Abstract
Temporal variations of atmospheric density distribution induce changes in the gravitational air mass attraction at a specific observation site. Additionally, the load of the atmospheric masses deforms the Earth’s crust and the sea surface. Variations in the local gravity acceleration and atmospheric pressure are known to be corrected with an admittance of about 3 nm/s2 per hPa as a standard factor, which is in accordance with the IAG Resolution No. 9, 1983. A more accurate admittance factor for a gravity station is varying with time and depends on the total global mass distribution within the atmosphere. The Institut für Erdmessung (IfE) performed absolute gravity observations in the Fennoscandian land uplift area nearly every year from 2003 to 2008. The objective is to ensure a reduction with 3 nm/s2 accuracy. Therefore, atmospheric gravity changes are modeled using globally distributed ECMWF data. The attraction effect from the local zone around the gravity station is calculated with ECMWF 3D weather data describing different pressure levels up to a height of 50 km. To model the regional and global attraction, and all deformation components the Green’s functions method and surface ECMWF 2D weather data are used. For the annually performed absolute gravimetry determinations, this approach improved the reductions by 8 nm/s2 (-19 nm/s2 to +4 nm/s2). The gravity modeling was verified using superconducting gravimeter data at station Membach inBelgiumimproving the residuals by about 15%.
Highlights
Since the end of last glacial period the Fennoscandian shield rises in the uplift centre about 1 cm per year resp. −16 nm/s2 per cm, cf. [1]
The results are applied to high-precision gravity data of superconducting gravimeter in Membach and to absolute observations in the Fennoscandia with FG5-220
The used method is based on globally distributed ECMWF weather data, whereby the globe was divided into three zones around the computation point: local, regional, and global zone
Summary
Since the end of last glacial period the Fennoscandian shield rises in the uplift centre about 1 cm per year resp. −16 nm/s2 per cm, cf. [1]. A joint project for gravimetric surveys of the land uplift in Fennoscandia was established in 2003 within a multinational cooperation. Annual measurements with the absolute gravimeter were performed in Fennoscandia from 2003 to 2008 by the Institut für Erdmessung (IfE) from the Leibniz Universität Hannover, Germany. In [5] a summary of all gravity measurements and the results of the IfE surveys are given. The gravimeter measures effects of different sources and is an “integral” sensor. The observations have to be reduced by time variable gravity changes due to solid Earth and ocean tides, polar motion, and atmospheric variations. Atmospheric mass redistributions cause temporal variations of density and of gravity of several 100 nm/s2. Continuous records with superconducting gravimeters, VLBI, GPS, and SLR techniques, cf. [7,8,9,10,11,12,13,14,15,16,17,18]
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