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On the surface tension of molten salts and its temperature dependence

机译:关于熔盐的表面张力及其温度依赖性

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摘要

A new equation, based on Eyring statistical thermodynamic theory, has been developed to calculate the surface tension and its temperature dependence of high-temperature molten salts. The derived equation has been applied to the calculation of the temperature dependence of the surface tension of molten alkali halides. The model used here is analytical and free of interatomic potentials usually used in computer simulation. The only data needed for the calculation are the sublimation energy and the temperature dependence of the liquid density, which are readily available. The need for such a model stems from the fact that the data in the literature are scarce and the temperature range studied is limited by the experimental demand of high temperatures and clean surface environment, which is difficult to attain. The ratio of surface to bulk Madelung constant was calculated to be 0.95, which is found to be constant for all molten salts studied. This finding is interesting and is presented for the first time. The error in this estimate did not exceed 1.3%. The values calculated do commensurate with the available experimental values for many of the molten salts. The results of temperature-dependent surface tension calculations of molten LiCl (910-1150 K), NaCl (1080-1230 K) and KCl (1050-1300 K) are fitted as gamma = 223.5-0.0814 (T-Tm), gamma = 114.4-0.091 (T-Tm) and gamma = 91 - 0.066 (T-Tm) (mJ m(-2)), respectively, where the surface tension decreases linearly with temperature and agrees well with the existing data.
机译:基于Eyring统计热力学理论,建立了一个计算高温熔盐表面张力及其温度依赖性的新方程。导出的方程已用于计算熔融碱金属卤化物表面张力的温度依赖性。这里使用的模型是解析的,没有计算机模拟中常用的原子间势。计算所需的唯一数据是升华能和液体密度的温度依赖性,这是现成的。之所以需要这样一个模型,是因为文献中的数据很少,而且所研究的温度范围受到高温和清洁表面环境的实验要求的限制,这是很难实现的。经计算,表面与本体马德隆常数之比为0.95,这对于所研究的所有熔盐来说都是常数。这一发现很有趣,而且是第一次出现。这一估计的误差不超过1.3%。计算值与许多熔盐的可用实验值相符。熔融LiCl(910-1150 K)、NaCl(1080-1230 K)和KCl(1050-1300 K)的温度相关表面张力计算结果分别拟合为gamma=223.5-0.0814(T-Tm)、gamma=114.4-0.091(T-Tm)和gamma=91-0.066(T-Tm)(mJ m(-2)),其中表面张力随温度线性降低,并与现有数据一致。

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