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Molecular association of heteronuclear vibrating square-well dumbbells in liquid-vapor phase equilibrium

机译:液相汽相平衡中异核振动方阱哑铃的分子缔合

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Molecular aggregates are formed by heteronuclear vibrating square-well dumbbells. In a recent article [G. A. Chapela and J. Alejandre, J. Chem. Phys., 132(10), 104704 (2010)], it is shown that heteronuclear vibrating square-well dumbbells with a diameter ratio between particles of 1/2 and interacting potential ratio of 4 form micelles of different sizes and shapes which manifest themselves in both the liquid and vapor phases, up to and above the critical point. This means that micellization and phase separation are present simultaneously in this simple model. These systems present a maximum in the critical temperature when plotted against the potential well depth of the second particle ε2. In the same publication, it was speculated that the formation of micelles was responsible for the appearance of the maximum. A thorough study on this phenomena is presented here and it is found that there is a threshold on the size of the second particle and its corresponding depth of interaction potential, where the micelles are formed. If the diameter and well depth of the second particle are small enough for the first and deep enough for the second, micelles are formed. For σ2/σ1 between 0.25 and 0.65 and ε2/ε1 larger than 5.7, micelles are formed up to and above the critical temperature. Outside these ranges micelles appear only at temperatures lower than the critical point. There is a strong temperature dependence on the formation and persistence of the aggregates. For the deepest wells and large enough second particles, a gel interconnected aggregate is obtained. In this work, the micelles are formed at temperatures as low as the triple point and as high as the critical point and, in some cases, persist well above it. The presence of these maxima in critical temperatures Tc when plotted against ε2 as follows. At lower values of ε2, an increase of Tc is obtained as is expected by the increase of the attractive volume as indicated by the principle of corresponding states. As ε2 increases further, the formation of molecular aggregates produce a saturation effect of the deepening of the potential well by encapsulating the particles of the second kind inside the micelles, so the resulting Tc represents a new poly disperse system of molecular aggregates and not the original heteronuclear vibrating square-well dumbbells. The surface tension is also analyzed for these systems, and it is shown that decreases with increasing attraction due to the formation of molecular aggregates. © 2011 American Institute of Physics Article Outline INTRODUCTION TECHNICAL DETAILS Vibrating square-well dumbbells and interaction potential Discontinuous molecular dynamics CALCULATED PROPERTIES Surface tension and vapor pressure Density profile and orthobaric densities Critical temperature and density Radial distribution function, cluster size, and radius of gyration RESULTS Maxima in Tc* vs ε2* for σ2* constant Maxima in Tc* vs σ2* for ε2* = 1 Triple-point crystal and the existence of gel-like structures Finite-size effects CONCLUDING REMARKS
机译:分子聚集体由异核振动方阱哑铃形成。在最近的一篇文章中[G. A.Chapela和J.Alejandre,J.Chem。 Phys。,132(10),104704(2010)]显示,直径为1/2的粒子和相互作用势比为4的异核振动方阱哑铃会形成不同大小和形状的胶束在液相和气相中都达到和超过临界点。这意味着在这个简单的模型中胶束化和相分离同时存在。当针对第二粒子ε2的势阱深度作图时,这些系统呈现出临界温度的最大值。在同一出版物中,推测胶束的形成与最大胶束的出现有关。这里对这种现象进行了彻底的研究,发现在形成胶束的第二粒子的大小及其对应的相互作用电位深度上有一个阈值。如果第二颗粒的​​直径和阱深度对于第一颗粒足够小而对于第二颗粒足够深,则形成胶束。当σ2 /σ1在0.25和0.65之间,而ε2 /ε1大于5.7时,在临界温度以上及以上形成胶束。在这些范围之外,胶束仅在低于临界点的温度下出现。温度强烈依赖于骨料的形成和持久性。对于最深的孔和足够大的第二颗粒,可以得到凝胶互连的聚集体。在这项工作中,胶束是在低至三点和高至临界点的温度下形成的,在某些情况下,其温度远高于其临界点。当针对ε2绘制时,在临界温度Tc 中存在这些最大值。在较低的ε2值下,如相应状态原理所指示的,由于吸引量的增加,可以预期得到Tc 的增加。随着ε2的进一步增加,分子团聚体的形成通过将第二种粒子包裹在胶束内部而产生了势阱加深的饱和效应,因此所得的Tc 代表了一种新的多分散体分子聚集体系统,而不是原始的异核振动方孔哑铃。还针对这些系统分析了表面张力,结果表明,由于分子聚集体的形成,表面张力会随着吸引力的增加而降低。 ©2011美国物理研究所文章大纲简介技术细节振动方阱哑铃和相互作用势不连续的分子动力学计算的特性表面张力和蒸气压密度分布和正压密度临界温度和密度径向分布函数,簇的大小和回转半径结果对于σ2*常数,Tc *与ε2*的极大值对于ε2* = 1三点晶体与Tc *与σ2*的极大值凝胶状结构的存在有限尺寸效应结论

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