Extraction of Wind and Wave Field from SAR data

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Transkript:

Extraction of Wind and Wave Field from SAR data S. Lehner, X. Li, Th. Bruns, W. Rosenthal German Aerospace Center (DLR), Oberpfaffenhofen

Motivation Derive integrated Wave Parameters (e.g. SWH, mean period) from satellite SAR data by an empirical algorithm without using a first guess: CWAVE (= make the SAR to measure like an altimeter on a parallel track) Thus develop global data set of SWH and mean period for assimilation into models and global statistics (altimeter and SAR, available since 1991) Derive 2D Spectrum from SAR using model first guess Observation of coastal wave variations using high resolution TerraSAR data Folie 2 Validation of TSX image spectra to measurements of marine radar and model data

Motivation example: Sea State Measurements in Storms GFO ASAR RA-2 SAR vs. Radar Altimeter cross over measurements On DWD model DWD model is not assimilated With RA information. Jan. 01, 2007 Folie 3

TSX Spotlight mode image acquired on May 15, 2009 at 17:19 UTC over Ekofisk oil platform Hs(m) Tp(s) Dir( ) WaMoS 3.8 8.1 87 TSX 3.8 8.5 60 Folie 4

Methodology Derive sets of parameters from SAR images (e.g. mean intensity, spectral parameters) use SAR parameters in an empirical algorithm tuned by sea state parameters from ECMWF model : CWAVE (named analog to CMOD for wind speed) Cross validate SAR, altimeter and buoy sea state measurements with models Derive 2D Spectrum from SAR using model first guess use cross spectrum and inversion algorithm Folie 5 Validation of TSX image spectra to measurements of marine radar and model data

Empirical Algorithm ---CWAVE developed for ERS/SAR and ENVISAT/ASAR wave mode data 22 Image and spectral parameters s 1,...,s N N i=1 N i=1 i j=1 H s = a 0 + a i s i + a i, j s i s j Since 1991 Since 2002 a 0,...,a N, a 1,1,...,a N,N The Parameters are fitted using a training data set of SAR wave mode data and colocated ECMWF wave spectra Folie 6 J. Schulz-Stellenfleth, Th, König, S.Lehner, JGR, 2007 X. Li, S. Lehner, Th. Bruns, JGR 2009

Conclusions (1) The empirical algorithm CWAVE_ENV yields ocean wave measurements with ASAR wave mode d without first guess information. Accuracy of retrieved SWH using CWAVE_ENV algorithm has the quality of the RA measurements and is near to in situ buoy measurements. Statistical Para. vs. Buoy vs. ECMWF model vs. DWD model vs. Radar Altimeter Cor. Bias RMSE SI Cor. Bias RMSE SI Cor. Bias RMSE SI Cor. Bias RMSE SI SWH 0.90 0.06 0.70 24% 0.93-0.02 0.43 16% 0.90-0.05 0.51 18% 0.93-0.11 0.51 13% The empirical algorithm CWAVE_ENV also can yield accurate mean wave period measurements. vs. ECMWF model Statistical Para. Cor. Bias RMSE SI T m02 0.87-0.05 s 0.60 s 0.08 T m-10 0.85-0.06 s 0.74 s 0.08 Folie 7 Using the algorithm CWAVE_ENV, ASAR WM data can be used for global wave statistical analys the sampling issue needs to be considered. From X. Li, S. Lehner, Th. Bruns

Validation and intercomparison of CWAVE_ENV CWAVE_ENV vs. Buoy bias = Y i X i rmse SI = = 1 X i ( Y 1 n i n X i 2 ) [( Y Y ) ( X X )] i i i i 2 Folie 8

vs. ECMWF_WAM reanalyzed, DWD_WAM -- forecast temporal resolution : ECMWF model : 6 hours ; DWD model : 3 hours spatial resolution: ECMWF model: 0.5 degree ; DWD model : 0.75 degree vs. ECMWF model vs. DWD model Folie 9

Crossover with altimeters RA: JASON RA: GFO Folie 10

SAR and Altimeter Hs on DWD Model Folie 11 CWAVE and RA-2 PARSA and RA-2 WVW and RA-2 Storm on 2007 Jan. 11 UTC 12:00 at NA Squares : ASAR Diamonds: RA-2

Global Significant Wave Height from PARSA (first guess Folie 12 From S. Abdallah

ENVISAT ASAR Level2 Product (WVW) f < 1/ 12s (, θ) H 12 = 4 E f dfd θ SWH Folie 13 H 12

ASAR + RA altimeter double tracks for strom investigation 0:00 UTC 12:00 UTC Folie 14 Storm on 2007 Feb. 10 at NA Squares : ASAR Diamonds: RA-2

CWAVE 2006 June~ 2007 May C-ERA-40, 1971-2000 KNMI Folie 15

Comparison of TSX image spectra to measurements of marine radar --WaMoS Sites: Ekofisk, Fino1, Helgoland, Azore Folie 16

Seastate Observations using TerraSAR-X TSX images Scan SAR, stripmap, spotlight Terceira Folie 17 X. Li et al, sub to IEEE TGARS

Observation of coastal wave variations using TSX data on the Portuguese island Azores. Wave refraction and diffraction Folie 18

DWD GSM Model at 18:00 UTC azimuth Folie 19 TerraSAR-X Spotlight data acquired on Mar.26th, 2008 at 19:32 UTC with ascending orbit with HH polarization, azimuth resolution: 2.8m, range resolution: 3.5m

Hs(m) Tp(s) Dir( ) WaMos 1.8 8.1 274 TSX 2.0 5.4 241 λ = P 42m Folie 20 TSX StripMap image (a) and subscene A (b) acquired over Helgoland on Nov.28, 2008 Remote at Sensing 5:50 Technology UTCInstitute

Ocean Wave Field shallow water λ T 2 = g h St Martin 50 m Folie 21

TSX Strip 23.3.2009 Lennox Island TSX Folie 22

Hs =4.9 m Tp = 7.5 s dir = 267 (87) Hurricane FRED Folie 23

Algorithm development for deriving SWH from TSX data Linear relation between SWH and TSX image energy, assuming! SWH F( E, α ) SAR _ image _ spectra α is peak wave direction relative to azimuth (satellite flight) direction Hs = a * 4 E(1.0 + cos( α)) + b Coefficients are determined by linear fitting with hindcast DWD model results Folie 24

Significant wave height TSX (m) 6 5 4 3 2 1 y = 0.975x + 0.1414 R 2 = 0.69 Si=0.29 Number of measurements:21 wave peak perriod TSX (s) 16 14 12 10 8 6 y = 1.0845x - 1.2069 R 2 = 0.66 Si=0.19 0 0 1 2 3 4 5 6 Significant wave height DWD (m) 400 4 4 6 8 10 12 14 16 wave peak period DWD (s) wave peak direction TSX ( ) 350 300 250 200 150 100 y = 0.7979x + 32.375 R 2 = 0.84 Folie 25 50 0 0 50 100 150 200 250 300 350 400 wave peak direction DWD ( )

Summary Coastal Measurements A preliminary result of the XWAVE algorithm shows good agreement with the numerical wave model from DWD, marine radar WAMOS, as well as the shipborne altimeter. Further validation and comparison to buoy measurements is being done (we acquired lots of images over buoys) TerraSAR X data can be used as a tool to observe wave reflection, wave refraction. Global statistics are not possible Folie 26 TerraSAR X data can be used for the observation of individual wave behaviour