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Gravity Field Model GPM3E97A
- by Georg Wenzel
-
The European Gravimetric Geoid (Denker
and Torge 1998, Denker 1998) is available to the scientific community,
representing a milestone in the development of the European Geoid.
Unfortunateley, the published CD-rom does not contain the free air gravity
anomalies which have been used for the computation of EGG97. The computation
of high resolution free air gravity anomalies from the published EGG97 quasi
geoid heights using an ultra high degree geopotential model is therefore
subject of this paper.
-
Using integral formulas in an
iterative algorithm, three very high degree geopotential models have been
computed from EGG97: GPM3E97C to degree 720, GPM3E97B to degree 1080, and
GPM3E97A to degree 1800. For GPM3E97A, about 800000 mean 5' x 5' quasi geoid
heights from EGG97 have been used inside Europe (25 deg < lat < 77
deg, -35.0 deg < lon < 67.4 deg) and about 8 million mean 5' x 5'
quasi geoid heights computed from geopotential model EGM96 to degree 360
have been used outside Europe. The rms discrepancy between the input quasi
geoid heights and quasi geoid heights computed from GPM3E97A is 0.005 m with
0.295 m maximum discrepancy (this results from the lack of resolution of
GPM3E97A compared to EGG97
EGM96 The NASA GSFC and NIMA Joint Geopotential Model
-
Welcome to the official webpage of the NASA and NIMA joint
geopotential model, EGM96. EGM96 is a spherical harmonic model of the
Earth's gravitational potential complete to degree and order 360. On this
website, we summarize the development of this model, and include information
presented at the International Symposium on Gravity, Geoid, and Marine
Geodesy, Tokyo, Japan, September 30 - October 4, 1996.
-
EGM96 The NASA GSFC and NIMA Joint Geopotential Model
Report
- Presented at IUGG99, IAG Section III "Determination of the Gravity
Field", Birmingham, July 18 - 30, 1999
DGFI Homepage
- Global Gravity Field Models
- International Services, FAGS,
IERS, IGS, IVL, ILRS, PSMSL -
- Goddard Space
Flight Center contact: E.
Pavlis
- GFZ:
GeoForschungsZentrum), Potsdam, Germany contact: P. Schwintzer
- GRGS: Groupe de Recherche de Geodesie Spatial) of CNES, the French space
agency contact: R. Biancale
- CSR: Center of Space
Research, Texas University, Austin, Texas contact: C.K.Shum
- ssg3167
- This paper summarizes the activities and achievements of the IAG Special Study
Group (SSG) 3.167: "Regional Land and Marine Geoid Modelling", which
was established by the XXIth General Assembly of IAG held in Boulder, Colorado,
USA, July 3-14, 1995. SSG3.165 Global Gravity Field Determination
and Evaluation Chairman: N. Pavlis
IAG-Special Commission SC7 (Institute of Theoretical Geodesy)
- The Special Commission will act as a forum of discussion and information
related to these various missions. Besides these topics the Special Commission
should also act as a brain pool for ideas of future developments in gravity
field research. This encompasses not only applications to various fields of
geo sciences but also developments of future satellite borne techniques to
measure the gravity field.
- Satellite gradiometry is superior for obtaining high spatial resolution
from a moderate mission length. A recent study showed that increase of
measurement precision or decrease of altitude results in a clear gain of
spatial resolution in case of SGG, while this effect is very moderate in
case of SST. A SGG mission like GOCE is superior in the short wavelengths
parts of the gravity field up to a spherical harmonics degree of 250. The
results of a mission like GOCE start to be better than those of a low-low
SST mission from degree 60 to 80 on. A high-low SST mission like CHAMP can
provide an improvement in the knowledge of the gravity field of
approximately one order of magnitude over present models for wavelengths
between 400 to 2000km.
gruen_161.html
- Gradiometry - an Inverse Problem in Modern Satellite Geodesy, Freeden, W.,
Schneider, F., Schreiner, M.
- Satellite gradiometry and its instrumentation is an ultra-sensitive
detection technique of the space gravitational gradient (i.e. the Hesse
tensor of the gravitational potential). Gradeometry will be of great
significance in inertial navigation, gravity survey, geodynamics and
earthquake prediction research. In this paper, satellite gradiometry
formulated as an inverse problem of satellite geodesy is discussed from two
mathematical aspects: Firstly, satellite gradiometry is considered as a
continuous problem of harmonic downward continuation. The space-borne
gravity gradients are assumed to be known continuously over the satellite
(orbit) surface. Our purpose is to specify sufficient conditions under which
uniqueness and existence can be guaranteed.
Earth Gravitational Model 1996 (EGM96) 1998
- This model of the Earth' gravitational filed was developed in a
collaborative effort of the NASA Goddard Space Flight Center, the National
Imagery and Mapping Agency (NIMA), and the Ohio State University. It is
based on surface gravity data, altimeter-derived gravity anomalies from
ERS-1 and from GEOSAT, extensive satellite tracking data (GPS, TDRSS, DORIS,
TRANET), and direct altimeter ranges from TOPEX/POSEIDON, ERS-1, and GEOSAT.
The spherical harmonics model includes terms up to degree 360.
The predecessor models are the OSU-91A (Rapp et al., 1991) and the JGM-2 (Nerem
et al., 1994) models.
- Please contact : F.G. Lemoine, NASA/GSFC, Laboratory for Terrestrial
Physics,
Greenbelt, Maryland 20771, (301) 286-2460, flemoine@ares.gsfc.nasa.gov
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