Surface conductivity of clays

Viacheslav Emelianov, Zeyu Zhang, A. Weller, Matthias Halisch, K. Titov
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Abstract

Clay minerals are extensively used in a wide range of applications. In particular, clay-bearing formations are considered as suitable radioactive waste repository. Electrical resistivity tomography is an appropriate tool to monitor the properties of clay-bearing locations. However, an inherent drawback of a conventional resistivity survey is its ambiguity in distinguishing between the effects of groundwater salinity, clay content, and porosity. A discrimination can be achieved on the basis of the induced polarization method that provides a complex conductivity. The main purpose of this study is the investigation of the complex conductivity of clay samples with a special focus on the contribution of surface conductivity produced by an excess of ions in the electrical double layer coating the solid particles. Six clay mixtures were selected that include an almost pure kaolinite sample, a sample consisting of a mixture of kaolinite, illite, and smectite, a crushed saponite breccia, a Ca-bentonite sample, and two illite clay samples. Besides the enriched kaolinite, the other samples are natural geomaterials that contain more than 40 weight per cent clay minerals. The mineralogical compositions of the samples were determined by quantitative X-ray diffraction analysis. The clay powder was mixed with a varying volume of sodium chloride solution to get plastic state clay samples with varying water content. The samples were investigated by the spectral induced polarization method in a frequency range between 1 mHz and 1 kHz. The resulting complex conductivity spectra indicate a decrease of the real part of the electrical conductivity with rising water content for the illite, bentonite and saponite breccia samples. The overall conductivity of these clay samples is dominated by their surface conductivity. In contrast, the electrical conductivity of kaolinite and kaolinite-illite mixture does not show any significant changes with the water content. For all samples, the imaginary part of electrical conductivity increases at low water content. The real part of the surface conductivity indicates a linear dependence on the volumetric clay content. The slope of this linear relationship can be used to distinguish the types of clay. The ratio between imaginary conductivity and surface conductivity, which decreases with increasing clay content, proves to be a suitable parameter that characterizes the connectivity of clay aggregates in the sample. The surface conductivity of the pure kaolinite sample has been determined in an additional multi-salinity experiment. The resulting surface conductivity is in good agreement with the experiment of varying water content. The multi-salinity experiment has shown that the resulting petrophysical parameters depend on the procedure of sample packing, which may lead to anisotropy. The effect of anisotropy is attributed to the alignment of the plate-like kaolinite particles in the course of the packing and consolidation procedure.
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粘土的表面传导性
粘土矿物被广泛应用于各种领域。特别是,含粘土地层被认为是合适的放射性废物储存库。电阻率层析成像技术是监测含粘土地层特性的合适工具。然而,传统电阻率勘测的一个固有缺点是难以区分地下水盐度、粘土含量和孔隙度的影响。通过提供复合电导率的诱导极化法可以实现区分。本研究的主要目的是调查粘土样本的复合电导率,特别关注由包裹固体颗粒的电双层中过量离子产生的表面电导率的贡献。研究选取了六种粘土混合物,包括一种几乎纯净的高岭石样品,一种由高岭石、伊利石和直闪石混合而成的样品,一种破碎的皂石角砾岩,一种钙膨润土样品,以及两种伊利石粘土样品。除富集高岭石外,其他样品均为天然地质材料,其中粘土矿物含量超过 40%。样品的矿物成分是通过定量 X 射线衍射分析确定的。将粘土粉末与不同体积的氯化钠溶液混合,得到不同含水量的可塑状态粘土样品。在 1 mHz 至 1 kHz 的频率范围内,采用光谱诱导极化法对样品进行了研究。得出的复电导率光谱表明,伊利石、膨润土和皂角砾岩样品的电导率实部随着含水量的增加而降低。这些粘土样品的整体电导率主要由其表面电导率决定。相比之下,高岭石和高岭石-伊利石混合物的电导率并没有随着含水量的增加而发生明显变化。对于所有样品,低含水量时电导率的虚部都会增加。表面电导率的实部与粘土的体积含量呈线性关系。这种线性关系的斜率可用于区分粘土类型。假想电导率和表面电导率之间的比率随着粘土含量的增加而减小,这被证明是表征样品中粘土聚集体连通性的合适参数。纯高岭石样品的表面电导率是在额外的多盐度实验中测定的。得出的表面电导率与不同含水量的实验结果十分吻合。多盐度实验表明,得出的岩石物理参数取决于样品堆积的程序,这可能导致各向异性。各向异性的影响归因于板状高岭石颗粒在堆积和固结过程中的排列。
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