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铜中熔体的均匀形核与生长

Homogeneous nucleation and growth of melt in copper.

作者信息

Zheng Lianqing, An Qi, Xie Yun, Sun Zehui, Luo Sheng-Nian

机构信息

School of Computational Science, Florida State University, Tallahassee, Florida 32306, USA.

出版信息

J Chem Phys. 2007 Oct 28;127(16):164503. doi: 10.1063/1.2790424.

Abstract

Molecular dynamics simulations are conducted to investigate homogeneous nucleation and growth of melt in copper described by an embedded-atom method (EAM) potential. The accuracy of this EAM potential for melting is validated by the equilibrium melting point obtained with the solid-liquid coexistence method and the superheating-supercooling hysteresis method. We characterize the atomistic melting process by following the temperature and time evolution of liquid atoms. The nucleation behavior at the extreme superheating is analyzed with the mean-first-passage-time (MFPT) method, which yields the critical size, steady-state nucleation rate, and the Zeldovich factor. The value of the steady-state nucleation rate obtained from the MFPT method is consistent with the result from direct simulations. The size distribution of subcritical nuclei appears to follow a power law similar to three-dimensional percolation. The diffuse solid-liquid interface has a sigmoidal profile with a 10%-90% width of about 12 A near the critical nucleation. The critical size obtained from our simulations is in reasonable agreement with the prediction of classical nucleation theory if the finite interface width is considered. The growth of melt is coupled with nucleation and can be described qualitatively with the Johnson-Meh-Avrami law. System sizes of 10(3)-10(6) atoms are explored, and negligible size dependence is found for bulk properties and for the critical nucleation.

摘要

开展分子动力学模拟,以研究由嵌入原子法(EAM)势描述的铜熔体的均匀形核与生长。通过固液共存法和过热度-过冷度滞后法获得的平衡熔点,验证了该EAM势对熔化描述的准确性。我们通过追踪液态原子的温度和时间演化来表征原子尺度的熔化过程。用平均首次通过时间(MFPT)方法分析了极端过热度下的形核行为,该方法可得出临界尺寸、稳态形核率和泽尔多维奇因子。从MFPT方法获得的稳态形核率值与直接模拟结果一致。亚临界核的尺寸分布似乎遵循类似于三维渗流的幂律。在临界形核附近,漫散的固液界面具有S形轮廓,10%-90%宽度约为12 Å。如果考虑有限的界面宽度,我们模拟得到的临界尺寸与经典形核理论的预测相当吻合。熔体的生长与形核相耦合,可用约翰逊-梅尔-阿夫拉米定律进行定性描述。研究了含有10³-10⁶个原子的系统尺寸,发现对于体性质和临界形核,尺寸依赖性可忽略不计。

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