2013
DOI: 10.1007/s00190-013-0650-3
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The static gravity field model DGM-1S from GRACE and GOCE data: computation, validation and an analysis of GOCE mission’s added value

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Cited by 48 publications
(32 citation statements)
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“…The reference ISA residuals are obtained as the difference between the observed ISA and the modelled ISA. The modelled ISAs are computed with state-of-the-art force models, which comprise the static gravity field model DGM-1S (Farahani et al 2013b), the corresponding mean monthly gravity field solution DMT-2 [data processing details in Farahani (2013)], tidal model EOT11a (Savcenko and Bosch 2012), the model of non-tidal mass redistribution in the atmosphere and oceans AOD1B RL05 (Flechtner et al 2014), L1B RL02 products, and other tidal and relativistic effects. Because the monthly gravity field solution is included in the background force model, all known signals are removed from the reference ISA residuals.…”
Section: Propagation Of Attitude Errors Into Inter-satellite Acceleramentioning
confidence: 99%
“…The reference ISA residuals are obtained as the difference between the observed ISA and the modelled ISA. The modelled ISAs are computed with state-of-the-art force models, which comprise the static gravity field model DGM-1S (Farahani et al 2013b), the corresponding mean monthly gravity field solution DMT-2 [data processing details in Farahani (2013)], tidal model EOT11a (Savcenko and Bosch 2012), the model of non-tidal mass redistribution in the atmosphere and oceans AOD1B RL05 (Flechtner et al 2014), L1B RL02 products, and other tidal and relativistic effects. Because the monthly gravity field solution is included in the background force model, all known signals are removed from the reference ISA residuals.…”
Section: Propagation Of Attitude Errors Into Inter-satellite Acceleramentioning
confidence: 99%
“…1) using Poisson wavelets of order 3 (Holschneider and IglewskaNowak 2007). They belong to the class of spherical radial base functions (SRBFs), which have become popular in regional gravity field modelling (e.g., Schmidt et al 2007;Klees et al 2007Klees et al , 2008Eicker 2008;Tenzer and Klees 2008;Wittwer 2009;Panet et al 2011;Slobbe 2013). The horizontal positions of the SRBFs are located on a Fibonacci point distribution (e.g., González 2010), one of several homogeneous point distributions on the sphere.…”
Section: Parameterizationmentioning
confidence: 99%
“…In our case, we found that a second iteration is not necessary. It is worth noting that a similar iterative scheme was successfully applied by Farahani (2013) and Farahani et al (2013Farahani et al ( , 2014 to deal with coloured noise in GRACE inter-satellite accelerations and GOCE gravity gradients in the context of global gravity field modelling. Figure 3 also shows the final √ PSDs of noise for CryoSat-2 and Geosat phase D GM data.…”
Section: Noise Estimation and Modellingmentioning
confidence: 99%
“…For models such as GOCO05s (Mayer-Gürr et al 2015), the quality of the noise covariance matrix benefits from (i) a post-fit residual analysis, which provides more realistic models of the data noise (e.g. Farahani et al 2013), and (ii) numerically efficient algorithms to propagate the full data noise covariance matrices into the noise covariance matrix of the estimated spherical harmonic coefficients (e.g. Farahani et al 2013).…”
Section: Introductionmentioning
confidence: 99%
“…Farahani et al 2013), and (ii) numerically efficient algorithms to propagate the full data noise covariance matrices into the noise covariance matrix of the estimated spherical harmonic coefficients (e.g. Farahani et al 2013). Some progress has also been made regarding high-resolution datasets frequently used in local quasi-geoid modelling.…”
Section: Introductionmentioning
confidence: 99%