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An atomic-level mechanism of annealing twinning in copper observed by molecular dynamics simulation

机译:分子动力学模拟观察到铜退火孪晶的原子级机理

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The current experimental methods are not able to reveal the actual processes of atomic movements during twinning and thus are incapable of clarifying the underlying mechanisms of annealing twinning, which are still not clear at present. We developed a method of molecular dynamics simulation to study the mechanism of annealing twinning in copper at an atomic-level. The simulation revealed that a annealing twin can be developed quickly from a pair of grains with σ3 misorientation interfaced by a (5?1?1?)/ (1?11) asymmetric boundary. The twinning proceeds by a mechanism in which every three adjacent (5?1?1?) atomic layers merge into a (1?1?1?) layer in the (5?1?1?) side, while the atomic arrangement in the (1?11) side remains unchanged. Such twinning takes place readily upon annealing at temperatures ranging from 700 to 1300 K, without requiring any extra driving force, indicating that annealing twinning in copper is indeed a thermally activated process with an activation energy estimated to be 0.1 eV. Similar annealing twinning is also observed in another two pairs of grains with σ3 misorientation interfaced by (8?22)/(022) and (2?44)/(2?00) asymmetric boundaries, respectively, yet their twinning rates are much slower than that of the (5?1?1?)/ (1?11) grain pair, suggesting a different mechanism governing the process. The simulation also suggested that annealing twinning may involve two separate steps of which one is the formation of grain pairs with σ3 misorientation and the other is the fine-tuning through which the grain pairs with σ3 misorientation are converted into ideal annealing twins, which can grow larger with grain growth.
机译:当前的实验方法无法揭示孪生过程中原子运动的实际过程,因此无法阐明退火孪生的潜在机理,目前尚不清楚。我们开发了一种分子动力学模拟的方法,以研究原子级铜的退火孪生机理。模拟结果表明,退火双晶可以快速地从一对取向为(3→5→1→1→)/(1→11)的σ3取向错误的晶粒上形成。孪生通过一种机理进行,在该机理中,每三个相邻的(5?1?1?)原子层在(5?1?1?1)侧合并为(1?1?1?1)层,而原子排列在(1?11)面保持不变。这种孪生在700至1300 K的温度范围内退火时很容易发生,而无需任何额外的驱动力,这表明铜中的退火孪生确实是一种热活化过程,其活化能估计为0.1 eV。在另外两对σ3取向错误的晶粒中也观察到相似的退火孪晶,它们分别由(8?22)/(022)和(2?44)/(2?00)不对称边界交界,但它们的孪生速率要慢得多与(5?1?1?)/(1?11)晶粒对相比,表明了控制该过程的机制不同。模拟还表明,退火孪晶可能涉及两个独立的步骤,其中一个是形成具有σ3取向错误的晶粒对,另一个是进行微调,通过该微调将具有σ3取向错误的晶粒对转换为理想的退火孪晶,并可以生长随着谷物的生长而增大。

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