Li Zifeng, Van Dyk Antony K, Fitzwater Susan J, Fichthorn Kristen A, Milner Scott T
Department of Chemical Engineering, Pennsylvania State University , State College Pennsylvania 16802, United States.
Dow Coating Materials, The Dow Chemical Company , Collegeville, Pennsylvania 19426, United States.
Langmuir. 2016 Jan 19;32(2):428-41. doi: 10.1021/acs.langmuir.5b03942. Epub 2016 Jan 6.
Charged particles in aqueous suspension form an electrical double layer at their surfaces, which plays a key role in suspension properties. For example, binder particles in latex paint remain suspended in the can because of repulsive forces between overlapping double layers. Existing models of the double layer assume sharp interfaces bearing fixed uniform charge, and so cannot describe aqueous binder particle surfaces, which are soft and diffuse, and bear mobile charge from ionic surfactants as well as grafted multivalent oligomers. To treat this industrially important system, we use atomistic molecular dynamics simulations to investigate a structurally realistic model of commercial binder particle surfaces, informed by extensive characterization of particle synthesis and surface properties. We determine the interfacial profiles of polymer, water, bound and free ions, from which the charge density and electrostatic potential can be calculated. We extend the traditional definitions of the inner and outer Helmholtz planes to our diffuse interfaces. Beyond the Stern layer, the simulated electrostatic potential is well described by the Poisson-Boltzmann equation. The potential at the outer Helmholtz plane compares well to the experimental zeta potential. We compare particle surfaces bearing two types of charge groups, ionic surfactant and multivalent oligomers, with and without added salt. Although the bare charge density of a surface bearing multivalent oligomers is much higher than that of a surfactant-bearing surface at realistic coverage, greater counterion condensation leads to similar zeta potentials for the two systems.
水悬浮液中的带电粒子在其表面形成一个电双层,这在悬浮液性质中起着关键作用。例如,乳胶漆中的粘结剂颗粒由于重叠双层之间的排斥力而保持悬浮在罐中。现有的双层模型假设界面清晰,带有固定的均匀电荷,因此无法描述水性粘结剂颗粒表面,这种表面是柔软且弥散的,并且带有来自离子表面活性剂以及接枝的多价低聚物的可移动电荷。为了处理这个具有工业重要性的系统,我们使用原子分子动力学模拟来研究商业粘结剂颗粒表面的结构逼真模型,该模型是基于对颗粒合成和表面性质的广泛表征而建立的。我们确定了聚合物、水、结合离子和自由离子的界面轮廓,由此可以计算电荷密度和静电势。我们将内亥姆霍兹平面和外亥姆霍兹平面的传统定义扩展到我们的弥散界面。在斯特恩层之外,模拟的静电势可以用泊松 - 玻尔兹曼方程很好地描述。外亥姆霍兹平面处的电势与实验测得的zeta电势比较吻合。我们比较了带有两种电荷基团(离子表面活性剂和多价低聚物)的颗粒表面,有无添加盐的情况。尽管在实际覆盖率下,带有多价低聚物的表面的裸电荷密度远高于带有表面活性剂的表面,但更大的反离子凝聚导致两个系统的zeta电势相似。