固态离子电解质电极区域的电势分布

H. S. Bokun, D. di Caprio, M. Holovko
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摘要

固态电解质被认为是由穿过固体体积的阳离子和阴离子组成的系统,阴离子的迁移率可以忽略,因为它们的大小与阳离子的大小相比较大。因此,在均匀情况下,发生局部电荷补偿。在外加电场的作用下,阳离子在近电极区域产生移动电荷和电场的不均匀再分布。该模型用于高温离子导体和电流源的统计力学描述。为了得到移动充电子系统随其密度分布的自由能泛函,采用重正规化Mayer函数的簇展开格式。由在单粒子场中运动的电荷组成的系统的哈密顿量被用作基一。根据集体变量法的结果,将主系统的二元函数表示为筛选势和平均力势。考虑了系统的短期和长期效应,计算了系统的内能。利用Gibbs - Duhem关系计算了体系的自由能泛函。从自由能极值的条件出发,得到了近电极区域运动粒子数密度和电势的分布。平均力的势是通过在晶格近似中求解一组积分方程,并考虑到短期和长期效应而得到的。从相关函数到相关函数的转换使我们能够识别电势的相关和不相关部分。考虑了电荷浓度偏离均匀分布对化学势的线性贡献。计算考虑了前三个配位球中粒子之间的相关性的贡献,这种相关性导致了第一个配位球的吸引,第二个配位球和第三个配位球的排斥。用特征方程根复数的四阶线性微分方程进行描述。本文对解析解的结果进行了分析。
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Distribution of electropotential in the electrode area of a solid state ion electrolyte
A solid state electrolyte is considered as a system consisting of cations moving through the volume of a solid body and anions whose mobility can be neglected due to their large size compared to the size of the cations. Accordingly, in the homogeneous case local charge compensation takes place. Under the action of an external electric field, cations create in the near electrode area inhomogeneous redistribution of mobile charges and electric field. The model is used for the statistical­mechanical description of high­temperature ionic conductors and current sources. To obtain the free energy functional of the mobile charge subsystem depending on the distribution of their density, the cluster expansion scheme for the renormalized Mayer functions is used. The Hamiltonian of a system consisting of electric charges moving in the field of single­particle cell potentials of average forces is used as the basis one. The binary function of the host system is expressed in terms of the screened potentials and the potentials of the average forces based on the results of the method of collective variables. The internal energy of the system is calculated taking into account the short­ and long­range effects. The Gibbs – Duhem relation was used for calculating the free energy functional of the system. The distribution of the number density of moving particles and the electric potential in the near electrode region were found from the condition of extremality of the free energy. The potentials of average forces are obtained as a result of solving a system of integral equations in the lattice approximation, with accounting of the short­ and long­range effects. The transition from the correlative function to the correlation function allowed us to identify the correlated and uncorrelated parts of the electric potential. The linear contributions of the deviation of the charge concentrations from a uniform distribution to the chemical potential are considered. The calculations take into account the contribution of the correlation between the particles in the first three coordination spheres that leads to attraction of the first, repulsion of the second and third neighbors. The description is carried out using a linear differential equation of the fourth­order with complex values of the roots of the characteristic equation. The paper analyzes the results of the analytical solution.
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