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Pore-Scale Analysis of the Waxman-Smits Shaly-Sand Conductivity Model

机译:Waxman-Smits泥质砂电导率模型的孔隙尺度分析

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Waxman-Smits and dual-water models of electrical conductivity of shaly sands account for the dual conductive pathways formed by pore brine and clay mineral exchange cations, while Archie's equations describe the electrical conductivity behavior of clay-free rocks. These empirical models are widely used in the interpretation of resistivity logs acquired in homogeneous reservoir rocks. However, the models are not explicit in their predictions of electrical conductivity with respect to rock structure, spatial fluid distribution in the pore space, wettability, or clay mineral distribution. The objective of this paper is to quantify the influence of exchange cations associated with hydrated clay minerals, salinity of pore bulk water, and water saturation on the electrical conductivity of shaly siliciclastic rocks. We accomplish this objective by calculating excess conductivities associated with hydrated clay minerals for explicit pore geometries of brine- and hydrocarbon-saturated shaly granular rocks. In so doing we introduce synthetic pore-scale representations intended to reproduce experimental observations of electrical conductivity of shaly sands.The synthetic pore-scale models are constructed to represent homogeneous shaly sands that include the structural effects of compaction, cementation, and distribution of grain-coating clay minerals. Our pore-scale model is implemented on the digitized representative of rock samples, which allows us to consider arbitrary media boundaries. Two-phase immiscible fluids are geometrically distributed in the pore space using the ordinary percolation algorithm. We introduce grain-coating hydrated clay minerals and their corresponding electric double layer in the synthetic rock models with a grain "shell" of variable dimensions and diffusivity with respect to those of pore-filling brine. Waxman-Smits formation factors and resistivity indices are calculated directly with random walk simulations of late-time diffusion within the conductive space formed by the pore water and clay mineral exchange cations in the digitized shaly-sand samples. Simulations with this simple model correctly reproduce the nonlinear behavior of rock conductivity at low and high salinity, and are consistent with reported laboratory measurements.
机译:泥质砂岩电导率的Waxman-Smits和双水模型解释了孔隙盐水和粘土矿物交换阳离子形成的双电导途径,而Archie方程描述了无黏土岩石的电导行为。这些经验模型被广泛用于解释均质储层岩石中的电阻率测井。但是,这些模型在关于岩石结构,孔隙空间流体分布,润湿性或粘土矿物分布方面的电导率预测中并不明确。本文的目的是量化与水合粘土矿物,孔隙水的盐度和含水饱和度相关的交换阳离子对泥质硅质碎屑岩电导率的影响。我们通过计算与水合粘土矿物相关的过量电导率来实现此目标,这些电导率适用于盐水和烃类饱和泥质颗粒岩的明确孔隙几何形状。在此过程中,我们引入了合成的孔隙尺度表示法,旨在再现泥质砂岩电导率的实验观察结果。合成的孔隙尺度模型被构建为代表均质的泥质砂岩,包括压实,胶结和颗粒分布的结构效应。涂料粘土矿物。我们的孔隙尺度模型是在岩石样品的数字化代表上实现的,这使我们可以考虑任意介质边界。使用普通的渗流算法,两相不混溶流体在孔隙空间中几何分布。我们在人造岩石模型中引入了覆有涂层的水合粘土矿物及其相应的双电层,这些岩石具有相对于孔隙填充盐水而言具有可变尺寸和扩散性的晶粒“壳”。 Waxman-Smits的形成因子和电阻率指数是通过随机游走模拟直接计算出来的,该模拟是在数字化泥质砂岩样品中由孔隙水和粘土矿物交换阳离子形成的导电空间内的后期扩散。使用此简单模型进行的模拟正确地再现了低盐度和高盐度下岩石电导率的非线性行为,并且与报告的实验室测量结果一致。

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