Gravity anomaly

Gravity anomalies are widely used in geodesy and geophysics. A gravity anomaly is the difference between the observed gravity and its theoretical value, which is calculated at the surface of an global spheroid (ellipsoid of Hayford or WGS84) by rather simple formulas (2 functions of latitude).

The observed value of gravity has to be reduced down to the zero level of the geoid, using

  1. the elevation of the point where gravimetry was done
  2. the normal gradient of gravity (rate of change of gravity for change of elevation), as in free air, usually 0.3086 milligals per meter
    • or the Bouguer gradient of 0.1967 milligals/m which considers the mean rock density (2.67 g/cm³) below of the point
  3. and (in special cases) a terrain model, using a map or a digital terrain model (DTM).
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Nj_cboug.jpg
(Bouguer) gravity anomaly map of the state of New Jersey (USGS)

For these reduction, different methods are used:

The Bouguer anomalies usually are negative in the mountains because of isostasy: the rock density of their roots is lower, compared with the surrounding earth's mantle. Typical anomalies in the Central alps are -150 milligals.
Rather local anomalies are used in applied geophysics: if they e.g. are positive, this may indicate metallic ores.

See also: Physical geodesy, gravity, vertical deflection

External links

See also: Gravity anomaly, Anomaly, Borehole, Bouguer anomaly, Density, Earth's mantle, Elevation, Ellipsoid, Faye, Free-air anomaly