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气-固相变动力学:结构、生长与机制

Kinetics of Vapor-Solid Phase Transitions: Structure, Growth, and Mechanism.

作者信息

Midya Jiarul, Das Subir K

机构信息

Theoretical Sciences Unit, Jawaharlal Nehru Centre for Advanced Scientific Research, Jakkur P.O., Bangalore 560064, India.

出版信息

Phys Rev Lett. 2017 Apr 21;118(16):165701. doi: 10.1103/PhysRevLett.118.165701. Epub 2017 Apr 17.

Abstract

The kinetics of the separation between low and high density phases in a single component Lennard-Jones model is studied via molecular dynamics simulations, at very low temperatures, in the space dimension d=2. For densities close to the vapor branch of the coexistence curve, disconnected nanoscale clusters of the high density phase exhibit essentially ballistic motion. Starting from nearly circular shapes, at the time of nucleation, these clusters grow via sticky collisions, gaining filamentlike nonequilibrium structure at a later time, with a very low fractal dimensionality. The origin of the latter is shown to lie in the low mobility of the constituent particles, in the corresponding cluster reference frame, due to the (quasi-long-range) crystalline order. Standard self-similarity in the domain pattern, typically observed in the kinetics of phase transitions, is found to be absent. This invalidates the common method, that provides a growth law comparable to that in solid mixtures, of quantifying growth. An appropriate alternative approach, involving the fractality, quantifies the growth of the characteristic "length" to be a power law with time, the exponent being strongly temperature dependent. The observed growth law is in agreement with the outcome of a nonequilibrium kinetic theory.

摘要

通过分子动力学模拟,研究了二维空间中单个组分的 Lennard-Jones 模型在极低温下低密度相和高密度相之间分离的动力学。对于接近共存曲线气相分支的密度,高密度相的不相连纳米级团簇表现出基本的弹道运动。在成核时,这些团簇从近似圆形开始,通过粘性碰撞生长,在稍后的时间获得丝状非平衡结构,分形维数非常低。结果表明,由于(准长程)晶体有序性,在相应的团簇参考系中,组成粒子的低迁移率导致了后者的出现。在相变动力学中通常观察到的域模式中的标准自相似性不存在。这使得常用的、提供与固体混合物中生长规律相当的生长量化方法无效。一种涉及分形性的适当替代方法将特征“长度”的生长量化为时间的幂律,指数强烈依赖于温度。观察到的生长规律与非平衡动力学理论的结果一致。

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