马氏体相变的相场模型研究进展

于继东 姚松林 吴强

于继东, 姚松林, 吴强. 马氏体相变的相场模型研究进展[J]. 高压物理学报, 2021, 35(4): 040109. doi: 10.11858/gywlxb.20210772
引用本文: 于继东, 姚松林, 吴强. 马氏体相变的相场模型研究进展[J]. 高压物理学报, 2021, 35(4): 040109. doi: 10.11858/gywlxb.20210772
YU Jidong, YAO Songlin, WU Qiang. Advances of Phase Field Modeling of Martensitic Phase Transformation[J]. Chinese Journal of High Pressure Physics, 2021, 35(4): 040109. doi: 10.11858/gywlxb.20210772
Citation: YU Jidong, YAO Songlin, WU Qiang. Advances of Phase Field Modeling of Martensitic Phase Transformation[J]. Chinese Journal of High Pressure Physics, 2021, 35(4): 040109. doi: 10.11858/gywlxb.20210772

马氏体相变的相场模型研究进展

doi: 10.11858/gywlxb.20210772
基金项目: 冲击波物理与爆轰物理重点实验室基金(6142A03191001);国家自然科学基金(11602249)
详细信息
    作者简介:

    于继东(1981-),男,博士,副研究员,主要从事高压物理力学研究. E-mail:yujidong@caep.cn

  • 中图分类号: O521.2

Advances of Phase Field Modeling of Martensitic Phase Transformation

  • 摘要: 马氏体相变是一种无扩散位移型一阶相变,会形成针状、表面浮凸等复杂的特征微结构。马氏体相变的特征微结构会显著影响材料的宏观物理力学特性,相关研究具有重要的科学和工程价值。相场模型具有可处理复杂界面演化问题的独特优势,已成为模拟马氏体相变的有力的理论与计算工具。概述了马氏体相变相场模型的研究进展,并分析了相场模型应用于弱马氏体相变和重构型马氏体相变的特点。

     

  • 图  TiNi合金降温-升温过程中的原位SEM图像:(a) 290 K,(b)降温至222 K,(c)再升温至265 K,(d)再升温至290 K[54]

    Figure  1.  Series of in situ SEM images of TiNi alloy at (a) 290 K and (b) 222 K upon cooling, and (c) 265 K and (d) 290 K upon heating[54]

    图  冲击加载下金属铁回收样品的TEM图像[55]

    Figure  2.  TEM image showing the microstructure of shock-compressed iron[55]

    图  铁的$\alpha $$\varepsilon $正相变过程(红线)及$\varepsilon $$\alpha $′逆相变过程(蓝线)中对称性相关的变体示意图[70]

    Figure  3.  Schematic illustration of the multiple symmetry-related variants for the forward $\alpha $$\varepsilon $ (red) and the reverse $\varepsilon $$\alpha $′ (blue) phase transitions in iron[70]

    图  塑性变形对双晶结构在压剪作用下高压相成核生长的影响[50]

    Figure  4.  Effect of dislocation band on nucleation and evolution of the high pressure phase of bicrystal under compression and shear[50]

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