William G. Lowrie Department of Chemical and Biomolecular Engineering, The Ohio State University, Columbus, Ohio 43210, USA.
Department of Chemistry, Louisiana State University, Baton Rouge, Louisiana 70803-1804, USA.
J Chem Phys. 2018 Apr 14;148(14):144312. doi: 10.1063/1.5023567.
We measured the nucleation rates of n-pentane through n-heptane in a supersonic nozzle at temperatures ranging from ca. 109 K to 168 K. For n-pentane and n-hexane, these are the first nucleation rate measurements that have been made, and the trends in the current data agree well with those in the earlier work of Ghosh et al. [J. Chem. Phys. 132, 024307 (2010)] for longer chain alkanes. Complementary Monte Carlo simulations, using the transferable potentials for phase equilibria-united atom potentials, suggest that despite the high degree of supercooling, the critical clusters remain liquid like under experimental conditions for n-pentane through n-heptane, but adopt more ordered structures for n-octane and n-nonane. For all three alkanes, the experimental and simulated nucleation rates are offset by ∼3 orders of magnitude when plotted as a function of ln S/(T/T - 1). Explicitly accounting for the surface tension difference between the real and model substances, or alternatively using the Hale [Phys. Rev. A 33, 4156 (1986); Metall. Mater. Trans. A 23, 1863 (1992)] scaling parameter, Ω, consistent with the model potential, increases the offset to ∼6 orders of magnitude.
我们在超声速喷嘴中测量了正戊烷通过正庚烷的成核速率,温度范围约为 109 K 至 168 K。对于正戊烷和正己烷,这是首次进行的成核速率测量,当前数据的趋势与 Ghosh 等人早期的工作[J. Chem. Phys. 132, 024307 (2010)]一致,适用于更长链烷烃。使用可传递相平衡-联合原子势的蒙特卡罗模拟表明,尽管过冷度很高,但在实验条件下,临界团簇仍然保持液态,适用于正戊烷至正庚烷,但对于正辛烷和正壬烷,它们采用更有序的结构。对于所有三种烷烃,实验和成核速率的模拟在以 ln S/(T/T-1)为函数绘制时相差约 3 个数量级。明确考虑真实物质和模型物质之间的表面张力差异,或者使用与模型势一致的 Hale[Phys. Rev. A 33, 4156 (1986); Metall. Mater. Trans. A 23, 1863 (1992)]缩放参数Ω,将偏差增加到约 6 个数量级。