1887
ASEG2003 - 16th Geophysical Conference
  • ISSN: 2202-0586
  • E-ISSN:

Abstract

Lithologies with high clay contents can have negative chargeability. This response is usually attributed to geometric effects in induced polarization and electromagnetic surveys. Negative chargeability has also been noted in laboratory studies, but has remained unexplained.

Traditional membrane polarisation models are of a series of membrane constrictions within a solid substrate, but this model produces only positive chargeability responses. Alternate soft clay polarisation model are considered, involving bulk sample ionic fluxes. These fluxes have been previously studied in electrokinetic dewatering and decontamination studies, but over longer time periods. Of particular note are the large pH gradients that form under an applied electric field. Relaxation of these gradients at the sample’s surface produces a potential in the opposite sign to the applied potential, and so produces negative chargeability.

Laboratory electrical impedance spectroscopy data is presented. The experimental data covers a variety of clay types at a variety of water contents. For pure clay samples, a relationship exists between negative chargeability and water content (as a percentage of liquid limit). This trend is not apparent in natural clays.

Field measurements of negative chargeability are presented. Logging data through a soft clay lithology is shown to discriminate between clay and sand layers.

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/content/journals/10.1071/ASEG2003ab017
2003-08-01
2026-01-14
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References

  1. Campanella, R. G. (1990). "Development and use of an electrical resistivity cone for groundwater contamination studies." Canadian Geotechnical Journal 27: 557-567.
  2. Carrier, M. and K. Soga (1999). "A four terminal measurement system for measuring the dielectric properties of clay at low frequencies." Engineering Geology 53: 115-123.
  3. Coster, H. G. L. and T. C. Chilcott (1999). The characterization of membranes and membrane surfaces using impedance spectroscopy. Surface chemistry and electrochemistry of membranes. Sorensen. Copenhagen, Denmark, Marcel Dekker Inc: 749-792.
  4. Hamed, J., Y. B. Acar, et al. (1991). "Pb(JI) removal from Kaolinite by electrokinetics." Journal of geotechnical engineering 117(No. 2): 241-271.
  5. Mitchell, J. K. (1993). Fundamentals of soil behaviour, John Wiley & Sons, Inc.
  6. Olhoeft, G. R. (1985). "Low-frequency electrical properties." Geophysics 50(12): 2492-2503.
  7. Parasnis, D. S. (1997). Principles of Applied Geophysics, Chapman and Hall.
  8. Roy, K. K. and H. M. Elliott (1980). "Model studies on some aspects of resistivity and membrane polarization behaviour over a layered earth." Geophysical prospecting 28: 759-775.
  9. Slater, L. D. and S. K. Sandberg (2000). "Resistivity and induced polarization monitoring of salt transport under natural hydraulic gradients." Geophysics 65: 408-420.
  10. Titov, K., V. Komarov, et al. (2002). "Theoretical and experimental study of time domain-induced polarization in water-saturated sands." Journal of Applied Geophysics 50: 417-433.
  11. Virkutye, J., M. Sillanpaa, et al. (2002). "Electrokinetic soil remediation - critical overview." The science of the total environment 289: 97-121.
/content/journals/10.1071/ASEG2003ab017
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  • Article Type: Research Article
Keyword(s): Clay; Induced Polarization; negative chargeability
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