International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy 1 GOCE data...
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International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy1
GOCE data for local geoid enhancement
Matija Herceg Per Knudsen
Carl Christian Tscherning
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy2
Motivation and objectives
• The success of GOCE depends on adequate methodologies for extracting the gravity field from its observations and on combining the gravity field with information from other sources
• Development of a method for regional gravity field recovery by using GOCE gradients in addition to the global models
• Use enhanced geoid for determination of MDT
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy3
The RPM method• The Earth anomalous gravity field at point Q is modeled by a
set of base functions, each obtained as the anomalous gravity potential from each point
• Point mass functions are harmonic functions, which may be used to represent the anomalous gravity potential T
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy4
The RPM method• Closed expresions are calculated by:
• For reduction of point masses, the derivative of the sum of a finite Legendre series is used:
• computed using a recursion algorithm (Tscherning and Rapp 1974)
• Reduced point masses
n
ll
ll tPsaS
0
1 )(
2
2
p
R
rVV
5
222
3
)(31
ltrr
lV qpC
RC VVV
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy5
The RPM method
Fitting the function of different gravity field quantities to the empirical covariance function
All gravity anomalies Marine gravity anomalies
GOCE Tzz gradient anomalies
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy6
Local gravity field modelling results
Gravity anomaly in region between Greenland and the United Kingdom (GOCINA)
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy7
Local gravity field modelling results
Reduced geoid in the GOCINA region
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy8
Tzz gradient anomaly prediction [E], where the contribution from the EGM2008 up to harmonic degree and order 100 is subtracted
Local gravity field modelling resultsObservations Prediction
Difference
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy9
Local gravity field modelling resultsCol prediction RPM prediction
Difference
Gravity anomaly prediction (LSC and RPM) comparison [mGal], where the contribution from the EGM2008 up to harmonic degree and order 100 is subtracted
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy10
Local gravity field modelling results
Geoid height prediction (LSC and RPM) comparison [m], where the contribution from the EGM2008 up to harmonic degree and order 100 is subtracted
Col prediction
Difference
RPM prediction
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy11
Power spectrum of the geoid height anomaly prediction when EGM2008 up to harmonic degree and order 100 is subtracted. The prediction is done by the LSC and the RPM
methods with different datasets
Local gravity field modelling results
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy12
Mean Dynamic Topography
GOCE Direct MDT
GOCE Direct enhanced MDT
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy13
Mean Dynamic Topography
GOCINA project MDTMaximenko MDTDTU10 MDT
GOCE Direct MDT GOCE Direct enhanced MDT
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy14
Current speed
GOCINA project MDT current speed
Maximenko MDT current speed
DTU10 MDT current speed
GOCE Direct MDT current speed
GOCE Direct enhanced MDT current speed
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy15
• The GOCE Direct MDT current speeds reveal all the gross features of the general circulation in the region
• Does not show improvement over the GOCE Direct MDT
Power spectrum of different derived MDT
Current speeds
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy16
Conclusions• LSC and RPM methods give similar results when the selected GOCE
gradient dataset is used• Using all available GOCE gradients leads to improvement in the
geoid height anomaly prediction• GOCE data provides a better estimation of the MDT in the GOCINA
region than any previously obtained using only satellite observations. It could not be concluded whether the enhanced geoid model contribute to a further improvement of the MDT in the GOCINA area
• GOCE Direct MDT surface geostrophic currents reveal all of the gross features of the general circulation
• GOCINA project shows the smallest scale details, which makes it still the best ocean circulation representation in this region
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, ItalyInternational Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy17
Future work
• Resolve the issues related to the mean value of the data• Use real error degree variances when computing the RPM
response• Use all GOCE gravity gradients• In the regions with higher gravity anomaly signal oscillations,
i.e. mountain regions, GOCE gradients can possibly provide higher geoid enhancements than the ones shown here
• Removing short wavelength signal from the GOCE gradients
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy18
The RPM method regularization
– Adding a diagonal matrix to the normal equations matrix (one, degree dependent factors, or degree variances)
– Diagonal matrix is scaled by a regularization parameter empirically determined, based on a trade-off between the strength of the regularization and the fit to the given observations
– Squared mean error of the input GOCE gradients 0.01 E
International Symposium on Gravity, Geoid and Height Systems GGHS 2012, Venice, Italy19
Power spectrum of the geoid height anomaly prediction when GOCE Direct r3 model up to harmonic degree and order 240 is subtracted. The prediction is done by the LSC
and the RPM methods with different datasets
Local gravity field modelling results