γα相变的室温动态特性

李英雷 叶想平 王志刚

李英雷, 叶想平, 王志刚. 铈γ→α相变的室温动态特性[J]. 爆炸与冲击, 2017, 37(3): 459-463. doi: 10.11883/1001-1455(2017)03-0459-05
引用本文: 李英雷, 叶想平, 王志刚. 铈γα相变的室温动态特性[J]. 爆炸与冲击, 2017, 37(3): 459-463. doi: 10.11883/1001-1455(2017)03-0459-05
Li Yinglei, Ye Xiangping, Wang Zhigang. Dynamic characteristics of the γ→α phase transition of cerium at room temperature[J]. Explosion And Shock Waves, 2017, 37(3): 459-463. doi: 10.11883/1001-1455(2017)03-0459-05
Citation: Li Yinglei, Ye Xiangping, Wang Zhigang. Dynamic characteristics of the γα phase transition of cerium at room temperature[J]. Explosion And Shock Waves, 2017, 37(3): 459-463. doi: 10.11883/1001-1455(2017)03-0459-05

γα相变的室温动态特性

doi: 10.11883/1001-1455(2017)03-0459-05
详细信息
    作者简介:

    李英雷(1974-),男,博士,副研究员,ylli@caep.cn

  • 中图分类号: O381

Dynamic characteristics of the γα phase transition of cerium at room temperature

  • 摘要: 通过试样组件尺寸匹配设计的被动围压SHPB实验,获得了99.8%纯铈在1.7GPa静水压内的、包含γα相变和逆相变过渡区的室温动态静水压-体应变连续曲线。研究显示:室温铈γα相变是具有明显滞后现象的一级相变,而非以往研究认为的体积跃变的一级相变;相变过渡区的静水压范围是0.8~1.3GPa。逆相变过渡区的静水压范围是0.6~1.1GPa;逆相变过渡区的静水压-体应变曲线滞后于相变过渡区的静水压-体应变曲线0.15GPa静水压;在相变和逆相变过渡区内,静水压-体应变曲线按照约4.2GPa体积模量的线性关系演化;演化机制为γα两相均匀混合、静水压驱动两相组份转化。基于该演化机制,构建了描述相变前后和相变过程的静水压-体应变响应的三段线性模型。
  • 图  1  实验装置结构示意图

    Figure  1.  Schematic of experiment system

    图  2  室温铈的静水压-体应变曲线

    Figure  2.  Curves of hydrostatic pressure and volume strain of cerium at room temperature

    图  3  室温铈静水压-体应变的实验曲线与模型曲线对比

    Figure  3.  Comparison of experimental and model simulating curves of hydrostatic pressure and volume strain of cerium at room temperature

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    Li Yinglei, Ye Xiangping, Zhang Zugen, et al.A design of passive confined SHPB experiment for materials with low bulk modulus[J].Explosion and Shcok Waves, 2014, 34(6):667-672. http://www.bzycj.cn/CN/abstract/abstract9400.shtml
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出版历程
  • 收稿日期:  2015-11-18
  • 修回日期:  2016-04-05
  • 刊出日期:  2017-05-25

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