Lirio Piñar J A, Calvo J, Ahualli S
Departamento de Física Aplicada, Facultad de Ciencias, <a href="https://ror.org/04njjy449">Universidad de Granada</a>, 18071 Granada, Spain.
Departamento de Matemática Aplicada, Facultad de Ciencias, <a href="https://ror.org/04njjy449">Universidad de Granada</a>, 18071 Granada, Spain and Modeling Nature (MNat) Research Unit, University of Granada, Spain.
Phys Rev E. 2024 Sep;110(3-1):034610. doi: 10.1103/PhysRevE.110.034610.
The problem of ion transport in porous media is fundamental to many practical applications such as capacitive deionization, where ions are electrostatically attracted to a porous electrode and stored in the electric double layer, leaving a partially desalinated solution. These electrodes are functionalized to achieve maximum efficiency: it is intended that for each depleted electron one ion is removed. For this purpose, the surface is coated with a polyelectrolyte layer of the same sign as the electronic charge. In this work, the movement of ions from the solution to the soft or polyelectrolyte-coated electrodes is studied. For this purpose, a one-dimensional model is used to study the electric and diffusive fluxes produced by the application of an electric field and the storage of these ions in the micropores. The partial differential equations governing the process are numerically solved using the explicit Euler method. The results of the model indicate that the number of ions removed using soft electrodes is approximately 15% greater than that achieved with bare electrodes. Ion adsorption kinetics show that coated electrodes provide slightly slower adsorption compared to bare electrodes. Regarding the charging time of the micropores, it can be seen that it is a faster process (characteristic time of 100 s) compared to the time in which the ion concentration reaches equilibrium: electromigration is faster than diffusion. Comparing the situations with and without polyelectrolyte coating, it is observed that saturation in the micropores is reached earlier when the electrodes are coated. Concerning the cell geometry, it has been found that the characteristic time is proportional to the length of the spacer and inversely proportional to the length of the electrodes. With regard to microporosity, the rate of the process is approximately constant, irrespective of the number of micropores. Moreover, the number of adsorbed ions strongly depends on their initial concentration. Finally, the analysis of the ionic diffusion coefficient is determinant in the kinetics of the process: Taking into account the tortuosity of the porous electrode, which directly affects the diffusion in the channel, is fundamental to obtain model predictions close to reality.
多孔介质中的离子传输问题对于许多实际应用来说至关重要,比如电容去离子化,在该过程中离子被静电吸引至多孔电极并存储在双电层中,从而留下部分脱盐溶液。这些电极经过功能化处理以实现最大效率:理想情况下,每消耗一个电子就去除一个离子。为此,电极表面涂覆有与电子电荷符号相同的聚电解质层。在这项工作中,研究了离子从溶液向软质或聚电解质涂覆电极的移动。为此,使用一维模型来研究施加电场产生的电通量和扩散通量,以及这些离子在微孔中的存储情况。使用显式欧拉方法对描述该过程的偏微分方程进行数值求解。模型结果表明,使用软质电极去除的离子数量比裸电极大约多15%。离子吸附动力学表明,与裸电极相比,涂覆电极的吸附速度略慢。关于微孔的充电时间,可以看出与离子浓度达到平衡的时间相比,这是一个更快的过程(特征时间为100秒):电迁移比扩散更快。比较有无聚电解质涂层的情况,可以观察到涂覆电极时微孔更早达到饱和。关于电池几何结构,已发现特征时间与间隔物的长度成正比,与电极的长度成反比。关于微孔率,该过程的速率大致恒定,与微孔数量无关。此外,吸附离子的数量强烈依赖于它们的初始浓度。最后,离子扩散系数的分析对于该过程的动力学起决定性作用:考虑到多孔电极的曲折度,其直接影响通道中的扩散,对于获得接近实际的模型预测至关重要。