A simulation study of microstructure evolution during solidification process of liquid metal Ni
Liu Hai-Rong, Rangsu Liu, Ailong Zhang, Zhaoyang Hou, Xin Wang, Tian Ze-An
Abstract
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Liu Hai-Rong, Rangsu Liu, Ailong Zhang, Zhaoyang Hou, Xin Wang, Tian Ze-An
Abstract
Open-access reader
A molecular dynamics simulation study has been performed for the microstructure evolution in a liquid metal Ni system during crystallization process at two cooling rates by adopting the embedded atom method (EAM) model potential. The bond-type index method of Honeycutt–Andersen (HA) and a new cluster-type index method (CTIM-2) have been used to detect and analyse the microstructures in this system. It is demonstrated that the cooling rate plays a critical role in the microstructure evolution: below the crystallization temperature T c , the effects of cooling rate are very remarkable and can be fully displayed. At different cooling rates of 2.0 × 10 13 K · s −1 and 1.0 × 10 12 K · s −1 , two different kinds of crystal structures are obtained in the system. The first one is the coexistence of the hcp (expressed by (12 0 0 0 6 6) in CTIM-2) and the fcc (12 0 0 0 12 0) basic clusters consisting of 1421 and 1422 bond-types, and the hcp basic cluster becomes the dominant one with decreasing temperature, the second one is mainly the fcc (12 0 0 0 12 0) basic clusters consisting of 1421 bond-type, and their crystallization temperatures T c would be 1073 and 1173 K, respectively.
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A molecular dynamics simulation study has been performed for the microstructure evolution in a liquid metal Ni system during crystallization process at two cooling rates by adopting the embedded atom method (EAM) model potential. The bond-type index method of Honeycutt–Andersen (HA) and a new cluster-type index method (CTIM-2) have been used to detect and analyse the microstructures in this system. It is demonstrated that the cooling rate plays a critical role in the microstructure evolution: below the crystallization temperature T c , the effects of cooling rate are very remarkable and can be fully displayed. At different cooling rates of 2.0 × 10 13 K · s −1 and 1.0 × 10 12 K · s −1 , two different kinds of crystal structures are obtained in the system. The first one is the coexistence of the hcp (expressed by (12 0 0 0 6 6) in CTIM-2) and the fcc (12 0 0 0 12 0) basic clusters consisting of 1421 and 1422 bond-types, and the hcp basic cluster becomes the dominant one with decreasing temperature, the second one is mainly the fcc (12 0 0 0 12 0) basic clusters consisting of 1421 bond-type, and their crystallization temperatures T c would be 1073 and 1173 K, respectively.
Key concepts: Crystallization, Microstructure, Materials science, Cluster (spacecraft), Molecular dynamics, Atom (system on chip), Thermodynamics, Liquid metal