Interference potential

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In potential theory , the influence of an irregularity to be determined ( disruptive body ) on a physical force field is referred to as interference potential .

Most important is the calculation of interference potentials in the terrestrial magnetic field and in the earth's gravity field . In the latter case, the following applies to a measuring point :

With

  • : Symbol for the interference potential in geodetic and geophysical specialist literature
  • (or also ): Total potential or potential energy of the force field at the measuring point, in principle all the masses in the considered 3D space contribute to this.
  • : Normal potential (see below)
  • : Position vector with which all three potentials usually change.

In general, the potential itself can not be used to locate and later analyze the disruptive body , but only its measurable functionals , e.g. B. Gradients or solder disturbances .

Starting from a regular distribution of the charges or the masses in the vicinity of the measuring points can a normal field (corresponding defined) and the measurement (corresponding to are compared). The difference (corresponding ) is called the magnetic or gravity anomaly . It can be approximated to the determined deviations through model calculations, in that the disruptive body is quantitatively determined in the trial-and-error process through targeted changes in the assumed potential sources, which is also called inversion of the disruptive potential.

Such model variations are in the gravitational field z. B.

However, the inversion of a potential is usually not clear ( inversion problem in potential theory ) and requires additional data (e.g. about rocks) or additional measurement methods.

See also