Frangenberg Matthias, Schmidt Annette M, Wilkens Jan
Faculty of Applied Natural Sciences, TH Köln - University of Applied Sciences, Leverkusen D-51379, Germany.
Department of Chemistry, Institute of Physical Chemistry, University of Cologne, Cologne D-50939, Germany.
Langmuir. 2025 Mar 4;41(8):5188-5201. doi: 10.1021/acs.langmuir.4c04456. Epub 2025 Feb 19.
Accurate determination of the zeta potential in colloidal dispersions often requires consideration of the relaxation effect, which is associated with the polarization of the electrical double layer and the surface conductivity. In this study, we pursue a new approach that combines conductivity measurements of the dispersion and dispersion medium with the electroacoustic and electrophoretic zeta potential determination. The conductivity data are analyzed with the Maxwell-Wagner-O'Konski theory, providing the Dukhin number. Zeta potentials of highly concentrated polymer dispersions were determined using the colloid vibration current (CVI) method and compared with those obtained by electrophoretic light scattering (ELS) in diluted dispersions. In both cases, the relaxation effect was now taken into account on the basis of the experimentally determined Dukhin number. The evaluation of the Dukhin numbers revealed significant surface conductivity for all investigated polymer dispersions. In addition, it was often found that not only the diffuse layer but also the stagnant layer contributes considerably to the surface conductivity. Proper consideration of both effects is essential for the reliable determination of the zeta potential, as otherwise inconsistencies can be observed in the evaluated data. Moreover, we have validated for the first time that the advanced CVI theory takes the effect of surface conductivity properly into account for a wide range of particle volume fractions. These values agree well with those obtained by the ELS method using the Dukhin-Semenikhin theory or a modified theory of Ohshima, Healy, and White. This study thus shows that the Dukhin number can serve as a key parameter to reliably connect conductivity and electrophoretic and electroacoustic experiments.
准确测定胶体分散体系中的zeta电位通常需要考虑弛豫效应,该效应与双电层极化和表面电导率有关。在本研究中,我们采用了一种新方法,将分散体系和分散介质的电导率测量与电声和电泳zeta电位测定相结合。利用麦克斯韦-瓦格纳-奥康斯基理论分析电导率数据,得出杜金数。使用胶体振动电流(CVI)方法测定了高浓度聚合物分散体系的zeta电位,并与稀释分散体系中通过电泳光散射(ELS)获得的结果进行了比较。在这两种情况下,都根据实验测定的杜金数考虑了弛豫效应。对杜金数的评估表明,所有研究的聚合物分散体系都具有显著的表面电导率。此外,经常发现不仅扩散层而且停滞层对表面电导率也有很大贡献。正确考虑这两种效应对于可靠测定zeta电位至关重要,否则在评估数据中会观察到不一致性。此外,我们首次验证了先进的CVI理论在很宽的颗粒体积分数范围内都能正确考虑表面电导率的影响。这些值与使用杜金-谢梅尼欣理论或大岛、希利和怀特修正理论的ELS方法获得的值非常吻合。因此,本研究表明杜金数可以作为一个关键参数,可靠地关联电导率以及电泳和电声实验。