1
Ocean Surface Topography Science Team, Reston, VA, USA, 19-23 October, 2015 References Feng et al., 2010. Splin based nonparametric estimation of the altimeter sea state bias correction, IEEE Geoscience and Remote Sensing Letters, vol. 7, issue 3, pp. 577-581. Tran et al., 2010. Overview andUpdate of the Sea State Bias Corrections for the Jason-2, Jason-1 and TOPEX Missions, Marine Geodesy, 33:S1, 348-362, • Rascle and Ardhuin, 2013, global wave parameter database for geophysical applications. Part 2: Model validation with improved source term parameterization. Ocean Modelling, 70, 174–188, •Rodriguez and Martin, 1994, Assessment of the TOPEX altimeter performance using waveform retracking, JGR, • Hayne et al., 1994, The corrections for significant wave height and attitude effects in the TOPEX radar altimeter, , JGR. • Vandemark et al., 2002, Direct estimation of sea state impacts on radar altimeter sea level mea- surements, Geophys. Res. Lett., 29(24), 2148, doi:10.1029/ 2002GL015776 Acknowledgements : JPL and NASA’s Science Directorate Physical Oceanography Program Objectives Understand details within the TOPEX retracking data (RGDR) released by JPL in early 2015 including the proposed range corrections • Develop TOPEX Ku-band 2D and 3D Sea State Bias (SSB) correction models for both RGDR and MGDR data • Provide a comprehensive data evaluation • Recommend optimal and sufficient SSB models for climate record TOPEX data applications • Release new SSB models for community evaluation Result PART 3: J1/Tx tandem cal/val phase evaluation (J1: cycles 1-21: Tx sideB: cycles 344-364) RGDR Skew=fit No SSB corr SSB corr RGDR Skew=0.1 RGDR Skew=fit SSHA data used • TX RGDR SSHA: the orbit: gsfc/std1410 GOT4.10tide • TX MGDR SSHA: the orbit: gsfc/std1410 GOT4.10tide • J1 GDR SSHA : the orbit: gsfc/std1204 GOT4.08tide SSB corr. models applied • TX RGDR: SPSSB2d • TX MGDR: CLS SSB2d(Tran et al. 2010) • J1 GDR CLS SSB2d (Tran et al. 2010) No SSB corr SSB corr Result PART 4: Latitude-dependent variance reduction on collinear SSHA difference Ascending RGDR Skew=0.1 Ascending Descendin g Difference between Tx RGDR and Tx MGDR SSHA without/with SSB Difference between Tx RGDR and J1 GDR SSHA without/with SSB Descendin g Ascending Descendi ng Ascending Descendi ng SPSSB2d vs. CLSSSB2d SPSSB3d vs. CLSSSB2d SPSSB2d vs. CLSSSB2d SPSSB3d vs. CLSSSB2d TOPEX Side A TOPEX Side B 1993 Side A skew01 Ascending Descending Ascending Descending Toward the Equator Result PART 1: Resual range correction difference between Tx RGDR(skew=0.1) and MGDR(swh/att/accl) Latitude-dependency Wave height - dependency 2000 Side B Skew 01 c) Skew- 01 Result PART 2: 2D SSB model comparison MGDR CLS SSB2d TX Side B RGDR SPSSB2d vs. MGDR CLSSSB2d TX Side B RGDR SPSSB2d vs. Jason 1 GDR CLSSSB2d a) Skew- fit b) TxB RGDR (skew==0.1) SPSSB2d J1 GDR CLS SSB2d = MGDR CLS SSB2d TxA RGDR (skew=0.1) SPSSB2d - SSB difference = SSB difference - = - SSB difference TX Side A RGDR SPSSB2d vs. MGDR CLSSSB2d Variance Reduction (cm 2 ) Variance Reduction (cm 2 ) Variance Reduction (cm 2 ) Variance Reduction (cm 2 ) Red = retracking – MGDR range correction due to swh/att/accel Black = retracking – MGDR range correction due ONLY to acce Red = retracking – MGDR range correction due to swh/att/accel Black = retracking – MGDR range correction due ONLY to acce cm cm cm cm Methodology SSHA (sea surface height anomaly) is calculated in terms of the latest geophysical corrections, including the new GSFC std1410 orbit SSB models based on SPline(SP) nonparametric estimator (Feng et al., 2010) using direct SSHA data (Vandemark et al, 2002) SSB correction look-up tables were derived as follows for both Side A and Side B data: • Produce yearly SPSSB models in 2D (swh, altU10) and 3D SSB(swh, altU10, Tm 02 ) where Tm 02 is the mean wave period from the Wavewatch 3 model (ver CFSR from IFREMER) • Final results are multi-year ensemble solutions for MGDR & RGDR (skewness= 0,0.1, derived (fit)) Side A: 1993-1998 (cycles 21-232); Side B: 1999-2002 (cycles 240-350) Result: Data Evaluation PART 1: Residual range correction differences observed between retracked RGDR and MGDR data (swh/att/accel) following Rodriguez and Martin (1994) PART2: SSB Model comparisons – RGDR compared to ‘standard’ MGDR CLS SSB2d developed with Linear Kernel Smoothing on collinear data (Tran et al. 2010) PART3: J1/Tx assessed for cal/val phase (J1 cycles 1-21; Tx 344-364) in terms of SSHA without SSB & SSHA with SSB corrections PART 4: Variance reduction (new SSB3d or SSB2d vs. CLS SSB2d) in MGDR and RGDR applications PART 1: Summary • The residual range correction between RGDR(skew=0.1) and MGDR is higher than those reported by Rodriguez and Martin (1994) – reasons TBD. • The residual range correction in skew=0.1 case is much lower than for the RGDR skew=fit case (not shown) - consistent with the MGDR swh/att/accel imposition of skew=0.1 (Hayne et al., 1994). Cross-equator range discontinuity is still seen due to sign change in range (i.e. height) rate, depending on whether a pass is descending or ascending. • Some level of SWH- dependent residual range correction still associated with range rate, toward or departing from the equator. PART 2: Summary TxA and TxB RGDR (skew=0.1) 2DSPSSB do show some significant difference, compared to the MGDR CLS SSB2d: 1) in the domain SWH>4-5m & U10 >7-12m/s, the MGDR CLS 2DSSB(Hs, U10) has less structure with SWH, but RGDR 2DSSBs display richer structure 2) at the lower U10 <2m/s, the RGDR 2DSSB displays more wind speed dependent feature than the MGDR CLS 2DSSB • New TxB RGDR 2D SSB model is closer to Jason-1 GDR 2d SSB in terms of SWH sensitivity PART3 Summary TX RGDR (skew=fit) not a recommended option for application ( excessive quadrant offsets ) Compared to TX MGDR, RGDR (skew=0.1) SSHA with SSB correction applied has reduced quadrant offset • TX RGDR (skew=0.1) after SSB correction looks fairly consistent with the J1 GDR PART 4 : Summary Briefly, one can expect modest improvement, mostly at high latitudes using the 2D RGDR (skew =0.1) SSB models versus the standard MGDR 2D SSB model when working with the RGDR data. Otherwise, the 3D SSB model improvement is more obvious and in line with gains seen for the Jason satellites when working with either the MGDR or RGDR datasets. Clearly one also needs the new SSB model in using RGDR (skew=fit) data. Revised sea state bias models for retracked Revised sea state bias models for retracked TOPEX altimeter data TOPEX altimeter data Hui Feng Hui Feng 1 1 , , Doug Vandemark Doug Vandemark 1 1 , and Phil Callahan , and Phil Callahan 2 2 1 1 Ocean Process Analysis Lab ,University of New Hampshire Ocean Process Analysis Lab ,University of New Hampshire , Durham, NH, , Durham, NH, USA USA 2 2 JPL, Pasadena JPL, Pasadena , CA, USA , CA, USA TxB RGDR (skew=0.1) SPSSB2d Latitude Latitude Latitude Latitude Latitud e Latitud e Latitud e Latitud e Cross-Equator discontinuity Toward the Equator

Ocean Surface Topography Science Team, Reston, VA, USA, 19-23 October, 2015 References Feng et al., 2010. Splin based nonparametric estimation of the altimeter

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Page 1: Ocean Surface Topography Science Team, Reston, VA, USA, 19-23 October, 2015 References Feng et al., 2010. Splin based nonparametric estimation of the altimeter

Ocean Surface Topography Science Team, Reston, VA, USA, 19-23 October, 2015

References• Feng et al., 2010. Splin based nonparametric estimation of the altimeter sea state bias correction, IEEE Geoscience and Remote Sensing Letters, vol. 7, issue 3, pp. 577-581.• Tran et al., 2010. Overview andUpdate of the Sea State Bias Corrections for the Jason-2, Jason-1 and TOPEX Missions, Marine Geodesy, 33:S1, 348-362, • Rascle and Ardhuin, 2013, global wave parameter database for geophysical applications. Part 2: Model validation with improved source term parameterization. Ocean Modelling, 70, 174–188,•Rodriguez and Martin, 1994, Assessment of the TOPEX altimeter performance using waveform retracking, JGR,• Hayne et al., 1994, The corrections for significant wave height and attitude effects in the TOPEX radar altimeter, , JGR.• Vandemark et al., 2002, Direct estimation of sea state impacts on radar altimeter sea level mea- surements, Geophys. Res. Lett., 29(24), 2148, doi:10.1029/ 2002GL015776

Acknowledgements : JPL and NASA’s Science Directorate Physical Oceanography Program

Objectives• Understand details within the TOPEX retracking data (RGDR) released by JPL in early 2015 including the proposed range corrections• Develop TOPEX Ku-band 2D and 3D Sea State Bias (SSB) correction models for both RGDR and MGDR data • Provide a comprehensive data evaluation• Recommend optimal and sufficient SSB models for climate record TOPEX data applications• Release new SSB models for community evaluation

Result PART 3: J1/Tx tandem cal/val phase evaluation (J1: cycles 1-21: Tx sideB: cycles 344-364)

RGDR Skew=fit

No SSB corr

SSB corr

RGDR Skew=0.1 RGDR Skew=fit

SSHA data used • TX RGDR SSHA: the orbit: gsfc/std1410 GOT4.10tide• TX MGDR SSHA: the orbit: gsfc/std1410 GOT4.10tide• J1 GDR SSHA : the orbit: gsfc/std1204 GOT4.08tideSSB corr. models applied• TX RGDR: SPSSB2d• TX MGDR: CLS SSB2d(Tran et al. 2010)• J1 GDR CLS SSB2d (Tran et al. 2010)

No SSB corr

SSB corr

Result PART 4: Latitude-dependent variance reduction on collinear SSHA difference

Ascending

RGDR Skew=0.1

AscendingDescending

Difference between Tx RGDR and Tx MGDR SSHA without/with SSB

Difference between Tx RGDR and J1 GDR SSHA without/with SSB

Descending

AscendingDescending AscendingDescending

SPSSB2d vs. CLSSSB2d SPSSB3d vs. CLSSSB2d SPSSB2d vs. CLSSSB2d SPSSB3d vs. CLSSSB2d

TOPEX Side A TOPEX Side B

1993 Side A skew01

Ascending Descending

Ascending Descending

Toward the Equator

Result PART 1: Resual range correction difference between Tx RGDR(skew=0.1) and MGDR(swh/att/accl)

Latitude-dependency Wave height -

dependency

2000 Side B Skew 01

c) Skew-01

Result PART 2: 2D SSB model comparison

MGDR CLS SSB2d

TX Side B RGDR SPSSB2d vs. MGDR CLSSSB2d

TX Side B RGDR SPSSB2d vs. Jason 1 GDR CLSSSB2d

a) Skew-fit

b)

TxB RGDR (skew==0.1) SPSSB2d

J1 GDR CLS SSB2d

=

MGDR CLS SSB2d TxA RGDR (skew=0.1) SPSSB2d

-

SSB difference

=

SSB difference

-

= -

SSB difference

TX Side A RGDR SPSSB2d vs. MGDR CLSSSB2d

Variance Reduction (cm2) Variance Reduction (cm2) Variance Reduction (cm2) Variance Reduction (cm2)

Red = retracking – MGDR range correction due to swh/att/accelBlack = retracking – MGDR range correction due ONLY to acce

Red = retracking – MGDR range correction due to swh/att/accelBlack = retracking – MGDR range correction due ONLY to acce

cmcm

cmcm

Methodology• SSHA (sea surface height anomaly) is calculated in terms of the latest geophysical corrections, including the new GSFC std1410 orbit• SSB models based on SPline(SP) nonparametric estimator (Feng et al., 2010) using direct SSHA data (Vandemark et al, 2002)• SSB correction look-up tables were derived as follows for both Side A and Side B data:

• Produce yearly SPSSB models in 2D (swh, altU10) and 3D SSB(swh, altU10, Tm02) where Tm02 is the mean wave period from the Wavewatch 3 model (ver CFSR from IFREMER)• Final results are multi-year ensemble solutions for MGDR & RGDR (skewness= 0,0.1, derived (fit))

Side A: 1993-1998 (cycles 21-232); Side B: 1999-2002 (cycles 240-350)

Result: Data Evaluation• PART 1: Residual range correction differences observed between retracked RGDR and MGDR data (swh/att/accel) following Rodriguez and Martin (1994)• PART2: SSB Model comparisons – RGDR compared to ‘standard’ MGDR CLS SSB2d developed with Linear Kernel Smoothing on collinear data (Tran et al. 2010)• PART3: J1/Tx assessed for cal/val phase (J1 cycles 1-21; Tx 344-364) in terms of SSHA without SSB & SSHA with SSB corrections• PART 4: Variance reduction (new SSB3d or SSB2d vs. CLS SSB2d) in MGDR and RGDR applications

PART 1: Summary

• The residual range correction between RGDR(skew=0.1) and MGDR is higher than those reported by Rodriguez and Martin (1994) – reasons TBD.

• The residual range correction in skew=0.1 case is much lower than for the RGDR skew=fit case (not shown) - consistent with the MGDR swh/att/accel imposition of skew=0.1 (Hayne et al., 1994).

• Cross-equator range discontinuity is still seen due to sign change in range (i.e. height) rate, depending on whether a pass is descending or ascending.

• Some level of SWH-dependent residual range correction still associated with range rate, toward or departing from the equator.

PART 2: Summary

• TxA and TxB RGDR (skew=0.1) 2DSPSSB do show some significant difference, compared to the MGDR CLS SSB2d: 1) in the domain SWH>4-5m & U10 >7-12m/s, the MGDR CLS 2DSSB(Hs, U10) has less structure with SWH, but RGDR 2DSSBs display richer structure 2) at the lower U10 <2m/s, the RGDR 2DSSB displays more wind speed dependent feature than the MGDR CLS 2DSSB

• New TxB RGDR 2D SSB model is closer to Jason-1 GDR 2d SSB in terms of SWH sensitivity

PART3 Summary • TX RGDR (skew=fit) not a recommended option for application ( excessive quadrant offsets )

• Compared to TX MGDR, RGDR (skew=0.1) SSHA with SSB correction applied has reduced quadrant offset

• TX RGDR (skew=0.1) after SSB correction looks fairly consistent with the J1 GDR

PART 4 : Summary Briefly, one can expect modest improvement, mostly at high latitudes using the 2D RGDR (skew =0.1) SSB models versus the standard MGDR 2D SSB model when working with the RGDR data. Otherwise, the 3D SSB model improvement is more obvious and in line with gains seen for the Jason satellites when working with either the MGDR or RGDR datasets. Clearly one also needs the new SSB model in using RGDR (skew=fit) data.

Revised sea state bias models for retracked TOPEX altimeter dataRevised sea state bias models for retracked TOPEX altimeter data

Hui FengHui Feng11,, Doug VandemarkDoug Vandemark11, and Phil Callahan, and Phil Callahan22 1 1Ocean Process Analysis Lab ,University of New HampshireOcean Process Analysis Lab ,University of New Hampshire, Durham, NH, USA, Durham, NH, USA

22JPL, PasadenaJPL, Pasadena, CA, USA, CA, USA

TxB RGDR (skew=0.1) SPSSB2d

LatitudeLatitude

LatitudeLatitudeL

atit

ud

e

Lat

itu

de

Lat

itu

de

Lat

itu

de

Cross-Equator discontinuity

Toward the Equator