晶体对称性和马氏体变化的可逆性
Kaushik Bhattacharya1, Sergio Conti, Giovanni Zanzotto
1Division of Engineering and Applied Science, California Institute of Technology, Pasadena, California 91125, USA. bhatta@caltech.edu
Nature
|March 6, 2004
概括
马石转换表现出基于晶体对称性的可逆或不可逆行为. 形状记忆合金的可逆性与共享的对称性组相关,允许最小可塑性的转换.
科学领域:
- 材料科学 材料科学 材料科学
- 固态物理 固态物理
- 晶体学 晶体学是指结晶学.
背景情况:
- 马石转换是在各种材料中观察到的无扩散相变.
- 这些转变涉及到快速的晶体结构变化和微观结构的发展.
- 转变可以是不可逆转的 (例如,炼钢) 或可逆转的 (例如,形状记忆合金).
研究的目的:
- 阐明马氏体变化的不同可逆性的根本原因.
- 建立一个理论框架,解释可逆和不可逆的马氏体行为.
- 将宏观可逆性与底层的晶体对称性变化联系起来.
主要方法:
- 运用了数学理论和数值模拟.
- 分析的重点在于在马氏体转变过程中晶体对称性的变化.
- 研究了格子不变剪切和相变的能量障碍.
主要成果:
- 可逆性的必要条件是将母相和产物相对称群纳入一个共同的有限对称群.
- 当满足这种条件时,格子不变剪切的能量屏障超过相变的能量屏障,从而实现几乎无可塑性的转换.
- 在其他情况下,不可逆性是不可避免的,因为塑性变形的能量屏障不高于相变屏障.
结论:
- 晶体对称性决定了马氏体变化的宏观可逆性.
- 这些发现为了解形状记忆合金行为和其他马石现象提供了理论基础.
- 实验观察证实了对称性在确定转换可逆性的关键作用.
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