Varnik Fathollah, Franosch Thomas
Interdisciplinary Centre for Advanced Materials Simulation (ICAMS), Ruhr-Universität Bochum, Universitätsstraße 150, D-44780 Bochum, Germany.
J Phys Condens Matter. 2016 Apr 6;28(13):133001. doi: 10.1088/0953-8984/28/13/133001. Epub 2016 Mar 4.
The relaxation dynamics of glass forming liquids and their structure are influenced in the vicinity of confining walls. This effect has mostly been observed to be a monotonic function of the slit width. Recently, a qualitatively new behaviour has been uncovered by Mittal and coworkers, who reported that the single particle dynamics in a hard-sphere fluid confined in a planar slit varies in a non-monotonic way as the slit width is decreased from five to roughly two particle diametres (Mittal et al 2008 Phys. Rev. Lett. 100 145901). In view of the great potential of this effect for applications in those fields of science and industry, where liquids occur under strong confinement (e.g. nano-technology), the number of researchers studying various aspects and consequences of this non-monotonic behaviour has been rapidly growing. This review aims at providing an overview of the research activity in this newly emerging field. We first briefly discuss how competing mechanisms such as packing effects and short-range attraction may lead to a non-monotonic glass transition scenario in the bulk. We then analyse confinement effects on the dynamics of fluids using a thermodynamic route which relates the single particle dynamics to the excess entropy. Moreover, relating the diffusive dynamics to the Widom's insertion probability, the oscillations of the local dynamics with density at moderate densities are fairly well described. At high densities belonging to the supercooled regime, however, this approach breaks down signaling the onset of strongly collective effects. Indeed, confinement introduces a new length scale which in the limit of high densities and small pore sizes competes with the short-range local order of the fluid. This gives rise to a non-monotonic dependence of the packing structure on confinement, with a corresponding effect on the dynamics of structural relaxation. This non-monotonic effect occurs also in the case of a cone-plate type channel, where the degree of confinement varies with distance from the apex. This is a very promising issue for future research with the possibility of uncovering the existence of alternating glassy and liquid-like domains.
玻璃形成液体的弛豫动力学及其结构在受限壁附近会受到影响。这种效应大多被观察到是狭缝宽度的单调函数。最近,米塔尔及其同事发现了一种定性的新行为,他们报告称,当平面狭缝中受限的硬球流体的狭缝宽度从五个粒子直径减小到大约两个粒子直径时,单粒子动力学以非单调方式变化(米塔尔等人,《物理评论快报》,2008年,第100卷,第145901页)。鉴于这种效应在液体处于强受限状态的科学和工业领域(如纳米技术)的应用中具有巨大潜力,研究这种非单调行为各个方面和后果的研究人员数量一直在迅速增加。这篇综述旨在概述这个新兴领域的研究活动。我们首先简要讨论诸如堆积效应和短程吸引力等竞争机制如何可能导致体相中出现非单调的玻璃化转变情况。然后,我们使用一种将单粒子动力学与过剩熵联系起来的热力学途径来分析受限对流体动力学的影响。此外,将扩散动力学与维登插入概率联系起来,可以很好地描述中等密度下局部动力学随密度的振荡。然而,在属于过冷区域的高密度下,这种方法失效,这表明出现了强集体效应。实际上,受限引入了一个新的长度尺度,在高密度和小孔径的极限情况下,它与流体的短程局部有序相互竞争。这导致堆积结构对受限的非单调依赖性,对结构弛豫动力学产生相应影响。这种非单调效应在锥板型通道的情况下也会出现,其中受限程度随离顶点的距离而变化。这是一个非常有前景的未来研究课题,有可能揭示交替的玻璃态和液态区域的存在。