Complex conductivity of water-saturated packs of glass beads

被引:326
作者
Leroy, P. [4 ]
Revil, A. [1 ,2 ]
Kemna, A.
Cosenza, P. [3 ]
Ghorbani, A. [3 ]
机构
[1] Colorado Sch Mines, Dept Geophys, Golden, CO 80401 USA
[2] Univ Savoie, CNRS, LGIT UMR 5559, Le Bourget Du Lac, France
[3] Univ Paris 06, UMR 7619 Sisyphe, Paris, France
[4] Univ Aix Marseille 3, CNRS, F-13628 Aix En Provence, France
关键词
spectral impedance; porous media; induced polarization; complex conductivity; double layer; particle size distribution;
D O I
10.1016/j.jcis.2007.12.031
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The low-frequency conductivity response of water-saturated packs of glass beads reflects a combination of two processes. One process corresponds to the polarization of the mineral/water interface coating the surface of the grains. The other process corresponds to the Maxwell-Wagner polarization associated with accumulation of the electrical charges in the pore space of the composite medium. A model of low-frequency conductivity dispersion is proposed. This model is connected to a triple-layer model of electrochemical processes occurring at the surface of silica. This model accounts for the partition of the counterions between the Stern and the diffuse layers. The polarization of the mineral/water interface is modeled by the electrochemical polarization model of Schurr for a spherical grain. We take into account also the DC surface conductivity contribution of protons of the sorbed water and the contribution of the diffuse layer. At the scale of a macroscopic representative elementary volume of the porous material, the electrochemical polarization of a single grain is convoluted with the grain size distribution of the porous material. Finally, the Maxwell-Wagner polarization is modeled using the complex conductivity of a granular porous medium obtained from the differential effective medium theory. The predictions of this model agree well with experimental data of spectral induced polarization. Two peaks are observed at low frequencies in the spectrum of the phase. The first peak corresponds to the distribution of the size of the beads and the second peak is due to the roughness of the grains. (C) 2007 Elsevier Inc. All rights reserved.
引用
收藏
页码:103 / 117
页数:15
相关论文
共 68 条
[21]   LINEAR SYSTEM DESCRIPTION OF ELECTRICAL PARAMETERS OF ROCKS [J].
FULLER, BD ;
WARD, SH .
IEEE TRANSACTIONS ON GEOSCIENCE ELECTRONICS, 1970, GE 8 (01) :7-&
[22]  
GAUDIN AM, 1955, T AM I MIN MET ENG, V202, P66
[23]   Theory of the low-frequency electrorotation of polystyrene particles in electrolyte solution [J].
Grosse, C ;
Shilov, VN .
JOURNAL OF PHYSICAL CHEMISTRY, 1996, 100 (05) :1771-1778
[24]  
Hanai T., 1968, EMULSION SCI
[25]   MULTIPLE ACTIVATED COMPLEX DISSOLUTION OF METAL (HYDR)OXIDES - A THERMODYNAMIC APPROACH APPLIED TO QUARTZ [J].
HIEMSTRA, T ;
VANRIEMSDIJK, WH .
JOURNAL OF COLLOID AND INTERFACE SCIENCE, 1990, 136 (01) :132-150
[26]   DIELECTRIC RESPONSE OF A DILUTE SUSPENSION OF SPHERES WITH THIN DOUBLE-LAYERS IN AN ASYMMETRIC ELECTROLYTE [J].
HINCH, EJ ;
SHERWOOD, JD ;
CHEW, WC ;
SEN, PN .
JOURNAL OF THE CHEMICAL SOCIETY-FARADAY TRANSACTIONS II, 1984, 80 :535-551
[27]  
Hunter R. J., 1988, Zeta Potential in Colloid Science, Principles and Applications, VThird
[28]  
Jonscher A., 1983, DIELECTRIC RELAXATIO
[29]  
Keller G.V., 1988, Electromagnetic methods in applied geophysics, P13, DOI [10.1190/1.9781560802631.ch2, DOI 10.1190/1.9781560802631.CH2]
[30]   Crosshole IP imaging for engineering and environmental applications [J].
Kemna, A ;
Binley, A ;
Slater, L .
GEOPHYSICS, 2004, 69 (01) :97-107