Complex resistivity of mineral rocks in the context of the generalized effective-medium theory
of the IP effect
Vladimir Burtman*, University of Utah and TechnoImaging , Masashi Endo, TechnoImaging, Wei Lin,
University of Utah, and Michael S. Zhdanov, University of Utah and TechnoImaging
Summary
One of the major problems in mineral exploration is the
inability to reliably distinguish between economic mineral
deposits and uneconomic mineralization. While the mining
industry uses many geophysical methods to locate mineral
deposits, until recently, there was no reliable technology for
identification and characterization of mineral resources. The
main goal of this paper is an application of the generalized
effective-medium theory of induced polarization (GEMTIP)
to studying the complex resistivity of typical mineral rocks.
We collected representative rock samples from the Cu-Au
deposit in Mongolia, and subjected them to the
mineralogical analysis using Quantitative Evaluation of
Minerals by Scanning Electron Microscopy (QEMSCan)
technology. We also conducted an analysis of the electrical
properties of the same samples using the laboratory complex
resistivity (CR) measurement system. As a result, we have
established relationships between the mineral composition
of the rocks, determined using QEMSCan analysis, and the
parameters of the GEMTIP model defined from the lab
measurements of the electrical properties of the rocks. These
relationships open the possibility for remote estimation of
types of mineralization using spectral IP data.
Introduction
The physical-mathematical principles of the IP effect were
originally formulated in the pioneering works of Wait (1959,
1982) and Sheinman (1969). However, the IP method did not
find wide application in mineral exploration until the 1970's
with the work of Zonge (e.g., Zonge, 1974; Zonge and
Wynn, 1975) and Pelton (Pelton et al., 1977, Pelton, 1978).
Significant contributions were also made by Kennecott
research team between 1965 and 1977 (e.g., Nelson, 1997).
Over the last 40 years several conductivity relaxation models
have been developed, which provided quantitative
characterization of the electric charging phenomena,
including the empirical Cole-Cole model (Cole & Cole,
1941; Pelton et al., 1978), electrochemical model of
Ostrander & Zonge (1978), the GEMTIP model of Zhdanov
(2008), based on generalized effective-medium theory of
induced polarization, and electrochemical model of Revil et
al. (2013). The GEMTIP resistivity model uses the effective-
medium theory to describe the complex resistivity of
heterogeneous rocks and incorporates the physical and
electrical characteristics of rocks at the porous/grain scale
and translates them into an analytic expression for the
effective complex resistivity. It was shown in the paper by
Zhdanov (2008) that the widely accepted Cole-Cole model
is a special case of the GEMTIP model, where all the grains
have a spherical shape. In the present paper, we investigate
a more general case with the grains having elliptical shape.
By choosing different values of the ellipticity coefficient,
one can consider the oblate or prolate ellipsoidal inclusions,
which provides a wide class of models to be used in the
analysis of the complex conductivity of the mineral rocks.
An important goal of this paper is an application of the
developed GEMTIP models to studying the complex
resistivity of the typical mineral rocks. We have collected
several dozens of representative rock samples from the Cu-
Au deposit in Mongolia. These rock samples were subjected
to the mineralogical analysis using Quantitative Evaluation
of Minerals by Scanning Electron Microscopy (QEMSCan)
technology. We also conducted an analysis of the electrical
properties of the same samples using laboratory complex
resistivity (CR) measurement system.
As the result of this study, we have established the
relationships between the mineral composition of the rocks,
determined using QEMScan analysis, and the parameters of
the GEMTIP model defined from the lab measurements of
the electrical properties of the rocks. These relationships
open a possibility for remote estimation of the type of
mineralization using the spectral IP data.
Multiphase heterogeneous medium filled with ellipsoidal
inclusions
The GEMTIP model provides a general solution of the
effective conductivity problem for an arbitrary multiphase
composite polarized medium (Zhdanov, 2008, 2009, 2010).
The GEMTIP theory opens a possibility of determining the
effective conductivity for grains with arbitrary shape;
however, the calculation of the parameters of the GEMTIP
model may become very complicated. In a special case of
inclusions with spherical shape, the GEMTIP model can be
reduced to the classical Cole-Cole model of complex
resistivity. There exists another special case of inclusions
with ellipsoidal shape, where the solution of the GEMTIP
formulas can be obtained in close form, similar to a model
with spherical inclusions. The advantage of the model with
ellipsoidal inclusions is that in this case one can use different
shapes of ellipsoids, from oblate to prolate, to model
different types of heterogeneous rock formations and
different types of inclusions (see Figure 1). The three-
phased GEMTIP model, developed by Zhdanov (2008), in a
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