The self-attraction correction for the FG5X absolute gravity meter

The gravitational attraction of the body of a gravity meter upon its own proof mass is sometimes called the self-attraction. The self-attraction is a source of systematic error for absolute measurements of g, the acceleration of an object due to Earth's gravity. While the effect is typically sm...

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Veröffentlicht in:Metrologia 2013-02, Vol.50 (1), p.1-8
Hauptverfasser: Niebauer, T M, Billson, Ryan, Schiel, Aaron, van Westrum, Derek, Klopping, Fred
Format: Artikel
Sprache:eng
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Zusammenfassung:The gravitational attraction of the body of a gravity meter upon its own proof mass is sometimes called the self-attraction. The self-attraction is a source of systematic error for absolute measurements of g, the acceleration of an object due to Earth's gravity. While the effect is typically small-of the order of one part per billion of the Earth's gravitational attraction-it is significant at the current level of accuracy of absolute gravity meters. In the past, a self-attraction correction for the FG5 gravity meter has been estimated by considering a rather coarse description of the instrument using simple geometrical shapes (spheres and cylinders). This paper describes a more complete calculation using a CAD-based digitized model of the newest FG5X instrument. We have also included the attraction of the co-moving drag-free chamber as well as the self-attraction of the counterweights used in the FG5X to reduce recoil. The results are also applicable to older style FG5 instruments with a fibre-optic interferometer base. The correction found with this new approach agrees with previous estimates but is now based upon a more complete and accurate model.
ISSN:0026-1394
1681-7575
DOI:10.1088/0026-1394/50/1/1