Delgado A V, Ahualli S, Arroyo F J, Jiménez M L, Carrique F
Departamento de Física Aplicada, Facultad de Ciencias, and MNat Unit of Excellence, Universidad de Granada, 18071 Granada, Spain.
Departamento de Física Aplicada, Facultad de Ciencias, and MNat Unit of Excellence, Universidad de Granada, 18071 Granada, Spain.
Adv Colloid Interface Sci. 2022 Jan;299:102539. doi: 10.1016/j.cis.2021.102539. Epub 2021 Sep 30.
Because of their singular phenomenology, the so-called salt-free colloids constitute a special family of dispersed systems. Their main characteristic is that the dispersion medium ideally contains only the solvent and the ions compensating exactly the surface charge of the particles. These ions (often called released counterions) come into the solution when the surface groups responsible for the particles charge get ionized. An increasing effort is nowadays dedicated to rigorously compare theoretical model predictions for ideal salt-free suspensions, where only the released counterions are supposed to be present in solution, with appropriately devised experiments dealing with colloids as close as possible to the ideal salt-free ones. Of course, if the supporting solution is aqueous, the presence of atmospheric contamination and any other charged species different from the released counterions in the solution must be avoided. Because this is not an easy task, the presence of dissolved atmospheric CO and of H and OH from water dissociation cannot be fully discarded in aqueous salt-free solutions (often denominated realistic in such case). Ultimately, at some point, the role of the released counterions will be comparable or even larger in highly charged concentrated colloids than that of added salts. These topics are covered in the present contribution. The model results are compared with experimental data on the dynamic mobility and dielectric dispersion of polystyrene spheres of various charges and sizes. As a rule, it is found that the model correctly predicts the significance of alpha and Maxwell-Wagner-O'Konski relaxations. Positions and amplitudes of such relaxations are well predicted, although it is necessary to assume that the released counterions are potassium or sodium instead of protons, otherwise the frequency spectra of experimental mobility and permittivity differ very significantly from those theoretically calculated. The proposed electrokinetic evaluation is an ideal tool for detecting in situ the possible contamination (or incomplete ion exchange of the latexes). A satisfactory agreement is found when potassium counterions are assumed to be in solution, mostly if one considers that the comparison is carried out without using any adjustable parameters.
由于其独特的现象学,所谓的无盐胶体构成了一类特殊的分散体系。它们的主要特征是,理想情况下,分散介质仅包含溶剂以及恰好补偿颗粒表面电荷的离子。当负责颗粒电荷的表面基团发生电离时,这些离子(通常称为释放的抗衡离子)进入溶液。如今,人们越来越致力于将理想无盐悬浮液的理论模型预测(其中假设溶液中仅存在释放的抗衡离子)与精心设计的实验进行严格比较,这些实验所涉及的胶体尽可能接近理想无盐胶体。当然,如果支撑溶液是水性的,必须避免大气污染物以及溶液中不同于释放的抗衡离子的任何其他带电物种的存在。由于这并非易事,在无盐水溶液(在这种情况下通常称为实际溶液)中,不能完全排除溶解的大气二氧化碳以及水电离产生的氢离子和氢氧根离子的存在。最终,在某些情况下,在高电荷浓缩胶体中,释放的抗衡离子的作用将比添加的盐的作用更大或相当。本论文涵盖了这些主题。将模型结果与不同电荷和尺寸的聚苯乙烯球体的动态迁移率和介电色散的实验数据进行了比较。通常发现,该模型正确地预测了α弛豫和麦克斯韦 - 瓦格纳 - 奥康斯基弛豫的重要性。尽管有必要假设释放的抗衡离子是钾离子或钠离子而非质子,否则实验迁移率和介电常数的频谱与理论计算值有很大差异,但这些弛豫的位置和幅度得到了很好的预测。所提出的电动评估是原位检测可能的污染(或乳胶的不完全离子交换)的理想工具。当假设溶液中存在钾抗衡离子时,发现了令人满意的一致性,尤其是如果考虑到比较是在不使用任何可调参数的情况下进行的。