Effects of thermal maturity and chemical composition of kerogen on its
dielectric constant
Archana Jagadisan
1
and Zoya Heidari
1
ABSTRACT
Reliable formation evaluation using borehole geophysical
measurements in organic-rich mudrocks requires knowledge
about the physical properties of kerogen. For instance, estimates
of water-filled pore volume are significantly affected by the as-
sumptions made for dielectric permittivity of kerogen, which
can be influenced by thermal maturity. However, the impact
of thermal maturity of pure kerogen on its dielectric properties
is not yet thoroughly understood. We quantify the dielectric con-
stant of kerogen samples extracted from three formations, with
different levels of natural thermal maturity, and we identify the
impact of thermal maturity on their dielectric properties. We first
isolate kerogen from mudrock samples using physical and
chemical treatments. We then synthetically mature the samples
in a controlled environment and measure their dielectric con-
stant (at 1 GHz) using a microwave resonator. X-ray photoelec-
tron spectroscopy (XPS) monitors the variation in chemical
composition of kerogen. The dielectric constant of the kerogen
samples varied significantly in the range of 1.89–3.2 upon being
heat treated from 25°C to 650°C. The variation in the dielectric
constant is explained by the alteration in the chemical compo-
sition and structure of kerogen as a result of thermal maturation.
XPS measurements also showed an increase in aromatic carbon
content in the kerogen samples as the thermal maturity in-
creased. The documented results enable the integration of the
kerogen geochemistry to the interpretation of dielectric mea-
surements, which contributes to improved interpretation of di-
electric logs in organic-rich mudrocks, and result in enhanced
formation evaluation of these reservoirs.
INTRODUCTION
Log-based formation evaluation of organic-rich mudrocks can be
challenging due to uncertainties associated with petrophysical proper-
ties of the rock components, such as kerogen, as well as the complex
rock physics of these reservoirs. For instance, one important challenge
faced in the formation evaluation of organic-rich mudrocks is to
reliably determine fluid saturations. Resistivity measurements have
typically been used for water saturation evaluation in conventional
formations. In unconventional organic-rich mudrocks, however, their
application in the quantification of water saturation becomes limited
due to significant uncertainties in the formation water salinity, as well
as complex pore structure and fluid distribution, which lead to failure
of conventional resistivity-porosity-saturation rock-physics models
such as Archie’s, dual-water, and Waxman-Smits models (Archie,
1942; Waxman and Smits, 1968; Clavier et al., 1984). Compared with
resistivity measurements, dielectric logs are less sensitive to water
salinity, especially at high frequencies (i.e., greater than 1 GHz) (Shao
et al., 2003; Seleznev et al., 2014). Thus, they have been considered to
be attractive options for water saturation assessment and as alterna-
tives to resistivity logs (Calvert and Wells, 1977) in the presence of
uncertainty in salt concentration and at low salinities.
Dielectric properties manifest as a complex permittivity. The real
component of the dielectric permittivity is usually expressed as rel-
ative permittivity, which is the dielectric property of a material rel-
ative to that of free space. The imaginary component contains a
frequency-dependent conductivity term. The complex permittivity
of porous media (von Hippel, 1954) can be expressed as
ε
Ã
ðfÞ¼ ε
r
ðfÞþ jε
i
ðfÞ¼ ε
r
ðfÞþ j
σðfÞ
2πε
0
f
; (1)
Manuscript received by the Editor 9 March 2018; revised manuscript received 12 July 2019; published ahead of production 22 October 2019; published online
30 December 2019.
1
The University of Texas at Austin, Hildebrand Department of Petroleum and Geosystems Engineering, Austin, Texas, USA. E-mail: archana.jagadisan@
utexas.edu; zoya@utexas.edu.
© 2020 Society of Exploration Geophysicists. All rights reserved.
D53
GEOPHYSICS, VOL. 85, NO. 1 (JANUARY-FEBRUARY 2020); P. D53–D64, 11 FIGS., 5 TABLES.
10.1190/GEO2018-0180.1
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