TY - JOUR
T1 - Monte Carlo Simulation of Grain Growth in Three-dimensions
AU - Saito, Yoshiyuki
PY - 1998
Y1 - 1998
N2 - The temporal evolution and morphology of grain growth in three dimensions were simulated by Monte Carlo method. In order to prevent impingement of grains of like orientation, new algorithm was adopted. The anisotropy of the grain boundary energy is incorporated into the model. Compared with the case in which no anisotropy of boundary energy is assumed, the suppression of grain growth was observed at the initial stage of growth in the grain structure with anisotropic grain boundary energy. However, the growth rate is higher at the later stage. The grain size and the face number distributions become broad. To evaluate the profile of the grain size distribution, a parameter called microstructural entropy, S, is defined. It was shown that the characteristics of size distribution profile may be represented by the value S. The average size of n-faced grain is proportional to the grain face number, n. The effect of the anisotropy of grain boundary energy on the n-dependence of the average grain size is not evident. The nearest neighbour face number correlation similar to the Aboav-Weaire relation in two dimension is observed in both grain structures with isotropic grain boundary energy and anisotropic grain boundary energy.
AB - The temporal evolution and morphology of grain growth in three dimensions were simulated by Monte Carlo method. In order to prevent impingement of grains of like orientation, new algorithm was adopted. The anisotropy of the grain boundary energy is incorporated into the model. Compared with the case in which no anisotropy of boundary energy is assumed, the suppression of grain growth was observed at the initial stage of growth in the grain structure with anisotropic grain boundary energy. However, the growth rate is higher at the later stage. The grain size and the face number distributions become broad. To evaluate the profile of the grain size distribution, a parameter called microstructural entropy, S, is defined. It was shown that the characteristics of size distribution profile may be represented by the value S. The average size of n-faced grain is proportional to the grain face number, n. The effect of the anisotropy of grain boundary energy on the n-dependence of the average grain size is not evident. The nearest neighbour face number correlation similar to the Aboav-Weaire relation in two dimension is observed in both grain structures with isotropic grain boundary energy and anisotropic grain boundary energy.
KW - Abnormal grain growth
KW - Computer simulation
KW - Grain face number distribution
KW - Grain growth
KW - Grain size distribution
KW - Growth law
KW - Monte Carlo method
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M3 - Article
AN - SCOPUS:0031655240
VL - 38
SP - 559
EP - 566
JO - Transactions of the Iron and Steel Institute of Japan
JF - Transactions of the Iron and Steel Institute of Japan
SN - 0915-1559
IS - 6
ER -