The melting mechanisms of UO2 nanocrystals: A molecular dynamics simulation

K. Nekrasov, A. Boyarchenkov, Sanjeev K. Gupta, A. Kupryazhkin
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引用次数: 1

Abstract

A molecular dynamics simulation of the melting of UO2 nanocrystals of the optimal truncated octahedron shape in the size range from 4317 to 381174 ions was carried out. The dependence of the melting temperature of the nanocrystals on the size was obtained at the time of evolution of the model system up to 150 ns. This dependence was characterized by nonlinearity caused by a change in the melting mechanism corresponding to the transition from larger nanocrystals to smaller ones. The nanocrystals containing more than 20 000 ions undergo the phase transition as a result of the formation of the surface melt on a single (111) face, which caused the irreversible propagation of the melt into the bulk. Smaller crystallites could melt at temperatures below the crystallization temperature of the (111) face, provided that two adjacent faces melt simultaneously due to the thermal activation. The difference in melting temperatures of the largest and smallestmodel crystals was 320K, which corresponds to the experimental estimates.A molecular dynamics simulation of the melting of UO2 nanocrystals of the optimal truncated octahedron shape in the size range from 4317 to 381174 ions was carried out. The dependence of the melting temperature of the nanocrystals on the size was obtained at the time of evolution of the model system up to 150 ns. This dependence was characterized by nonlinearity caused by a change in the melting mechanism corresponding to the transition from larger nanocrystals to smaller ones. The nanocrystals containing more than 20 000 ions undergo the phase transition as a result of the formation of the surface melt on a single (111) face, which caused the irreversible propagation of the melt into the bulk. Smaller crystallites could melt at temperatures below the crystallization temperature of the (111) face, provided that two adjacent faces melt simultaneously due to the thermal activation. The difference in melting temperatures of the largest and smallestmodel crystals was 320K, which corresponds to the experimenta...
UO2纳米晶的熔化机制:分子动力学模拟
对尺寸为4317 ~ 381174个离子的最佳截断八面体UO2纳米晶体的熔融过程进行了分子动力学模拟。在模型体系演化至150ns时,得到了纳米晶体的熔化温度与尺寸的关系。这种依赖关系的特点是由由大纳米晶体向小纳米晶体转变所对应的熔化机制变化引起的非线性。含有超过20,000个离子的纳米晶体由于在单个(111)面上形成表面熔体而经历相变,这导致熔体不可逆地传播到体中。较小的晶体可以在低于(111)晶面结晶温度的温度下熔化,前提是相邻的两个晶面由于热活化而同时熔化。最大和最小模型晶体的熔化温度差为320K,与实验估计相符。对尺寸为4317 ~ 381174个离子的最佳截断八面体UO2纳米晶体的熔融过程进行了分子动力学模拟。在模型体系演化至150ns时,得到了纳米晶体的熔化温度与尺寸的关系。这种依赖关系的特点是由由大纳米晶体向小纳米晶体转变所对应的熔化机制变化引起的非线性。含有超过20,000个离子的纳米晶体由于在单个(111)面上形成表面熔体而经历相变,这导致熔体不可逆地传播到体中。较小的晶体可以在低于(111)晶面结晶温度的温度下熔化,前提是相邻的两个晶面由于热活化而同时熔化。最大和最小模型晶体的熔化温度差为320K,与实验结果相符。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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