarbonTracker
No statistical significantregional biases
Single measurementprecision ~2.5ppm
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e Comparison with FTS, CarbonTracker, GOSAT
Smoothed Results show:Good agreement of year-to-year increase and seasonal amplitude.
(Data density allows smoothing only at Park Falls and Darwin)
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e WFMD XCO2
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e Global increase
• Computational costs are orders of magnitude lower• Processing of global data easily possible• A global dataset 2003-2009 is available• Similar annual global patterns• Continuous year-to-year increase of global XCO2
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e CO2 uptake by growing vegetation
Mean wind direction
LongitudeWest East
XCO2
Fnet
Assumption:XCO2 gradient in wind direction
approximately proportionalto net surface flux Fnet
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e CO2 uptake by growing vegetation
Calculation of gradients aboveboreal forests (Canada+Russia):Good agreement with CarbonTracker(year-to-year progression and size)
Canada: larger neg. gradientssuggest stronger CO2 uptake
Russia: less strong gradientssuggest weaker CO2 uptake
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e
http://www.esa-ghg-cci.org/Intercomparison with other XCO2 algorithms
• Within the GHG CCI several different XCO2 retrieval techniques are involved: BESD, WFMD, and the algorithms of SRON, University of Leicester, ACOS, and NIES
• First inter-comparisons with FTS measurements show many similarities but also differences which have to be analyzed
M. R
eute
r, E
MS
, Ber
lin, S
epte
mb
er 2
011
Ret
rieva
l of a
tmos
pher
ic C
O2
from
sat
ellit
e ne
ar-in
frar
edna
dir
spec
tra
in th
e fr
ame
of E
SA
’s c
limat
e ch
ange
initi
ativ
e
http://www.esa-ghg-cci.org/
THANKS!