Römer F, Kraska T
Institute for Physical Chemistry, University Cologne, 50939 Koeln, Germany.
J Chem Phys. 2007 Dec 21;127(23):234509. doi: 10.1063/1.2805063.
Homogeneous nucleation and growth of zinc from supersaturated vapor are investigated by nonequilibrium molecular dynamics simulations in the temperature range from 400 to 800 K and for a supersaturation ranging from log S=2 to 11. Argon is added to the vapor phase as carrier gas to remove the latent heat from the forming zinc clusters. A new parametrization of the embedded atom method for zinc is employed for the interaction potential model. The simulation data are analyzed with respect to the nucleation rates and the critical cluster sizes by two different methods, namely, the threshold method of Yasuoka and Matsumoto [J. Chem. Phys. 109, 8451 (1998)] and the mean first passage time method for nucleation by Wedekind et al. [J. Chem. Phys. 126, 134103 (2007)]. The nucleation rates obtained by these methods differ approximately by one order of magnitude. Classical nucleation theory fails to describe the simulation data as well as the experimental data. The size of the critical cluster obtained by the mean first passage time method is significantly larger than that obtained from the nucleation theorem.
通过非平衡分子动力学模拟,研究了在400至800 K的温度范围内以及对数过饱和度log S = 2至11的条件下,锌从过饱和蒸汽中的均匀成核和生长过程。向气相中添加氩气作为载气,以去除形成的锌簇的潜热。相互作用势模型采用了一种新的锌嵌入原子方法参数化。通过两种不同方法,即安冈和松本的阈值方法[《化学物理杂志》109, 8451 (1998)]以及韦德金德等人的成核平均首次通过时间方法[《化学物理杂志》126, 134103 (2007)],对模拟数据的成核速率和临界簇尺寸进行了分析。通过这些方法获得的成核速率大约相差一个数量级。经典成核理论无法很好地描述模拟数据和实验数据。通过平均首次通过时间方法获得的临界簇尺寸明显大于从成核定理获得的尺寸。