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全氟磺酸离子聚合物分散体的胶体稳定性。第一部分。单离子静电相互作用势能

Colloidal Stability of PFSA-Ionomer Dispersions. Part I. Single-Ion Electrostatic Interaction Potential Energies.

作者信息

Srivastav Harsh, Weber Adam Z, Radke Clayton J

机构信息

Department of Chemical and Biomolecular Engineering, University of California, Berkeley, 201 Gilman, South Drive, Berkeley, California 94720, United States.

Energy Technologies Area, Lawrence Berkeley National Laboratory, Building 30, Cyclotron Road, Berkeley, California 94720, United States.

出版信息

Langmuir. 2024 Apr 2;40(13):6654-6665. doi: 10.1021/acs.langmuir.3c03903. Epub 2024 Mar 8.

Abstract

Charged colloidal particles neutralized by a single counterion are increasingly important for many emerging technologies. Attention here is paid specifically to hydrogen fuel cells and water electrolyzers whose catalyst layers are manufactured from a perfluorinated sulfonic acid polymer (PFSA) suspended in aqueous/alcohol solutions. Partially dissolved PFSA aggregates, known collectively as ionomers, are stabilized by the electrostatic repulsion of overlapping diffuse double layers consisting of only protons dissociated from the suspended polymer. We denote such double layers containing no added electrolyte as "single ion". Size-distribution predictions build upon interparticle interaction potential energies from the Derjaguin-Landau-Verwey-Overbeek (DLVO) formalism. However, when only a single counterion is present in solution, classical DLVO electrostatic potential energies no longer apply. Accordingly, here a new formulation is proposed to describe how single-counterion diffuse double layers interact in colloidal suspensions. Part II (Srivastav, H.; Weber, A. Z.; Radke, C. J. DOI: 10.1021/acs.langmuir.3c03904) of this contribution uses the new single-ion interaction energies to predict aggregated size distributions and the resulting solution pH of PFSA in mixtures of -propanol and water. A single-counterion diffuse layer cannot reach an electrically neutral concentration far from a charged particle. Consequently, nowhere in the dispersion is the solvent neutral, and the diffuse layer emanating from one particle always experiences the presence of other particles (or walls). Thus, in addition to an intervening interparticle repulsive force, a backside osmotic force is always present. With this new construction, we establish that single-ion repulsive pair interaction energies are much larger than those of classical DLVO electrostatic potentials. The proposed single-ion electrostatic pair potential governs dramatic new dispersion behavior, including dispersions that are stable at a low volume fraction but unstable at a high volume fraction and finite volume-fraction dispersions that are unstable with fine particles but stable with coarse particles. The proposed single-counterion electrostatic pair potential provides a general expression for predicting colloidal behavior for any charged particle dispersion in ionizing solvents with no added electrolyte.

摘要

由单个抗衡离子中和的带电胶体颗粒对于许多新兴技术变得越来越重要。这里特别关注氢燃料电池和水电解槽,其催化剂层由悬浮在水/醇溶液中的全氟磺酸聚合物(PFSA)制成。部分溶解的PFSA聚集体统称为离聚物,通过仅由悬浮聚合物解离的质子组成的重叠扩散双层的静电排斥而稳定。我们将这种不添加电解质的双层称为“单离子”。尺寸分布预测基于Derjaguin-Landau-Verwey-Overbeek(DLVO)形式的颗粒间相互作用势能。然而,当溶液中仅存在单个抗衡离子时,经典的DLVO静电势能不再适用。因此,这里提出了一种新的公式来描述单抗衡离子扩散双层在胶体悬浮液中的相互作用。本论文的第二部分(Srivastav, H.; Weber, A. Z.; Radke, C. J. DOI: 10.1021/acs.langmuir.3c03904)使用新的单离子相互作用能来预测丙醇和水混合物中PFSA的聚集尺寸分布以及由此产生的溶液pH值。单抗衡离子扩散层在远离带电粒子的地方无法达到电中性浓度。因此,在分散体中任何地方溶剂都不是中性的,并且从一个粒子发出的扩散层总是会感受到其他粒子(或壁)的存在。因此,除了中间的粒子间排斥力外,总是存在背面渗透力。通过这种新结构,我们确定单离子排斥对相互作用能比经典DLVO静电势的相互作用能大得多。所提出的单离子静电对势控制着显著的新分散行为,包括在低体积分数下稳定但在高体积分数下不稳定的分散体,以及对于细颗粒不稳定但对于粗颗粒稳定的有限体积分数分散体。所提出的单抗衡离子静电对势为预测在不添加电解质的电离溶剂中任何带电粒子分散体的胶体行为提供了一个通用表达式。

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