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通过 NVT 播种模拟估计对称 Lennard-Jones 混合物中的气泡空化率。

Estimation of bubble cavitation rates in a symmetrical Lennard-Jones mixture by NVT seeding simulations.

机构信息

Departamento de Química-Física I (Unidad de I+D+i asociada al CSIC), Facultad de Ciencias Químicas, Universidad Complutense de Madrid, 28040 Madrid, Spain.

Instituto de Química Física Rocasolano, CSIC, C/ Serrano 119, 28006 Madrid, Spain.

出版信息

J Chem Phys. 2023 Mar 28;158(12):124109. doi: 10.1063/5.0142109.

Abstract

The liquid-vapor transition starts with the formation of a sufficiently large bubble in the metastable liquid to trigger the phase transition. Understanding this process is of fundamental and practical interest, but its study is challenging because it occurs over timescales that are too short for experiments but too long for simulations. The seeding method estimates cavitation rates by simulating a liquid in which a bubble is inserted, thus avoiding the long times needed for its formation. In one-component systems, in the NpT ensemble, the bubble grows or redissolves depending on whether its size is larger or smaller than the critical size, whereas in the NVT ensemble (i.e., at constant number of particles, volume, and temperature), the critical bubble can remain in equilibrium. Provided that a good criterion is used to determine the bubble size, this method, combined with the Classical Nucleation Theory (CNT), gives cavitation rates consistent with those obtained by methods independent of the CNT. In this work, the applicability of NVT seeding to homogeneous cavitation in mixtures is demonstrated, focusing on a partially miscible symmetrical binary Lennard-Jones (LJ) liquid at a temperature within the mixing regime. At the same stretching pressure, cavitation rates are higher in the binary mixture than in the pure liquid due to the lower interfacial free energy of the mixture. Curiously, the cost of creating a bubble is similar in the pure and binary LJ liquids at the same metastability, Δμ/Δμ, with Δμ being the difference in chemical potential between the metastable liquid and coexistence, and Δμ between the spinodal and coexistence.

摘要

液体-蒸汽相变始于亚稳液体中形成足够大的气泡,从而引发相变。理解这个过程具有基础和实际意义,但由于其发生的时间尺度对于实验来说太短,而对于模拟来说又太长,因此研究起来具有挑战性。成核方法通过模拟插入气泡的液体来估计空化率,从而避免了形成气泡所需的长时间。在单组分系统中,在 NpT 系综中,气泡的生长或再溶解取决于其尺寸是否大于或小于临界尺寸,而在 NVT 系综(即,在固定粒子数、体积和温度下),临界气泡可以保持平衡。只要使用良好的标准来确定气泡尺寸,这种方法与经典成核理论 (CNT) 相结合,就可以得到与不依赖 CNT 的方法获得的空化率一致的结果。在这项工作中,证明了 NVT 播种在混合物中均匀空化的适用性,重点关注温度处于混合区域内的部分互溶对称二元 Lennard-Jones (LJ) 液体。在相同的拉伸压力下,由于混合物的界面自由能较低,混合物中的空化率高于纯液体。奇怪的是,在相同的亚稳性下,Δμ/Δμ,其中Δμ是亚稳液体和共存之间的化学势差,以及旋节线和共存之间的化学势差,在纯 LJ 液体和二元 LJ 液体中创建气泡的成本相似。

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