激光金属沉积GH4169在不同应变率下的剪切特性及破坏机理研究

李小龙 李鹏辉 郭伟国 袁康博

李小龙, 李鹏辉, 郭伟国, 袁康博. 激光金属沉积GH4169在不同应变率下的剪切特性及破坏机理研究[J]. 爆炸与冲击, 2020, 40(8): 083101. doi: 10.11883/bzycj-2019-0254
引用本文: 李小龙, 李鹏辉, 郭伟国, 袁康博. 激光金属沉积GH4169在不同应变率下的剪切特性及破坏机理研究[J]. 爆炸与冲击, 2020, 40(8): 083101. doi: 10.11883/bzycj-2019-0254
LI Xiaolong, LI Penghui, GUO Weiguo, YUAN Kangbo. Shear characteristics and failure mechanism of laser metal deposition GH4169 at different strain rates[J]. Explosion And Shock Waves, 2020, 40(8): 083101. doi: 10.11883/bzycj-2019-0254
Citation: LI Xiaolong, LI Penghui, GUO Weiguo, YUAN Kangbo. Shear characteristics and failure mechanism of laser metal deposition GH4169 at different strain rates[J]. Explosion And Shock Waves, 2020, 40(8): 083101. doi: 10.11883/bzycj-2019-0254

激光金属沉积GH4169在不同应变率下的剪切特性及破坏机理研究

doi: 10.11883/bzycj-2019-0254
基金项目: 国家自然科学基金(11872051,11572261,11372255)
详细信息
    作者简介:

    李小龙(1995- ),男,硕士研究生,lxl006@mail.nwpu.edu.cn

    通讯作者:

    李鹏辉(1991- ),男,博士研究生,lipenghui359@mail.nwpu.edu.cn

  • 中图分类号: O347.3

Shear characteristics and failure mechanism of laser metal deposition GH4169 at different strain rates

  • 摘要: 为了能在传统的分离式Hopkinson压杆上准确可靠地测试激光金属沉积GH4169的动态剪切特性,基于数值模拟方法对比分析了三种不同动态剪切试样形式及尺寸对剪切区应力分布的影响,结果表明:经过尺寸优化后的双剪切试样的剪切区剪应力占主导地位,可实现近似纯剪切的动态剪切实验。利用此试样形式,系统测试了不同取向(扫描方向、沉积方向)的LMD GH4169试样在不同应变率下的剪切应力应变曲线,并对破坏后试样进行了SEM分析观察。结果表明:(1) 本文中选用的试样形式剪切纯度高,应力沿剪切区宽度厚度分布均匀,可以更好地得到材料的动态剪切特性;(2) 对实验所得剪应力-剪应变曲线进行分析,发现本材料在扫描路径方向和沉积方向并没有表现出明显的各向异性,但随着应变率的增加,具有明显的应变率强化效应;将单轴压缩和动态剪切应力应变曲线同时转换为等效应力应变曲线,对比证实了试样形式能很好反应材料的剪切特性;(3) 通过对LMD GH4169剪切变形破坏试样的微观分析发现,随着应变率升高,断口韧窝尺寸和深度减小,韧性降低,在更小的变形量下容易剪切失效。初始微观缺陷容易导致材料的动态剪切破坏。
  • 图  1  三种试样形式

    Figure  1.  Three sample forms

    图  2  加载脉冲与模型装配图

    Figure  2.  Loading pulse and model assembly drawing

    图  3  剪切区应力分量-时间曲线

    Figure  3.  Stress component-time curves of shear zone

    图  4  数值模拟波形图

    Figure  4.  Numerical simulation waves

    图  5  剪切区应力分量随宽度的变化曲线

    Figure  5.  Curves of shear zone stress component vary with width

    图  6  实验材料

    Figure  6.  Experimental material

    图  7  加约束受力分析

    Figure  7.  Constrained stress analysis

    图  8  未加约束受力分析

    Figure  8.  Unconstrained stress analysis

    图  9  实验装置示意图

    Figure  9.  Experimental device schematic

    图  10  LMD GH4169在不同应变率下的剪应力-剪应变曲线

    Figure  10.  Shear stress-shear strain curves of LMD GH4169 under different strain rates

    图  11  剪切强度-应变率曲线

    Figure  11.  Shear strength-strain rate curve

    图  12  动态剪切与压缩实验等效应力应变曲线对比

    Figure  12.  Equivalent stress-strain curves comparison for dynamic shear and compression testing

    图  13  不同工艺GH4169动态剪切力学行为比较

    Figure  13.  Comparison of dynamic shear mechanical behaviors of different processes GH4169

    图  14  应变率0.1 s−1x向试样断口形貌

    Figure  14.  SEM observations in fracture specimens at the strain rate 0.1 s−1 along x-direction

    图  15  应变率10 000 s−1x向试样断口形貌

    Figure  15.  SEM observations in fracture specimens at the strain rate 10 000 s−1 along x-direction

    图  16  应变率30 000 s−1x向试样断口形貌

    Figure  16.  SEM observations in fracture specimens at the strain rate 30 000 s−1 along x-direction

    表  1  三种试样尺寸

    Table  1.   Sizes of three specimens

    试样形式剪切区宽度Ls/mm剪切区高度h/mm剪切区厚度t/mm
    帽型试样[9]0/0.1/0.22
    片式帽型试样[11]0/0.2/0.523
    双剪切试样[12]0.2/0.5/120.5
    下载: 导出CSV

    表  2  材料弹性参数

    Table  2.   Material elasticity parameters

    材料E/GPaρ/(kg·m−3)μ
    18Ni钢19078000.3
    GH416921082400.3
     注:E为弹性模量,ρ为密度,μ为泊松比。
    下载: 导出CSV

    表  3  GH4169的J-C本构模型参数[13]

    Table  3.   J-C constitutive model parameters of GH4169[13]

    A/MPaB/MPanCm
    12416220.65220.01341.3
    下载: 导出CSV

    表  4  LMD GH4169工艺参数

    Table  4.   LMD GH4169 process parameters

    激光功率/W扫描速度/(mm·s−1)送粉速度/(g·min−1)载粉气流/(L·min−1)光斑直径/mm搭接率/%抬升高度/mm
    220010973500.3
    下载: 导出CSV
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出版历程
  • 收稿日期:  2019-06-24
  • 修回日期:  2020-01-03
  • 刊出日期:  2020-08-01

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