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Molecular Dynamics Simulation of the Surface Tension of Aqueous Sodium Chloride: from Dilute to Highly Supersaturated Solutions and Molten Salt

机译:氯化钠水溶液表面张力的分子动力学模拟:从稀溶液到高过饱和溶液和熔盐

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摘要

Sodium chloride (NaCl) is one of the key components of atmospheric aerosols. The surface tension of aqueous NaCl solution (σNaCl,sol) and its concentration dependence are essential to determine the equilibrium water vapor pressure of aqueous NaCl droplets. Supersaturated NaCl solution droplets are observed in laboratory experiments and under atmospheric conditions, but the experimental data for σNaCl,sol are mostly limited up to sub-saturated solutions. In this study, the surface tension of aqueous NaCl is investigated by molecular dynamics (MD) simulations and pressure tensor method from dilute to highly supersaturated solutions. We show that the linear approximation of concentration dependence of σNaCl,sol at molality scale can be extended to the supersaturated NaCl solution until a molality of ~9.6 mol kg−1 (i.e., solute mass fraction (xNaCl) of ~0.36). Energetic analyses show that this monotonic increase of surface tension is driven by the increase of excessive surface enthalpy (∆H) as the solution becomes concentrated. After that, the simulated σNaCl,sol remains almost unchanged until xNaCl of ~0.47 (near the concentration upon efflorescence). The existence of the "inflection point" at xNaCl of ~0.36 and the stable surface tension of xNaCl between ~0.36 and ~0.47 can be attributed to a competitive growth of excessive surface entropy term (T · ∆S) and the excessive surface enthalpy term (∆H). After a "second inflection point" at xNaCl of ~0.47, the simulated σNaCl,sol gradually regains the growing momentum with a tendency to approach the surface tension of molten NaCl (~148.4 mN m−1 at 298.15 K, MD simulation based extrapolation). This fast increase of σNaCl,sol at xNaCl > 0.47 is primarily still an excessive surface enthalpy-driving process, although contribution from concurrent fluctuation of excessive surface entropy is expected but in a relatively smaller scale. Our results reveal different regimes of concentration dependence of the surface tension of aqueous NaCl at 298.15 K: a water-dominated regime (xNaCl from 0 to ~0.36), a transition regime (xNaCl from ~0.36 to ~0.47) and a molten NaCl-dominated regime (xNaCl from ~0.47 to 1).
机译:氯化钠(NaCl)是大气气溶胶的关键成分之一。 NaCl水溶液(σNaCl,sol)的表面张力及其浓度依赖性对于确定NaCl液滴的平衡水蒸气压至关重要。在实验室实验和大气条件下观察到过饱和的NaCl溶液液滴,但是σNaCl,sol的实验数据主要限于亚饱和溶液。在这项研究中,NaCl水溶液的表面张力通过分子动力学(MD)模拟和压力张量方法研究,从稀溶液到高过饱和溶液。我们表明,在摩尔浓度范围内,σNaCl,sol浓度依赖性的线性近似可以扩展到过饱和NaCl溶液,直到摩尔浓度为〜9.6 mol kg-1(即,溶质质量分数(xNaCl)为〜0.36)。能量分析表明,表面张力的这种单调增加是由于溶液浓缩时过量的表面焓(∆H)的增加所致。之后,模拟的σNaCl,sol几乎保持不变,直到xNaCl为〜0.47(接近风化浓度)为止。 xNaCl处“拐点”的存在为〜0.36,xNaCl的稳定表面张力在〜0.36至〜0.47之间,这可以归因于过量的表面熵项(T·∆S)和过量的表面焓项的竞争性增长。 (∆H)。在xNaCl处的“第二拐点”为〜0.47之后,模拟的σNaCl,sol逐渐恢复增长的势头,趋向于接近熔融NaCl的表面张力(在298.15〜K处约为148.4 mN m-1,基于MD模拟的外推法) 。尽管预期由过量表面熵的同时波动引起的贡献,但是在xNaCl >> 0.47的情况下,σNaCl,sol的快速增加仍然仍然是过量的表面焓驱动过程,但是规模相对较小。我们的研究结果揭示了298.15 K下NaCl水溶液的表面张力的浓度依赖性的不同机制:水主导机制(xNaCl从0到〜0.36),过渡机制(xNaCl从〜0.36到〜0.47)和熔融NaCl-主导制度(xNaCl从〜0.47到1)。

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