The SEASAT Scatterometer Global Gridded Dealiased Wind Component data set consists of zonal and meridional wind components in meters per second. Each data file contains a 1 degree by 1 degree gridded synoptic wind field which extends from 70° South to 70° North and from 1° East to 360° East. Data are available at 6-hour intervals for the period between 6 September 1978 and 20 September 1978. This data set, also referred to as PO.DAAC product 013, underwent restoration in 1997.
Seasat Scatterometer Global 50km sigma-0 data-Wentz (PO.DAAC product 031)
Seasat scatterometer global dealiased wind vectors-Wentz (PO.DAAC product 029)
"The satellite orbit was near-circular, with an inclination of 108 deg, a period of about 101 min, and an altitude of approximately 800km. For the wide-swath instruments (i.e., SASS, SMMR, and VIRR), 95 percent of global coverage was accomplished every 36 h. The ground-track speed was about 6.6 km/s" [Boggs, 1982].
SEASAT Configuration
"The illumination pattern for each antenna was active for 1.89-s measurement periods. The 1.89-s measurement interval was repeated continually and contiguously, but a different antenna or polarization was activated for each consecutive sampling period. Each of eight possible SASS science operational modes was associated with a different prescribed antenna/polarization sequence ordered .... All modes were characterized by an antenna switching-cycle period of 7.56 s, during which four antenna-beam/polarization combinations were cycled through. This timing was to provide sigma-0 measurements spaced approximately 50km apart (footprint area center-to-center distance) in the along-track direction"
"Fifteen Doppler filters were used to electronically subdivide each full antenna footprint into 15 measurement resolution "Doppler" cells of approximate dimension 20 km (cross-beam) by 50 km (along-beam). The intersection of the antenna-beam pattern and Doppler lines determined the resolution cell size, orientation, and location on the Earth.... The instantaneous-field-of-view (IFOV) cell boundaries were determined by the Doppler filter noise bandwidth and the antenna 3-dB beamwidth (.5 deg) in the narrow-beam dimension. [The integrated cell is the area swept out by a sequence of 61 overlapping IFOV cells generated over the course of a 1.89-s measurement period.] The surface area of this final integrated Doppler resolution cell is greater than the instantaneous illuminated region because the satellite moved (about 12.5-km ground-track distance) during the measurement period. Each of these integrated Doppler cells is a SASS footprint, and has one sigma-0 backscatter measurement value associated with it" [Boggs, 1982].
Scatterometer Ground Pattern and Swath
"This calibration data is in the form of known calibration
signal levels applied to the scatterometer receiver. This
data was used to determine the current time-varying system
gain, which was then used to process the subsequent 124
science data frames. Since measurements leading to sigma-0
backscatter data were not generated during the calibration
frames, the SASS sensor data has an X-shaped gap in the
(two-sided) swath. The along-track dimension of the gap is
evidently given by one or two antenna beam patterns,
depending on whether the instrument mode was double- or
single-sided, respectively. The subsatellite point moved
nearly 1600 km between nominal occurences of calibration
frame sets." [Boggs, 1982]
Mode | Antenna/Polarization Sequence | Side |
---|---|---|
1 | 4V, 1V, 3V, 2V; repeat | Both |
2 | 4H, 1H, 3H, 2H; repeat | Both |
3 | 4V, 4H, 3V, 3H; repeat | Left |
4 | 1V, 1H, 2V, 2H; repeat | Right |
5 | 4V, 4V, 3V, 3V; repeat | Left |
6 | 1V, 1V, 2V, 2V; repeat | Right |
7 | 4H, 4H, 3H, 3H; repeat | Left |
8 | 1H, 1H, 2H, 2H; repeat | Right |
9 | Continuous Calibrate | |
10 | Standby |
"The data package received from GSFC consisted of the (non-SAR) sensor and engineering data as well as attitude and orbit determination data. This data was decommutated, organized by major frame, and converted from data numbers to engineering units. Footprint locations were calculated, and data was then formatted into archival-quality MSDR (Master Sensor Data Record) tape files..." [Boggs, 1982].
Sensor Data Record (SDR) files were then created from the MSDR tape files. "A Sensor Data Record tape file is a complete record of all data processed by the IDPS for a given data type for a given period of time. Thus, a SASS SDR contains all calculated scatterometer data taken from MSDRs for the desired range in time" [Boggs, 1982].
F.J. Wentz reprocessed the SASS SDR data to obtain sigma-0 values with 50-km by 50-km resolution cells (see PO.DAAC product 031). In a joint effort between the Jet Propulsion Laboratory (JPL), the University of California Los Angeles (UCLA), and the Atmospheric Environmental Service (AES) of Canada, meridional and zonal components of the wind were then calculated from Wentz's sigma-0 values. The results of this effort are presented in this data set.
Meridional Wind Component: magnitude of the wind velocity in
the north-south direction at 19.5 meters above the ocean
surface.
Latitude | Longitude | U Component | V Component | Data Quality Flag |
---|---|---|---|---|
Degrees North | Degrees East | m/s | m/s | |
-65 | 245 | -0.49 | 3.62 | 4 |
-65 | 246 | -1.43 | 4.03 | 4 |
-65 | 247 | -1.53 | 2.57 | 4 |
-65 | 248 | -1.59 | 0.46 | 4 |
-65 | 249 | -1.64 | -1.59 | 4 |
-65 | 250 | -1.61 | -3.66 | 4 |
-65 | 251 | -2.01 | -6.10 | 4 |
-65 | 252 | -7.03 | -7.77 | 4 |
-65 | 253 | -12.93 | -1.65 | 4 |
-65 | 254 | -13.70 | -5.30 | 4 |
-65 | 255 | -8.43 | -7.98 | 4 |
where:
syn denotes synoptic wind fields yyyy denotes the four digit year mm denotes the two digit month dd denotes the two digit day hh denotes the two digit hour z denotes hours zulu
The data are available in ASCII.
"The measurement accuracy of sigma-0 was affected primarily by communication noise, attitude pointing uncertainty, instrument processing (e.g., quantization errors and gain uncertainty), and various bias errors. Bias errors are in general deterministic and, depending upon the existence of adequate comparison data, are removable. The remaining errors which are random in nature and not removable, limit the ultimate accuracy of scattering coefficient measurements" [Boggs, 1982].
Radar returns from land and ice correspond to different scattering processes than those over open ocean, and can contaminate wind vector estimates.
Reference height for surface winds
The reference height for SASS wind vectors is 19.5 meters.
program read_seasat_013 C C READ_SEASAT_013: A Fortran program to read the SEASAT C Scatterometer global gridded dealiased C wind vectors produced in a joint effort C between JPL, UCLA and AES (referred to C as PO.DAAC product 013). C C This program was adapted from program READTAPE.FOR. Comments C from READTAPE.FOR are included below. C C 4/97 K.L. Perry C C c***************************** READTAPE ************************** c c This program reads the JPL-UCLA-AES Dealiased Gridded Surface c Wind Vectors data set described in the NODS Data Archives c Contents Document. c c This program reads in global 1x1 degree gridded synoptic c wind fields of Seasat scatterometer data dealiased and produced c as described in Peteherych et al., 1984, Proceedings of the URSI c Commision F Symposium and Workshop, Shoresh, Israel, May 14-23, c NASA Conf. Publ. CP-2303, 575-585, and Wurtele et al., 1982, c "Wind direction alias removal studies of Seasat scatterometer c derived wind fields", Journal of Geophysical Research, 87, 3365-77. c c The field parameters are: c c u(ni,nj) - zonal wind component, in m/s c v(ni,nj) - meridional wind component, in m/s c ia(ni,nj) - data quality flag c (a quality flag which is greater than 3 implies good data) c (a quality flag which is less than 4 implies good data) c c The arrays cover 1x1 degree gridded fields from 70S -> 70N, 1E -> 360E c at 6-hour intervals starting from 00z:6-Sep-78 to 18z:20-Sep-78. c c The tape is written at 6250 bpi with recl=2160, block=32400. Each c global field is contained in one file with an EOF mark at the end c of each file. c c******************************************************************* C C Declare Variables integer ni,nj parameter(ni=360) C =gridded longitude (1 East to 360 East) parameter(nj=141) C =gridded latitude (70 South to 70 North) character*6 indata(ni*nj*3) real utmp(ni*nj),vtmp(ni*nj) integer iatmp(ni*nj) real u(ni,nj),v(ni,nj) integer ia(ni,nj) integer lon(ni),lat(nj) integer i,j,n C Open and read the input file C C Please note that the data are not stored as 2D arrays. C They are stored in one giant 1D array (ie, 1 row which C contains 360x241x3 values) open(1,file='syn19780907.18z') read(1,91) (indata(i),i=1,ni*nj*3) 91 format(1552280a6) close(1) C Convert the character array do 100 i=1,ni*nj read(indata(i),'(f6.2)') utmp(i) read(indata(i+ni*nj),'(f6.2)') vtmp(i) read(indata(i+ni*nj*2),'(i6)') iatmp(i) 100 continue C Convert the one dimensional arrays to 2D arrays C Calculate the latitude and longitude n=1 do 300 j=1,nj do 200 i=1,ni u(i,j)=utmp(n) v(i,j)=vtmp(n) ia(i,j)=iatmp(n) lon(i)=i n=n+1 200 continue lat(j)=j-71 300 continue C Write the output do 500 j=1,nj do 400 i=1,ni if (ia(i,j).gt.0) then write(*,*) lat(j),lon(i),u(i,j),v(i,j),ia(i,j) endif 400 continue 500 continue stop end
Phone: (626) 744-5508
Fax: (626) 744-5506
Email:
podaac@podaac.jpl.nasa.gov
URL:
http://podaac.jpl.nasa.gov
Orders can also be placed through the Earth Observing System Data Gateway (EDG) http://podaac.jpl.nasa.gov/imswelcome.
Boggs, D. H.,1982. Seasat Scatterometer Geophysical Data Record (GDR) Users Handbook, JPL Document D-129, Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA.
Brown, R.A., V.J. Cardone, T. Guymer, J. Hawkins, J.E. Overland, W.J. Pierson, S. Peteherych, J.C. Wilkerson, P.M. Woiceshyn, and M. Wurtele, 1982.Surface Wind Analyses for SEASAT, J. Geophys. Res., 87, 3355-3364.
Jones, W.L., L.C. Schroeder, D.H. Boggs, E.M. Bracalente, R.A. Brown, G.J. Dome, W.J. Pierson, and F.J. Wentz, 1982. The SEASAT-A Satellite Scatterometer: The Geophysical Evaluation of Remotely Sensed Wind Vectors Over the Ocean, J. Geophys. Res., 87, 3297-3317.
Wentz, F.J., S. Peteherych, and L.A. Thomas, 1984. A Model Function for Ocean Radar Cross Sections at 14.6 GHz, J. Geophys. Res., 89, 3689-3704.
Wurtele, M.G., P.M. Woiceshyn, S. Peteherych, M. Borowski, and W.S. Appleby, 1982. Wind Direction Alias Removal Studies of SEASAT Scatterometer-Derived Wind Fields, J. Geophys. Res., 87, 3365-3377.
SIGMA-0 (SIGMA-NAUGHT)
Normalized Radar Cross-Section.
See the EOSDIS Glossary for a more general listing of terms related to the Earth Observing System project.