Munaò Gianmarco, Costa Dino, Malescio Gianpietro, Bomont Jean-Marc, Prestipino Santi
Dipartimento di Scienze Matematiche e Informatiche, Scienze Fisiche e Scienze della Terra, Università degli Studi di Messina, Viale F. Stagno d'Alcontres 31, 98166 Messina, Italy.
Université de Lorraine, LCP-A2MC, UR 3469, Metz F-57078, France.
Soft Matter. 2022 Aug 31;18(34):6453-6464. doi: 10.1039/d2sm00944g.
We investigate by Monte Carlo simulations a mixture of particles with competing interactions (hard-sphere two-Yukawa, HSTY) and hard spheres (HS), with same diameters and a square-well (SW) cross attraction. In a recent study [G. Munaò , , 2022, , 2027-2039], we have analysed situations-in terms of relative concentration and attraction strength-where HS promote the formation of clusters involving particles of both species under thermodynamic conditions that would not allow for clustering of the pure HSTY fluid. Here, we focus on the role played by the range of cross attraction in determining the equilibrium structure of the mixture, starting from a homogeneous low-density state. When the width of the well exceeds approximately , clustering takes place in the system, with aggregates characterised by various sizes and shapes. Only for low HSTY concentrations (less than 10%) a single big cluster appears, anticipating the behaviour observed for a wider well, around 1.2. In the latter case, a spherical cluster encompassing almost all particles is the stable structure at equilibrium. We interpret this outcome as a macrophase, liquid-vapour separation where the spherical cluster is just the form taken at low density by the liquid phase inside the vapour phase: indeed, when the density takes larger values, periodic boundary conditions select liquid-vapour interfaces with other non-spherical shapes, similarly as found for a finite sample of simple fluid going through the liquid-vapour coexistence region. For still higher densities we document the existence of a solid phase characterized by the alternation of bilayers filled with particles of one species and bilayers of the other species, giving the solid a peculiar wafer structure.
我们通过蒙特卡罗模拟研究了具有竞争相互作用的粒子混合物(硬球双 Yukawa 势,HSTY)和硬球(HS),它们具有相同的直径以及方阱(SW)交叉吸引力。在最近的一项研究[G. Munaò, 2022, 2027 - 2039]中,我们分析了在相对浓度和吸引力强度方面的情况,即在热力学条件下,HS 促进了两种物种粒子团簇的形成,而这些条件不允许纯 HSTY 流体发生团簇。在这里,我们从均匀的低密度状态开始,关注交叉吸引力范围在确定混合物平衡结构中所起的作用。当阱的宽度超过约 时,系统中会发生团簇现象,聚集体具有各种大小和形状。仅对于低 HSTY 浓度(小于 10%),会出现单个大团簇,这预示着在阱宽约为 1.2 时更宽阱情况下观察到的行为。在后一种情况下,包含几乎所有粒子的球形团簇是平衡时的稳定结构。我们将此结果解释为一种宏观相,即液 - 气分离,其中球形团簇只是气相中液相在低密度下所呈现的形式:实际上,当密度取更大值时,周期性边界条件会选择具有其他非球形形状的液 - 气界面,这与通过液 - 气共存区域的简单流体有限样本的情况类似。对于更高的密度,我们记录到存在一种固相,其特征是由一种物种粒子填充的双层与另一种物种的双层交替排列,赋予固体一种特殊的薄片结构。