G. B. Patel
STX Corporation
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Journal of Geophysical Research | 1994
R. S. Nerem; F. J. Lerch; J. A. Marshall; Erricos C. Pavlis; B. H. Putney; Byron D. Tapley; R. J. Eanes; John C. Ries; B. E. Schutz; C. K. Shum; M. M. Watkins; Steven M. Klosko; J. C. Chan; Scott B. Luthcke; G. B. Patel; Nikolaos K. Pavlis; R. G. Williamson; Richard H. Rapp; R. Biancale; F. Nouel
The TOPEX/POSEIDON (T/P) prelaunch Joint Gravity Model-1 (JGM-I) and the postlaunch JGM-2 Earth gravitational models have been developed to support precision orbit determination for T/P. Each of these models is complete to degree 70 in spherical harmonics and was computed from a combination of satellite tracking data, satellite altimetry, and surface gravimetry. While improved orbit determination accuracies for T/P have driven the improvements in the models, the models are general in application and also provide an improved geoid for oceanographic computations. The postlaunch model, JGM-2, which includes T/P satellite laser ranging (SLR) and Doppler orbitography and radiopositioning integrated by satellite (DORIS) tracking data, introduces radial orbit errors for T/P that are only 2 cm RMS with the commission errors of the marine geoid for terms to degree 70 being ±25 cm. Errors in modeling the nonconservative forces acting on T/P increase the total radial errors to only 3–4 cm RMS, a result much better than premission goals. While the orbit accuracy goal for T/P has been far surpassed, geoid errors still prevent the absolute determination of the ocean dynamic topography for wavelengths shorter than about 2500 km. Only a dedicated gravitational field satellite mission will likely provide the necessary improvement in the geoid.
Journal of Geophysical Research | 1993
David E. Smith; F. J. Lerch; R. S. Nerem; Maria T. Zuber; G. B. Patel; Susan K. Fricke; Frank G. Lemoine
Doppler tracking data of three orbiting spacecraft have been reanalyzed to develop a new gravitational field model for the planet Mars, Goddard Mars Model 1 (GMM-1). This model employs nearly all available data, consisting of approximately 1100 days of S band tracking data collected by NASAs Deep Space Network from the Mariner 9 and Viking 1 and Viking 2 spacecraft, in seven different orbits, between 1971 and 1979. GMM-1 is complete to spherical harmonic degree and order 50, which corresponds to a half-wavelength spatial resolution of 200–300 km where the data permit. GMM-1 represents satellite orbits with considerably better accuracy than previous Mars gravity models and shows greater resolution of identifiable geological structures. The notable improvement in GMM-1 over previous models is a consequence of several factors: improved computational capabilities, the use of optimum weighting and least squares collocation solution techniques which stabilized the behavior of the solution at high degree and order, and the use of longer satellite arcs than employed in previous solutions that were made possible by improved force and measurement models. The inclusion of X band tracking data from the 379-km altitude, near-polar orbiting Mars Observer spacecraft should provide a significant improvement over GMM-1, particularly at high latitudes where current data poorly resolve the gravitational signature of the planet.
IEEE Transactions on Geoscience and Remote Sensing | 1993
R. S. Nerem; B. H. Putney; J. A. Marshall; F. J. Lerch; Erricos C. Pavlis; Steven M. Klosko; Scott B. Luthcke; G. B. Patel; R. G. Williamson; Nikita P. Zelensky
The research that has been conducted in the Space Geodesy Branch at NASA/Goddard Space Flight Center in preparation for meeting the 13-cm radial orbit accuracy requirement for the TOPEX/Poseidon (T/P) mission is described. New developments in modeling the Earths gravitational field and modeling the complex nonconservative forces acting on T/P are highlighted. The T/P error budget is reviewed, and a prelaunch assessment of the predicted orbit determination accuracies is summarized. >
Journal of Geophysical Research | 1991
F. J. Lerch; James G. Marsh; S. M. Klosko; G. B. Patel; D. S. Chinn; Erricos C. Pavlis; Carl A. Wagner
Several tests have been designed to estimate the correct error variances for the GEM-T1 gravitational solution that was derived exclusively from satellite tracking data. The basic method uses both independent and dependent subset data solutions and produces a coefficient by coefficient estimate of the model uncertainties. The GEM-T1 errors have been further analyzed using a method based on eigenvalue-eigenvector analysis, which calibrates the entire covariance matrix. Dependent satellite data sets and independent altimetric, resonant satellite, and surface gravity data sets all confirm essentially the same error assessment The calibration test results yield very stable calibration factors, which vary only by approximately 10% over the range of tests performed. Based on these calibrated error estimates, GEM-T1 is a significantly improved solution, which to degree and order 8 is twice as accurate as earlier satellite derived models like GEM-L2. Also, by being complete to degree and order 36, GEM-T1 is more complete and has significantly reduced aliasing effects that were present in previous models.
Geophysical Research Letters | 1993
F. J. Lerch; R. S. Nerem; D. S. Chinn; J. C. Chan; G. B. Patel; S. M. Klosko
Orbit error projections based on the error covariance estimates of Goddard Earth Model (GEM)-T3 have been shown to be reliable through their projection on observation residuals within independent data sets. Special geopotential solutions were developed based upon the same data set and weighting used in the GEM-T3 gravity model, but with a significant satellite data set eliminated from the solution. These subset gravity models are then used to compute the observation residuals within orbital solutions for the omitted satellite and the results are compared to their predicted values based on the error covariance of these models. To ensure meaningful results, the tests were designed so that the observation residuals are dominated by geopotential modeling errors. This yields a reliable test of the error estimates of the subset solutions and hence tests the data weighting used in the construction of these models (GEM-T3 and subset solutions alike). The error estimates for GEM-T3 are based upon an optimal data weighting method and have been obtained in a separate calibration process. The test results shown here indicate that the GEM-T3 error estimates for the gravity parameters are calibrated and that the predicted orbit errors correspond well with actual orbit accuracies. Test results of the complete GEM-T3 model with totally independent high precision DORIS Doppler tracking data acquired on the French SPOT-2 satellite confirms these conclusions.
Geophysical Research Letters | 1982
F. J. Lerch; Steven M. Klosko; G. B. Patel
Journal of Geophysical Research | 1990
James G. Marsh; C. J. Koblinsky; F. J. Lerch; Steven M. Klosko; J. W. Robbins; R. G. Williamson; G. B. Patel
Journal of Geophysical Research | 1994
F. J. Lerch; R. S. Nerem; B. H. Putney; T. L. Felsentreger; B. V. Sanchez; J. A. Marshall; Steven M. Klosko; G. B. Patel; R. G. Williamson; D. S. Chinn; J. C. Chan; K. E. Rachlin; N. L. Chandler; J. J. McCarthy; Scott B. Luthcke; Nikolaos K. Pavlis; D. Pavlis; J. W. Robbins; S. Kapoor; Erricos C. Pavlis
Journal of Geophysical Research | 1985
F. J. Lerch; Steven M. Klosko; G. B. Patel; Carl A. Wagner
Journal of Geophysical Research | 1985
F. J. Lerch; Steven M. Klosko; Carl A. Wagner; G. B. Patel