User Services Office
Physical Oceanography Distributed Active Archive Center (PO.DAAC)
Jet Propulsion Laboratory (JPL)
Phone: (626) 744-5508
Fax: (626) 744-5506
Email:
podaac@podaac.jpl.nasa.gov
URL:
http://podaac.jpl.nasa.gov
GEOS-3 Satellite Altimeter Geometry
Within battery power constraints, altimeter data can be taken whenever the satellite is within view of a telemetry site, with data always transmitted in near real time. No storage of data is possible on board the spacecraft, although some averaging of data prior to transmission is possible. In addition transmision may also be via an S-band link through ATS-6, so that more than half a revolution of continuous visibility of GEOS-3 is possible for those missions for which ATS-6 is scheduled.
The major calibrations considered necessary for the built-in test/calibration system were time delay (bias), AGC/gain, and waveform calibration. Internally generated signals are provided for calibration. A 10-second time delay (bias) test is performed in each mode to determine the bias to within the required one meter. In each mode, a two-point AGC/gain calibration is obtained using IF reference pulses. For waveform calibration, controlled video waveforms are used in both modes. [Hofmeister et al., 1976]
The figure below displays the flow of raw telemetry data employed during the GEOS-3 mission. Data acquired at the NASA STDN sites (including ROSMAN and Madrid ATS-6 stations) were routed to the NASA Wallops telemetry station eigher in real-time using data communications, or analog tapes were recorded at the sites and then mailed to Wallops. At the Wallops telemetry station, the data (either real-time or on analog tapes) were digitized to provide a computer campatible tape for further processing in the altimeter data reduction programs. In the case of data acquired at the DoD telemetry sites, these data were digitized by DoD and made available for processing at Wallops in the same altimeter data reduction programs. [Stanley and Dwyer, 1980]
GEOS-3 Data Flow
The records appear in chronological order and are separated into passes by the presence of header records before the first data record of each pass. The header records were inserted when either a time gap exceeding 15 seconds occurred in the data or the pass traversed more than the physical limit, approximately 12,400 sq km.
GEOS-3 Altimeter Data Records
FIELD BYTES UNITS CONTENT ----- ----- ----- ---------------------------------------------- 1 1-4 DAYS MODIFIED JULIAN DATE OF OBSERVATION (JULIAN DATE - 2,400,000.5 DAYS) 2 5-8 SECONDS TIME FROM BEGINNING OF DAY 3 9-12 10**-6 SECS CONTINUATION OF TIME TO THE MICROSECOND 4 13-16 10**-6 DEG GEODETIC LATITUDE 5 17-20 10**-6 DEG EAST LONGITUDE 6 21-24 MM SMOOTHED SEA SURFACE HEIGHT ABOVE ELLIPSOID WITHOUT TIDE OR OTHER MODEL CORRECTIONS (A = 6378145 METERS, F=1/298.255) 7 25-28 MM SATELLITE HEIGHT ABOVE ELLIPSOID 8 29-30 MM SCHWIDERSKI TIDE HEIGHT ABOVE MEAN SURFACE WITH 9 TERMS INCLUDED (M2, S2, K1, O1, N2, P1, K2, Q1, MF) 9 31-32 MM CARTWRIGHT'S SOLID TIDE HEIGHT WITH ZERO FREQUENCY TERM NOT INCLUDED, H2=.61, H3=.29 10 33-34 CM H 1/3, SIGNIFICANT WAVE HEIGHT 11 35-36 10**-3 SURFACE REFLECTIVITY (SIGMA NAUGHT) 12 37-38 CM/SEC WIND SPEED 13 39-40 10**-2 SWELL COEFFICIENT (GAMMA) 14 41-42 10**-4 DEG POINTING ANGLE 15 43-44 10**-2 FRAME AVERAGE MEAN SQUARED SLOPE 16 45-46 10**-2 DB AUTOMATIC GAIN CONTROL 17 47-48 INDEX OF ICE PROBABILITY 18 49-50 REVOLUTION NUMBER OF ORBIT 19 51-52 STATUS BITS (1,2,3,...16) 1 0 (INTENSIVE), 1 (GLOBAL) MODE 2 0 (), 1 (MODIFIED KALMAN EDIT) 3 0 (LOW), 1 (HIGH) DATA RATE 4 0 (ALL), (ANY/ALL NON) AUTO TRACK 5 0 (NO), 1 () APG/AASG EDIT 6 0 (NO), 1 (ORIGINAL) KALMAN EDIT 7-16 0 (WATER, 1 (LANDOR ICE) THIS 10 BIT FIELD REPRESENTS LOCATIONS ALONG THE GROUND TRACK SPACED AT .1024 SECONDS
Multiples of 20 or 32 observations per frame led to selecting a 10-point filter for low-rate data and an 8-point filter for high-rate data. In both cases, the largest and smallest values were removed and the remaining 8 or 6 points meaned. The means were assigned times at the midpoint of the 10- or 8-point span to preserve equal spacing. Consequently, passes of low-and high-rate data have different spacing of about 1.024 and 0.8192 seconds, respectively.
The other variables were computed in a manner that maintains the original precision. The latitude and east longitude values were linearly interpolated from frame values; satellite heights were quadratically interpolated. The Schwiderski oean- and Cartwright solid-tide heights are computed independently of the altimeter tapesi using software developed by Clyde E. Goad of NGS. The ocean tide computation consists of the M2, S2, K1, O1, N2, P1, K2, Q1 and MF components. The solid-Earth tide ignores the zero frequency term and uses values of H2=0.61 and H3=0.29.
The remaining fields of each compressed data record are frame values except for the automatic gain control (AGC) and the status bits. The AGC is a mean of the eight or six values corresponding to the trimmed set of sea heights. There are two or four relevant status samples per frame for the low-or high-rate data.
Figure 1. Compressed surface heights, April 19, 1976
Figure 2. Smoothed surface heights, April 19, 1976
The best estimates of the biases are
Intensive Mode | -5.30 m | ± 0.21 m |
Global Mode | -3.55 m | ± 0.42 m |
NOTE: The negative signs indicate that the measured altitudes are too short. The data is corrected by subtracting the above bias numbers for the respective modes.
The time tag correction that should be applied consists of
-20.8 msec + 1 interpulse period (10.240512 msec).
The noise figure of the GEOS-3 altimeter coupled with orbital tracking errors have prevented the direct use of this altimetry data in detailed studies, such as ocean circulation and surface velocity.
Since no further attention was given to the original observations beyond each 8 or 10 points, there were occasions when a group of partially or completely bad heights was compressed to a single bad height. Thus, users of the data must be cautious of these spurious values. The decision to keep these values on the tape was primarily based on the consideration of simplicity and respect for the other data fields which might be useful to investigators. Users are intentionally placed in a position of editing the compressed sea surface heights to their own satisfaction.
ftp://podaac.jpl.nasa.gov/pub/sea_surface_height/geos3
Phone: (626) 744-5508
Fax: (626) 744-5506
Email:
podaac@podaac.jpl.nasa.gov
URL:
http://podaac.jpl.nasa.gov
ftp podaac.jpl.nasa.gov
name: anonymous
password: use email address
cd /pub/sea_surface_height/geos3
Cartwright, D.E. and A.C. Edden, 1973. Corrected tables of tidal harmonics, Geophysical Journal, 33, 253-264.
Hofmeister, E.L., B.N. Keeney, T.W. Godbey, and R.J. Berg, 1976. Data User's Handbook and Design Error Analysis: GEOS-3 Radar Altimeter Volume I, NASA CR-156870, National Aeronautics and Space Administration, 540 pp.
Leitao, C.D., N.E. Huang, and C.G. Parra, 1978. Remote Sensing of Gulf Stream Using GEOS-3 Radar Altimeter, NASA Technical Paper 1209, National Aeronautics and Space Administration, 31 pp.
Martin, C.F., 1977. Altimeter Error Sources at the 10-cm Permormance Level, NASA CR-141420, National Aeronautics and Space Administration, 63 pp.
Martin, C.F. and M.L. Butler, 1977. Calibration Results for the GEOS-3 Altimeter, NASA CR-141430, National Aeronautics and Space Administration, 119 pp.
Rufenach, C.L. and W.R. Alpers, 1978. Measurement of Ocean Wave Heights Using the Geos 3 Altimeter, Journal of Geophysical Research, Vol. 83, C10, 5011-5018.
Schwiderski, E.W., 1980. On charting global ocean tides, Reviews of Geophysics and Space Physics, 18(1), 243-268.
Stanley, H.R. and R.E. Dwyer, 1980. NASA Wallops Flight Center GEOS-3 Altimeter Data Processing Report, NASA Reference Publication 1066, National Aeronautics and Space Administration, 130 pp.