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Development of Algorithm for the Development of Algorithm for the Retrieval of Atmospheric Profiles from Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT Infrared Sounder onboard INSAT - - 3D 3D Pradeep K Thapliyal M V Shukla, P C Joshi and P K Pal M V Shukla, P C Joshi and P K Pal Meteorology & Oceanography Group (MOG) Meteorology & Oceanography Group (MOG) Space Applications Centre (SAC) Space Applications Centre (SAC) Indian Space Research Indian Space Research Organisation Organisation (ISRO) (ISRO) Ahmedabad Ahmedabad - - 380015 (INDIA) 380015 (INDIA) International TOVS Study Conference (ITSC-17), Monterey, CA (USA) 14-20 April 2010 [email protected] [email protected]
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Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Jan 16, 2020

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Page 1: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Development of Algorithm for the Development of Algorithm for the Retrieval of Atmospheric Profiles from Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSATInfrared Sounder onboard INSAT--3D3D

Pradeep K ThapliyalM V Shukla, P C Joshi and P K PalM V Shukla, P C Joshi and P K Pal

Meteorology & Oceanography Group (MOG)Meteorology & Oceanography Group (MOG)Space Applications Centre (SAC)Space Applications Centre (SAC)

Indian Space Research Indian Space Research OrganisationOrganisation (ISRO)(ISRO)AhmedabadAhmedabad--380015 (INDIA)380015 (INDIA)

International TOVS Study Conference (ITSC-17), Monterey, CA (USA) 14-20 April 2010

[email protected]@sac.isro.gov.in

Page 2: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Channel No.

Wavelength Band Resolution(Km)

1 0.55 - 0.75 μm 12 1.55 - 1.70 μm 13 3.7 - 3.95 μm 44 6.5 - 7.1 μm 85 10.3 - 11.3 μm 46 11.3 - 12.50 μm 4

Channel No.

Wavelength Band Resolution(Km)

1 0.55 - 0.75 μm 12 1.55 - 1.70 μm 13 3.7 - 3.95 μm 44 6.5 - 7.1 μm 85 10.3 - 11.3 μm 46 11.3 - 12.50 μm 4

Channel No.

Wavelength Band Resolution(Km)

1 0.55 - 0.75 μm 12 1.55 - 1.70 μm 13 3.7 - 3.95 μm 44 6.5 - 7.1 μm 85 10.3 - 11.3 μm 46 11.3 - 12.50 μm 4

INSAT-3D Satellite/Sensor

INSAT-3D SounderResolution: 10 km

INSAT-3D Imager

3-Axis Stabilized Geostationary Meteorological Satellite (India)

Location: TBD•

Launch Date: Dec. 2010

Atmospheric SounderChannel

No.λC (Δλ)(in μm)

Principal absorbing constituents

1 14.71 (0.281) CO2 – band2 14.37 (0.268) CO2 – band3 14.06 (0.256) CO2 – band4 13.96 (0.298) CO2 – band5 13.37 (0.286) CO2 – band6 12.66 (0.481) water vapor7 12.02 (0.723) water vapor8 11.03 (0.608) window9 9.71 (0.235) ozone10 7.43 (0.304) water vapor11 7.02 (0.394) water vapor12 6.51 (0.255) water vapor13 4.57 (0.048) N2O14 4.52 (0.047) N2O15 4.45 (0.0456) CO2

16 4.13 (0.0683) CO2

17 3.98 (0.0663) window18 3.74 (0.140) window19 0.695 (0.05) vis

Atmospheric SounderChannel

No.λC (Δλ)(in μm)

Principal absorbing constituents

1 14.71 (0.281) CO2 – band2 14.37 (0.268) CO2 – band3 14.06 (0.256) CO2 – band4 13.96 (0.298) CO2 – band5 13.37 (0.286) CO2 – band6 12.66 (0.481) water vapor7 12.02 (0.723) water vapor8 11.03 (0.608) window9 9.71 (0.235) ozone

Atmospheric SounderChannel

No.λC (Δλ)(in μm)

Principal absorbing constituents

1 14.71 (0.281) CO2 – band2 14.37 (0.268) CO2 – band3 14.06 (0.256) CO2 – band4 13.96 (0.298) CO2 – band5 13.37 (0.286) CO2 – band6 12.66 (0.481) water vapor7 12.02 (0.723) water vapor8 11.03 (0.608) window9 9.71 (0.235) ozone10 7.43 (0.304) water vapor11 7.02 (0.394) water vapor12 6.51 (0.255) water vapor13 4.57 (0.048) N2O14 4.52 (0.047) N2O15 4.45 (0.0456) CO2

16 4.13 (0.0683) CO2

17 3.98 (0.0663) window18 3.74 (0.140) window19 0.695 (0.05) vis

Page 3: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

INSATINSAT--3D Sounder Specifications3D Sounder Specifications

System weightSystem weight: 153 kg: 153 kg

System PowerSystem Power: < 100 Watts: < 100 Watts

IFOVIFOV: 280 : 280 μμradrad (E(E--W) x 280 W) x 280 μμradrad (N(N--S) ~10kmS) ~10km

No. of simultaneous sounding per channelNo. of simultaneous sounding per channel: 4: 4

Field of Regard (FOR)Field of Regard (FOR): 24: 24°° EE--W x 21W x 21°° NN--S S

Step sizeStep size: E: E--W: 278.9 W: 278.9 μμradrad, N, N--S: 1115.6 S: 1115.6 μμradrad

Active Scan CoverageActive Scan Coverage: E: E--W and NW and N--S from ~1S from ~1°° (64 steps) to (64 steps) to ~10~10°° (640 steps)(640 steps)

Signal quantizationSignal quantization: 14 Bits/sample: 14 Bits/sample

Downlink Downlink dataratedatarate: 40K Bits/Sec: 40K Bits/Sec

Blackbody calibrationBlackbody calibration: Every 30 minutes or ground command: Every 30 minutes or ground command

Page 4: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Vertical Profiles of:Vertical Profiles of:––

TemperatureTemperature––

HumidityHumidity

(Surface (Surface ––

100 100 hPahPa))Surface Skin TemperatureSurface Skin TemperatureTotal Ozone Total Ozone

Pressure Levels (40) in hPa :1000, 950, 920, 850, 750, 700, 670, 620, 570, 500, 475, 430, 400, 350, 300, 250, 200, 150, 135, 115, 100, 85,70,60, 50, 30, 25, 20, 15, 10, 7, 5, 4, 3, 2, 1.5, 1, 0.5, 0.2, 0.1

Observation zenith angle, INSAT-3D at 84E

6400 km x 6400 km scan takes 180 minutes

Objectives

Page 5: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Characteristics of the atmosphere over GOES vs INSAT-3D Observations

INSAT-3D

INSAT-3D

INSAT-3D

INSAT-3D

GOES-W GOES-E GOES-W GOES-E

GOES-W GOES-E GOES-W GOES-E

NCEP NCEP

NCEP NCEP

Page 6: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

TwoTwo--step retrieval algorithm of CIMSS/UWstep retrieval algorithm of CIMSS/UW––

Regression retrieval followed by Physical retrieval Regression retrieval followed by Physical retrieval (Jun Li et al. 2000)(Jun Li et al. 2000)

Different modules include:Different modules include:––

Fast RT model Fast RT model ––

PFAAST PFAAST ((HaalHaal

Woolf)Woolf)

––

Sounder Radiance bias correction Sounder Radiance bias correction ––

Linear Regression (Linear Regression (ObsObs

vsvs

SimSim

Tb)Tb)––

Cloud detection routine Cloud detection routine (McMillan & Dean, 1982)(McMillan & Dean, 1982)

––

PP

ss

from forecast and from forecast and εε

from SSEC/UW dataset at sounder pixelfrom SSEC/UW dataset at sounder pixel––

Hybrid First Guess: Linear combination of Regression and ForecasHybrid First Guess: Linear combination of Regression and Forecastt––

Physical retrieval Physical retrieval (Jun Li et al. 2000)(Jun Li et al. 2000)

––

Total Ozone from Separate Regression Routine Total Ozone from Separate Regression Routine (Jun Li et al. 2001)(Jun Li et al. 2001)

Retrieval package is ready and installed at SACRetrieval package is ready and installed at SAC

Improvement in humidity sounding achievedImprovement in humidity sounding achieved

Further work under ISROFurther work under ISRO--SSEC SSEC MoUMoU

Retrieval Algorithm Retrieval Algorithm

Page 7: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

INSATINSAT--3D Retrieval Algorithm 3D Retrieval Algorithm -- FlowchartFlowchart

Hybrid First Guess (X0 )X0 = Wfcst .Xfcst + Wreg .Xreg

Compute radiances: y=F(Xn )(For first iteration X1 = X0 )

CompareCalculate residual

Sounder Radiances(FOR: 4x4, 2x2, or single pixel)

Cloud detection/clearing

Radiance Bias CorrectionRad Tb (Y)

Exit Physical retrieval fail

Regression as final retrieval

Iteration < 8Residual > Threshold

Iterate with new profile

Iteration = 8Residual > Threshold

Residual < Threshold

Output (X)Physical retrieval successful

Xn+1 = X0 + (KnT E-1 Kn + γI)-1.

{KnT E-1 [δYn

m + Kn (Xn – X0)] + γ(Xn – X0)}

Cloudy FORExit

clear pixels < 25 %

Forecast profile (Xfcst )Regression Retrieval Xreg = Xmean +RC.(dY)T

∑=

++ −=nch

knkkn nchxyYr

1

21

21 /)]([

Average Radiances of all clear pixels in FOR

clear pixels > 25 %

(Threshold NEΔT)

Physical RetrievalPhysical Retrieval

Radiative Transfer simulation Y = F(X) + ε

RC = dX.dYT.(dY.dYT)-1

(K=∂Y/∂X)

(Li et al, 2000, JAM; Ma et al, 1997, JAM)

Compute Wfcst Compute WReg

Page 8: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

PFAAST RT Model PFAAST RT Model

Std. Dev. of PFAAST - LBL Tb differences for 49 profiles, 5 Angles (0-60)

0

0.1

0.2

0.3

0.4

0.5

0.6

0.7

0.8

0.9

1

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18

Sounder Channel #

Std

Dev

of D

iffer

ence

Tb

(K)

NeDT@StdTempPFAAST (7 ZenAng 0-70)PFAAST (6 ZenAng 0-62.5)PFAAST (5 ZenAng 0-60)

PFAAST (PFAAST (PressurePressure--layer Fast Algorithm for Atmospheric Transmittances)layer Fast Algorithm for Atmospheric Transmittances)

Improvement in PFAAST by restricting domain Improvement in PFAAST by restricting domain uptoupto zenith angle 60zenith angle 60°°

Page 9: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Regression RetrievalRegression Retrieval––

Coefficients at different zenith angles (150 classes from 0Coefficients at different zenith angles (150 classes from 0--6565°°))––

3 different latitude zones (03 different latitude zones (0--20, 2020, 20--40, 4040, 40--60 in N/S) 60 in N/S) ––

Different coefficients for land and ocean (Emissivity differenceDifferent coefficients for land and ocean (Emissivity difference))––

Spectral emissivity as predictor over landSpectral emissivity as predictor over land––

NonNon--linear term (Tblinear term (Tb22))

and Pand P

ss

as predictor as predictor ––

q and q and ln(qln(q) as predictand for hybrid regression retrieval) as predictand for hybrid regression retrieval

Statistics (independent testing dataset 30NStatistics (independent testing dataset 30N--30S)30S)–

RMSE TS : 0.64 K, RMSE Total O3

: 14 Dob, –

RMSE TPW: REG_LNQ: 0 .71 cm, REG_HYB: 0.56 cm

(a) Entire dataset300

400

500

600

700

800

900

100015 20 25 30 35 40 45

RMSE humidity (%)

Pres

sure

(hPa

)

REG_LNQREG_QREG_HYB

(b) Dry atmospheric profiles300

400

500

600

700

800

900

100025 35 45 55 65 75

RMSE humidity (%)

Pres

sure

(hPa

)

REG_LNQREG_QREG_HYB

(b) Wet atmospheric profiles300

400

500

600

700

800

900

100015 20 25 30 35 40 45

RMSE humidity (%)

Pres

sure

(hPa

)REG_LNQREG_QREG_HYB

Page 10: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

••

CCost Function: ost Function: J(X) = [J(X) = [YYmm

--

Y(X)]Y(X)]T T EE--1 1 [[YYmm

--

Y(X)] + (X Y(X)] + (X --

XX

00

))TT

HH

(X (X --

XX

00

))XX00

is the first guess profile, is the first guess profile, YYmm

radiance measurements, and radiance measurements, and Y(X)Y(X)

is forward model.is forward model.HH

is a priori matrix that constrains the solution (e.g. first gueis a priori matrix that constrains the solution (e.g. first guess error ss error covcov. matrix).. matrix).EE is expected radiance error covariance matrix.is expected radiance error covariance matrix.

Physical RetrievalPhysical Retrieval

••

Minimization of the cost function using nonlinear Newtonian iterMinimization of the cost function using nonlinear Newtonian iteration yields ation yields the following iterative solution:the following iterative solution:

XX

n+1n+1

= X= X

00

+ (+ (KK

nn

TT

EE--11

KK

nn

+ + γγ

nn

I)I)--11. {. {KK

nn

TT

EE--11

[[δδYY

nn

mm

+ + KK

nn

((XX

nn

––

XX

00

)] + )] + γγ

nn

(X(X

nn

––

XX

00

)})}

••

Iterative solution in terms of eigenvectors is:Iterative solution in terms of eigenvectors is:

ff

n+1n+1

= (= (ξξ

nn

TT

EE--11

ξξ

nn

+ + γγ

nn

I)I)--11. {. {ξξ

nn

TT

EE--11

[[δδYY

nn

mm

+ + ξξ

nn

.f.f

nn

] + ] + γγ

nn

.f.f

nn

}}

wherewhere,, ξξ

= K.V= K.V, , and and VV

is eigenvector matrix, and is eigenvector matrix, and ff

is is coefficient vectorcoefficient vectorVV contains 5 contains 5 EOFsEOFs

for temperature profile, 3 for temperature profile, 3 EOFsEOFs

for humidity profile.for humidity profile.

(Jun Li et al. 2000)(Jun Li et al. 2000)

Page 11: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

––

Expansion coefficient convergence test:Expansion coefficient convergence test:

ddn+1 n+1 = (f= (fn+1n+1 –– ffnn))TT.(.(ξξnnTT EE--11 ξξnn + + γγnnI)I)--11.(f.(fn+1n+1 –– ffnn))

ddn+1n+1 00 solution converges (i.e., solution converges (i.e., ffn+1n+1 ffnn).).

Iteration stops when Iteration stops when (d(dn+1n+1 –– ddnn)) < threshold< threshold (~ 0.1). (~ 0.1). If If ddn+1n+1 > > ddnn thenthen γγnn is increased.is increased.

––

Brightness temperature residual testBrightness temperature residual test::

RMS radiance residual is defined as: RMS radiance residual is defined as:

If If rrn+1n+1 ≤≤ rrnn the iteration continues until the iteration continues until rr

n+1n+1

is acceptably small (less then NEDT)is acceptably small (less then NEDT)

∑=

++ −=nch

knkkn nchxyYr

1

21

21 /)]([

Convergence TestConvergence Test

Sample ResultSample Result

Page 12: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

SUMMARYSUMMARY

INSATINSAT--3D having 19 channel Sounder is scheduled for 3D having 19 channel Sounder is scheduled for launch in Dec 2010launch in Dec 2010

Retrieval package based on twoRetrieval package based on two--step algorithm ready for step algorithm ready for INSATINSAT--3D3D

Accuracies of the retrieved products are comparable to the Accuracies of the retrieved products are comparable to the similar products from other missions (Simulation study).similar products from other missions (Simulation study).

Algorithm to be developed for cloud property Algorithm to be developed for cloud property retrieval/cloudy sky retrievals.retrieval/cloudy sky retrievals.

Further improvements/developments under Further improvements/developments under ISROISRO--SSEC SSEC MoUMoU

Page 13: Development of Algorithm for the Retrieval of Atmospheric ...Development of Algorithm for the Retrieval of Atmospheric Profiles from Infrared Sounder onboard INSAT-3D Pradeep K Thapliyal.

Special Thanks toSpecial Thanks to……..ITWG for financial support to attend ITSCITWG for financial support to attend ITSC--1717SSEC/UWSSEC/UW for providing visiting fellowship (2005for providing visiting fellowship (2005--06)06)Allen HuangAllen Huang and and Jun LiJun Li for providing guidance and for providing guidance and support in the retrieval algorithmsupport in the retrieval algorithmHaalHaal WoolfWoolf for the RT Modelfor the RT ModelS S SuzaneSuzane and and E E BorbasBorbas for the for the SeeBorSeeBor dataset and dataset and spectral spectral emissivityemissivity datasetdataset