The omission error modelling of global gravity field models using different digital terrain models
Martin Pitoňák1, Matej Varga2, Michal Šprlák1
Gravity disturbances over test areas:
a) Czechia, b) Slovakia and c) southern
Colorado.
1NTIS – New Technologies for the Information Society, Faculty of Applied Sciences, University of West Bohemia, Pilsen, Czechia
2Institute of Geodesy and Photogrammetry, GSEG, ETH Zürich, Switzerland
The main goal of this contribution is to compare different approaches for modelling the omission error which could be one error source among many others in geoid determination. To do so we employ gravity disturbances over three test areas, namely, Czechia, Slovakia and southern Colorado. Firstly we subtract the high frequency part of gravitational field generated from the XGM2019e_2159 (Zingerle et al., 2019) model up to the degree 2160 terrestrial datasets. Then we will model the omitted signal in XGM2019e_2159 by (i) the topographic gravity field model dV_ELL_Earth_5480 (Rexer et al. 2017), (ii) the Earth’s short-scale gravity field models ERTM2160 (Hirt et al., 2014) and SRTM2gravity (Hirt et al., 2019) and by (iii) the forward modelling of residual topographic masses in spatial domain. Residual topographic masses were represented as differences between selected global (or near-global) digital elevation models such as AW3D30 (Tadano et al., 2014), ACE2 (Berry et al., 2010), MERIT DEM (Yamazaki et al., 2017), and SRTM 4.1 (Jarvis et al., 2008) and EARTH2014 (Hirt and Rexer 2015).
Results:
�
b)
c)
| XGM2019 | dV_ELL_Earth_5480 | AW3D30 | ACE2 | MERIT | SRTM4.1 | ERTM2160 | SRTM2gravity |
CZECHIA | ||||||||
STD | 11,152 | 8,102 | 9,568 | 9,718 | 9,741 | 9,642 | 7,287 | 7,282 |
MAX | 50,773 | 52,409 | 47,210 | 47,169 | 47,045 | 47,277 | 51,868 | 52,203 |
MIN | -32,225 | -33,327 | -31,171 | -31,514 | -31,302 | -31,371 | -35,845 | -36,247 |
MEAN | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 |
SLOVAKIA | ||||||||
STD | 13,496 | 9,021 | 8,211 | 8,240 | 8,213 | 8,269 | 7,222 | 7,163 |
MAX | 34,530 | 33,679 | 25,016 | 25,169 | 26,899 | 25,109 | 24,912 | 24,296 |
MIN | -46,546 | -35,212 | -32,283 | -31,059 | -30,783 | -30,511 | -39,004 | -38,390 |
MEAN | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 |
COLORADO | ||||||||
STD | 16,205 | 12,013 | 9,306 | 9,629 | 9,346 | 9,629 | 6,483 | 6,028 |
MAX | 30,601 | 20,774 | 28,013 | 31,347 | 28,301 | 31,347 | 13,304 | 14,581 |
MIN | -52,763 | -38,334 | -20,787 | -21,075 | -20,982 | -21,075 | -17,702 | -17,014 |
MEAN | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 | 0,000 |
RTM: r1=0.1° (polyhedron), r2=0.5° (prism), r3=1° (tesseroid), r4=5° (point-mass). In the fourth-zone we used ACE2 with spatial resolution of 9’’. We took advantage of TGF software (Yang et al., 2020).
Conclusion:
a)
r = 6365478.5 m
r = 6366154 m
r = 6377176.353 m
Acknowledgment: This contribution was supported by project HR Award of University of West Bohemia and by the project No. 21-13713S of the Czech Science Foundation