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From Molecular Dynamics to hydrodynamics - a novel Galilean invariant thermostat

机译:从分子动力学到流体动力学 - 一种新颖的伽利略不变量   恒温器

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摘要

This article proposes a novel thermostat applicable to any particle-baseddynamic simulation. Each pair of particles is thermostated either (withprobability P) with a pairwise Lowe-Andersen thermostat, or (with probability1-P) with a thermostat that is introduced here, which is based on a pairwiseinteraction similar to the Nose-Hoover thermostat. When the pairwiseNose-Hoover thermostat dominates (low P), the liquid has a high diffusioncoefficient and low viscosity, but when the Lowe-Andersen thermostat dominates,the diffusion coefficient is low and viscosity is high. This novelNose-Hoover-Lowe-Andersen thermostat is Galilean invariant and preserves bothtotal linear and angular momentum of the system, due to the fact that thethermostatic forces between each pair of the particles are pairwise additiveand central. We show by simulation that this thermostat also preserveshydrodynamics. For the (non-interacting) ideal gas at P=0, the diffusioncoefficient diverges and viscosity is zero, while for P>0 it has a finitevalue. By adjusting probability P, the Schmidt number can be varied by ordersof magnitude. The temperature deviation from the required value is at least anorder of magnitude smaller than in Dissipative Particle Dynamics (DPD), whilethe equilibrium properties of the system are very well reproduced. Applicationsof this thermostat include all standard molecular dynamic simulations of denseliquids and solids with any type of force field, as well as hydrodynamicsimulation of multi-phase systems with largely different bulk viscosities,including surface viscosity, and of dilute gases and plasmas.
机译:本文提出了一种适用于任何基于粒子的动态仿真的新型恒温器。每对粒子都使用成对的Lowe-Andersen恒温器(概率为P)或此处引入的恒温器(概率为1-P)进行恒温,该恒温器基于类似于Noose-Hoover恒温器的成对相互作用。当成对的Nose-Hoover恒温器占主导地位(低P)时,液体具有较高的扩散系数和低粘度,而当Lowe-Andersen恒温器占主导地位时,扩散系数低且粘度高。这种新颖的Nose-Hoover-Lowe-Andersen恒温器是伽利略不变式,并且由于每对粒子之间的恒温力是成对加和中心的事实,因此既保留了系统的总线性动量又保留了系统的角动量。通过仿真显示,该恒温器还保留了流体动力学。对于在P = 0处的(非相互作用)理想气体,扩散系数发散并且粘度为零,而对于P> 0,它具有一个有限值。通过调整概率P,施密特数可以改变几个数量级。与要求值的温度偏差至少比“耗散粒子动力学”(DPD)中小一个数量级,而系统的平衡特性可以很好地再现。该恒温器的应用包括在任何类型的力场下对稠密液体和固体进行的所有标准分子动力学模拟,以及体积粘度(包括表面粘度),稀薄气体和等离子体的多相系统的流体动力学模拟。

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