Measurement of Gravity for Study of Figure of the Earth

  • R. K. Verma
Chapter
Part of the Solid Earth Sciences Library book series (SESL, volume 3)

Abstract

Ever since 1687 when Sir Issac Newton gave his famous law of gravitation scientists all over the world have used it to study the figure of the earth. The law can be written as follows,
$$F = G \cdot \frac{{{m_1}{m_2}}}{{{r^2}}}$$
(1.1)
Where F is the force of attraction between two point masses m1 and m2 and r is the distance between them, G is the universal gravitational constant. The value of G has been determined by several workers including Henry Cavendish in 1798 and its latest value adopted is (6.673 ± 0.003) X 10−8 c.g.s. units (IUGG, 1967). In Equation (1.1) if we substitute m1 = 1 unit, m2 = M, the mass of the earth, R- the distance from the centre of gravity of the earth to its surface, we can write,
$$g = \frac{{GM}}{{{R^2}}}$$
(1.2)
Where g is the acceleration due to gravity. It is expressed in ft sec −2 or cm sec −2. Geophysicists generally use a unit of ‘gal’ which is defined as an acceleration of 1 cm sec−2. One milligal is 1/1000 of a gal.

Keywords

Rock Mass Bouguer Anomaly Terrain Correction Gravity Observation Topographic Correction 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© D. Reidel Publishing Company, Dordrecht, Holland 1985

Authors and Affiliations

  • R. K. Verma
    • 1
  1. 1.Indian School of MinesDhanbadIndia

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