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      Bars and spheroids in gravimetry problem

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          Abstract

          The direct gravimetry problem is solved by dividing each deposit body into a set of vertical adjoining bars, whereas in the inverse problem, each deposit body is modelled by a homogeneous ellipsoid of revolution (spheroid). Well-known formulae for the z-component of gravitational intensity for a spheroid are transformed to a convenient form. Parameters of a spheroid are determined by minimizing the Tikhonov smoothing functional with constraints on the parameters, which makes the ill-posed inverse problem by unique and stable. The Bulakh algorithm for initial estimating the depth and mass of a deposit is modified. The proposed technique is illustrated by numerical model examples of deposits in the form of two and five bodies. The inverse gravimetry problem is interpreted as a gravitational tomography problem or, in other words, as "introscopy" of Earth's crust and mantle.

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          Author and article information

          Journal
          2016-04-23
          Article
          1604.06927
          256dcbfe-43e0-43f0-8bc3-9ccc2abed889

          http://arxiv.org/licenses/nonexclusive-distrib/1.0/

          History
          Custom metadata
          41A29, 65C20, 65F22, 86A22
          24 pages, 12 figures. arXiv admin note: text overlap with arXiv:1508.04410
          math.NA physics.geo-ph

          Numerical & Computational mathematics,Geophysics
          Numerical & Computational mathematics, Geophysics

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