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    Complete spherical Bouguer gravity anomalies over Australia

    135131_135131.pdf (1.650Mb)
    Access Status
    Open access
    Authors
    Kuhn, Michael
    Featherstone, Will
    Kirby, Jonathan
    Date
    2009
    Type
    Journal Article
    
    Metadata
    Show full item record
    Citation
    Kuhn, Michael and Featherstone, Will and Kirby, Jonathan. 2009. Complete spherical Bouguer gravity anomalies over Australia. Australian Journal of Earth Sciences. 56 (2): pp. 213-223.
    Source Title
    Australian Journal of Earth Sciences
    DOI
    10.1080/08120090802547041
    ISSN
    08120099
    Faculty
    Department of Spatial Sciences
    Faculty of Science and Engineering
    WA School of Mines
    URI
    http://hdl.handle.net/20.500.11937/34751
    Collection
    • Curtin Research Publications
    Abstract

    We have computed complete (or refined) spherical Bouguer gravity anomalies for all 1,095,065 land gravity observations in the June 2007 release of the Australian national gravity database. The spherical Bouguer shell contribution was computed using the supplied ground elevations of the gravity observations. The spherical terrain corrections, residual to each Bouguer shell, were computed on a 9 arc-second grid (~250 m by ~250 m spatial resolution) from a global Newtonian integration using heights from version 2.1 of the GEODATA digital elevation model (DEM) over Australia and the GLOBE and JGP95E global DEMs outside Australia. A constant topographic mass-density of 2670 kg/m3 was used for both the spherical Bouguer shell and spherical terrain correction terms. The difference between the complete spherical and complete planar Bouguer gravity anomaly exhibits an almost constant bias of about -18.7 mGal over areas with moderate elevation changes, thus verifying the planar model as a reasonable approximation in these areas. However, the results suggest that in mountainous areas with large elevation changes, the complete spherical Bouguer gravity anomaly should be selected in preference over the less rigorous complete planar counterpart.

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