Gibson H M, Wilding N B
Department of Physics, University of Bath, Bath BA2 7AY, United Kingdom.
Phys Rev E Stat Nonlin Soft Matter Phys. 2006 Jun;73(6 Pt 1):061507. doi: 10.1103/PhysRevE.73.061507. Epub 2006 Jun 21.
Linearly sloped or "ramp" potentials belong to a class of core-softened models which possess a liquid-liquid critical point (LLCP) in addition to the usual liquid-gas critical point. Furthermore, they exhibit thermodynamic anomalies in their density and compressibility, the nature of which may be akin to those occurring in water. Previous simulation studies of ramp potentials have focused on just one functional form, for which the LLCP is thermodynamically stable. In this work we construct a series of ramp potentials, which interpolate between this previously studied form and a ramp-based approximation to the Lennard-Jones (LJ) potential. By means of Monte Carlo simulation, we locate the LLCP, the first order high density liquid (HDL)-low density liquid (LDL) coexistence line, and the line of density maxima for a selection of potentials in the series. We observe that as the LJ limit is approached, the LLCP becomes metastable with respect to freezing into a hexagonal close packed crystalline solid. The qualitative nature of the phase behavior in this regime shows a remarkable resemblance to that seen in simulation studies of accurate water models. Specifically, the density of the liquid phase exceeds that of the solid; the gradient of the metastable LDL-HDL line is negative in the pressure (p)-temperature (T) plane; while the line of density maxima in the p-T plane has a shape similar to that seen in water and extends into the stable liquid region of the phase diagram. As such, our results lend weight to the "second critical point" hypothesis as an explanation for the anomalous behavior of water.
线性倾斜或“斜坡”势属于一类核心软化模型,除了通常的液-气临界点外,还具有液-液临界点(LLCP)。此外,它们在密度和压缩性方面表现出热力学异常,其性质可能与水中出现的异常相似。先前对斜坡势的模拟研究仅集中在一种函数形式上,其LLCP在热力学上是稳定的。在这项工作中,我们构建了一系列斜坡势,它们在先前研究的形式和基于斜坡的 Lennard-Jones(LJ)势近似之间进行插值。通过蒙特卡罗模拟,我们确定了该系列中一些势的LLCP、一阶高密度液体(HDL)-低密度液体(LDL)共存线以及密度最大值线。我们观察到,随着接近 LJ 极限,LLCP 相对于冻结成六方密堆积晶体固体变得亚稳。该区域内相行为的定性性质与精确水模型的模拟研究中观察到的非常相似。具体而言,液相密度超过固相密度;在压力(p)-温度(T)平面中,亚稳 LDL-HDL 线的斜率为负;而 p-T 平面中的密度最大值线形状与水中的相似,并延伸到相图的稳定液相区域。因此,我们的结果为“第二临界点”假说是对水的异常行为的一种解释提供了支持。