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首页> 外文期刊>Izvestiya. Physics of the solid earth >Mathematical modeling of membrane polarization occurring in rocks due to applied electrical field
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Mathematical modeling of membrane polarization occurring in rocks due to applied electrical field

机译:电场作用下岩石中膜极化的数学模型

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摘要

Membrane polarization occurs in sediments with different surface area of capillaries (pores) and is regarded as a slow type of polarization. This phenomenon is the foundation of the well known methods of induced polarization (IP): time domain and frequency domain induced polarization. The characteristic parameters of induced polarization which are required for studying physical properties of rocks are measured in the laboratory. Data measured in the laboratory confirmed the distinctions of IP processes at time-on and time-off. Additionally linear dependence of voltage and applied current is not always observed. This paper presents the first step of studying: theoretical consideration for time-on and mathematical modeling of membrane polarization, ion concentrations of electrolyte in the pores of different models of pores space, and arising voltage. The problem of concentration of ions along the pores can be solved using the diffusion equation with specified initial and boundary conditions. Reduced boundary conditions for time-on show that transient concentrations at the boundaries are linear with time. It allows obtaining the analytical solution for this equation. Mathematical modeling has been performed for different combinations of pores. It is shown that if electrical current flows from the pores with greater transfer numbers to the pores with smaller transfer numbers, an excess of ions will be observed at this boundary. If the difference of transfer numbers is negative, there is a decrease in the concentration of ions at the vicinity of the boundary. This decrease will continue until the concentration at this boundary reaches zero. In this case the galvanic chain will be interrupted and electrical current flowing through the sample does not penetrate to this cell. The duration of the process of ions distribution in the pore and time of blockage t (0) is proportional to the radii of contacted pores and inversely proportional to the transfer number difference and square of the current flowing through this cell. It was shown by both laboratory measurement and field processes that induced polarization relates to low porous rocks with small transfer number differences.
机译:膜极化发生在具有不同毛细管(孔隙)表面积的沉积物中,被认为是缓慢的极化类型。这种现象是众所周知的感应极化(IP)方法的基础:时域和频域感应极化。在实验室中测量了研究岩石物理特性所需的感应极化特征参数。实验室中测得的数据证实了在开机和关机时知识产权流程的区别。另外,并不总是观察到电压和施加电流的线性相关性。本文提出了研究的第一步:膜极化的时间和数学建模的理论考虑,不同孔隙空间模型中孔隙中电解质的离子浓度以及产生的电压。可以使用具有指定初始条件和边界条件的扩散方程来解决离子沿孔的浓度问题。导通时间减少的边界条件表明,边界处的瞬态浓度与时间呈线性关系。它允许获得该方程式的解析解。已经对孔的不同组合进行了数学建模。结果表明,如果电流从迁移数较大的孔流向迁移数较小的孔,则在该边界处将观察到过量的离子。如果转移数的差为负,则边界附近的离子浓度降低。这种下降将持续到该边界处的浓度达到零为止。在这种情况下,电流链将中断,流经样品的电流不会渗透到该电池中。离子在孔中的分布过程的持续时间和堵塞的时间t(0)与接触孔的半径成正比,与流过该单元的电流的传递数差和平方成反比。实验室测量和现场过程均表明,感应极化与低传输数差的低孔隙度岩石有关。

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