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Comparison between solutions of the general dynamic equation and the kinetic equation for nucleation and droplet growth

机译:通用动力学方程与成核和液滴生长动力学方程解的比较

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摘要

A comparison is made between two models of homogeneous nucleation and droplet growth. The first is a kinetic model yielding the master equations for the concentrations of molecular clusters. Such a model does not make an explicit distinction between nucleation and droplet growth. The second model treats nucleation and growth separately, fully ignoring stochastic effects, and leads to the continuous general dynamic equation (GDE). Problems in applying the GDE model are discussed. A numerical solution of the kinetic equation is compared with an analytic solution of the GDE for two different cases: (1) the onset of nucleation and (2) the nucleation pulse. The kinetic model yields the thickness of the condensation front in size space as a function of supersaturation and dimensionless surface tension. If the GDE is applied properly, solutions of the GDE and the kinetic equation agree, with the exception of very small clusters, near-critical clusters, and the condensation front.
机译:在均相成核和液滴生长的两个模型之间进行了比较。首先是一个动力学模型,得出分子簇浓度的主方程。这样的模型在成核和液滴生长之间没有明确的区别。第二个模型分别处理成核和生长,完全忽略了随机效应,并得出了连续的一般动力学方程(GDE)。讨论了应用GDE模型的问题。对于两种不同情况,将动力学方程的数值解与GDE的解析解进行了比较:(1)成核的开始和(2)成核脉冲。动力学模型得出了尺寸空间中冷凝前沿的厚度,它是过饱和和无因次表面张力的函数。如果适当地使用GDE,则GDE的解和动力学方程是一致的,除了非常小的簇,近临界簇和冷凝前沿。

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