1887
ASEG2009 - 20th Geophysical Conference
  • ISSN: 2202-0586
  • E-ISSN:

Abstract

Introduction

Researchers involved in induced polarization studies are well familiar with Seigel’s (1959) definition of the chargeability parameter as the ratio of the secondary potential drop immediately after an infinitely long injected current is turned off, to the primary potential drop that builds up at the end of the current pulse. A major advantage of Seigel’s formulation is that it allows to recover the intrinsic chargeability of the subsurface applying a simple perturbation to the sensitivity matrix of the background resistivity (i.e. not affected by IP effects) model. In fact he proved that the apparent chargeability above an heterogeneous earth is simply

(1)  

where and represent the intrinsic chargeability and background resistivity of the media (for a layered earth, layers) that compose the subsurface, and the apparent background resistivity. This important result implies that the chargeability model can be readily obtained after the resistivity model has been recovered, and forms the basis of well established time domain IP inversion techniques (Li and Oldenburg, 2000a; Loke, 1999; Oldenburg and Li, 1994; Sogade et al., 2006). This manuscript aims at showing a fundamental discrepancy between Seigel’s fundamental theory and many different well accepted IP models. While contradicting in practice Seigel’s model, these other models do make use of important mathematical formulation that Seigel derived from his model.

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/content/journals/10.1071/ASEG2009ab103
2009-12-01
2026-01-19
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References

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  • Article Type: Research Article
Keyword(s): chargeability; inversion; mathematical formulation; TDIP
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