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非稳态载荷对二维轮轨纯滚动接触应力和变形的影响

温泽峰 金学松 肖新标

温泽峰, 金学松, 肖新标. 非稳态载荷对二维轮轨纯滚动接触应力和变形的影响[J]. 交通运输工程学报, 2006, 6(4): 14-19.
引用本文: 温泽峰, 金学松, 肖新标. 非稳态载荷对二维轮轨纯滚动接触应力和变形的影响[J]. 交通运输工程学报, 2006, 6(4): 14-19.
WEN Ze-feng, JIN Xue-song, XIAO Xin-biao. Influence of non-steady state loading on two-dimensional wheel-rail pure rolling contact stresses and deformation[J]. Journal of Traffic and Transportation Engineering, 2006, 6(4): 14-19.
Citation: WEN Ze-feng, JIN Xue-song, XIAO Xin-biao. Influence of non-steady state loading on two-dimensional wheel-rail pure rolling contact stresses and deformation[J]. Journal of Traffic and Transportation Engineering, 2006, 6(4): 14-19.

非稳态载荷对二维轮轨纯滚动接触应力和变形的影响

基金项目: 

国家自然科学基金项目 50575188

国家自然科学基金项目 50375129

西南交通大学基础科学研究基金项目 2005B18

详细信息
    作者简介:

    温泽峰(1976-), 男, 广西上林人, 西南交通大学副研究员, 工学博士, 从事轮轨滚动接触力学研究

  • 中图分类号: U211.5

Influence of non-steady state loading on two-dimensional wheel-rail pure rolling contact stresses and deformation

More Information
  • 摘要: 为了揭示轮轨波状表面与非稳态载荷的内在联系, 利用有限元法, 建立了二维弹塑性轮轨纯滚动接触计算模型, 分析法向接触载荷波动值对钢轨残余应力、应变和变形的影响。模型中材料本构采用考虑棘轮效应的Jiang-Sehitoglu模型, 非稳态仅考虑法向接触载荷的简谐变化, 用弹塑性无限半空间表面上重复移动赫兹法向压力分布模拟反复纯滚动接触过程。发现非稳态法向接触载荷作用下产生同样波长的波状接触表面; 随滚动次数的增加, 残余应力增大, 但很快趋于稳定, 而残余应变也增大, 但增大速率衰减; 载荷波动值越大, 波谷和波峰处的纵向残余应力越大, 波谷处的轴向残余应力、残余剪应变和表面纵向位移越大, 而波峰处的轴向残余应力、残余剪应变和表面纵向位移越小, 波深越大。

     

  • 图  1  线滚动接触

    Figure  1.  Linear rolling contact

    图  2  有限元模型

    Figure  2.  Finite element model

    图  3  γxzr等值线分布

    Figure  3.  Isoline distributing of γxzr

    图  4  τxz-γxz曲线

    Figure  4.  τxz-γxz curves

    图  5  残余应力

    Figure  5.  Residual stresses

    图  6  残余应力与滚过次数曲线

    Figure  6.  Curves of residual stresses and rolling pass times

    图  7  γxzr曲线

    Figure  7.  γxzrcurves

    图  8  γxzr-N曲线

    Figure  8.  γxzr-N curves

    图  9  C0对残余应力和残余剪应变的影响

    Figure  9.  Influences of C0 onresidual stresses and residual shear strains

    图  10  0 δxr-N曲线

    Figure  10.  δxr-N curves

    图  11  1 δzr-N曲线

    Figure  11.  δzr-N curves

    图  12  Δδrz-N曲线

    Figure  12.  Δδrz-N curves

    图  13  δrz/dN-N曲线

    Figure  13.  δrz/dN-N curves

    表  1  塑性模型

    Table  1.   Plasticity model

    屈服准则 f= (S-α) · (S-α) -2k2=0 S为偏应力张量; α为背应力张量; k为剪切屈服强度
    流动准则 dεp=1hdSnn n为屈服面的法线方向; h为塑性模量; εp为塑性应变张量; 〈〉为Macauley括号, 即〈x〉=0.5 (x+x)
    硬化准则 α=i=1Μαi dαi=ciri[n-(αiri)χi+1αiαi]dp(i=1,2,,Μ) αi为第i个背应力张量分量; M为背应力张量分量总数; dp为等效塑性应变增量; ciriχi为材料常数
    下载: 导出CSV

    表  2  材料常数

    Table  2.   Material constants

    E=210 GPa, υ=0.3, k=100 MPa, M=5
    c1=1632.3, c2=493.0, c3=149.0, c4=45.0, c5=13.6
    r1=120.5 MPa, r2=76.3 MPa, r3=89.6 MPa, r4=100.4 MPa, r5=152.5 MPa
    χ1 =χ2 =χ3 =χ4=χ5=5
    下载: 导出CSV
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出版历程
  • 收稿日期:  2006-04-17
  • 刊出日期:  2006-12-25

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