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铁路钢轨裂纹萌生的键型近场动力学预测模型

马晓川 刘林芽 冯青松 徐井芒 徐金辉 王平

马晓川, 刘林芽, 冯青松, 徐井芒, 徐金辉, 王平. 铁路钢轨裂纹萌生的键型近场动力学预测模型[J]. 交通运输工程学报, 2021, 21(3): 228-237. doi: 10.19818/j.cnki.1671-1637.2021.03.015
引用本文: 马晓川, 刘林芽, 冯青松, 徐井芒, 徐金辉, 王平. 铁路钢轨裂纹萌生的键型近场动力学预测模型[J]. 交通运输工程学报, 2021, 21(3): 228-237. doi: 10.19818/j.cnki.1671-1637.2021.03.015
MA Xiao-chuan, LIU Lin-ya, FENG Qing-song, XU Jing-mang, XU Jin-hui, WANG Ping. Prediction model of rail crack initiation using bond-based peridynamics theory[J]. Journal of Traffic and Transportation Engineering, 2021, 21(3): 228-237. doi: 10.19818/j.cnki.1671-1637.2021.03.015
Citation: MA Xiao-chuan, LIU Lin-ya, FENG Qing-song, XU Jing-mang, XU Jin-hui, WANG Ping. Prediction model of rail crack initiation using bond-based peridynamics theory[J]. Journal of Traffic and Transportation Engineering, 2021, 21(3): 228-237. doi: 10.19818/j.cnki.1671-1637.2021.03.015

铁路钢轨裂纹萌生的键型近场动力学预测模型

doi: 10.19818/j.cnki.1671-1637.2021.03.015
基金项目: 

国家重点研发计划项目 2021YFE0105600

国家自然科学基金项目 U1734207

国家自然科学基金项目 51978263

江西省自然科学基金项目 20192BAB216035

江西省教育厅科学技术研究项目 GJJ200640

详细信息
    作者简介:

    马晓川(1990-),男,山东潍坊人,华东交通大学讲师,工学博士,从事铁路轨道结构伤损研究

  • 中图分类号: U213.4

Prediction model of rail crack initiation using bond-based peridynamics theory

Funds: 

National Key Research and Development Program of China 2021YFE0105600

National Natural Science Foundation of China U1734207

National Natural Science Foundation of China 51978263

Jiangxi Natural Science Foundation of Jiangxi Province 20192BAB216035

Science and Technology Research Project of Jiangxi Education Department GJJ200640

More Information
  • 摘要: 为克服经典连续介质力学在解决不连续问题时的困难,采用近场动力学方法预测铁路钢轨的裂纹萌生,以避免数学构架在不连续处的失效问题;建立了考虑轨枕支承作用的钢轨形变分析模型,分析了模型参数合理取值及收敛性,计算了车轮滚动接触荷载下的钢轨位移;根据近场动力学损伤理论,以键伸长率为指标,分别研究了车轮全滑动、粘着-滑动及无摩擦状态对铁路钢轨裂纹萌生的影响规律。计算结果表明:近场动力学模型和经典连续介质力学模型的钢轨形变计算结果十分吻合,最大计算误差均在8%以内,验证了所建近场动力学模型的正确性;当裂纹萌生于钢轨轨头时,其启裂位置不在钢轨表面,而在钢轨表面以下约2 mm的位置,与现场观察结果一致,验证了近场动力学方法在模拟铁路钢轨疲劳裂纹萌生时的适用性;当车轮荷载位于钢轨跨中时,在车轮状态由全滑动向无摩擦转变的过程中,钢轨疲劳裂纹的萌生起点位置由轨头转移到轨底、由接触斑前端转移到接触斑中心,裂纹类型由局部滚动接触疲劳裂纹转变为整体结构疲劳裂纹,键最大伸长率由1.1×10-3降低到8.1×10-4,因此,增大切向接触应力会降低钢轨裂纹萌生寿命;当车轮荷载位于轨枕上方时,随车轮滚动状态的改变,钢轨裂纹的萌生位置始终位于轨头。

     

  • 图  1  质点的变形与相互作用

    Figure  1.  Deformation and interaction of particles

    图  2  键的损伤

    Figure  2.  Damage of bonds

    图  3  钢轨构造尺寸与质点离散状态

    Figure  3.  Rail structure sizes and discrete state of particles

    图  4  轮轨赫兹接触模型

    Figure  4.  Wheel-rail Hertz contact model

    图  5  模型尺寸对质点位移计算值的影响规律

    Figure  5.  Influence laws of model sizes on displacements of particles

    图  6  质点位移随迭代次数的变化规律

    Figure  6.  Change laws of particle displacements with iterations

    图  7  基于经典连续介质力学的钢轨形变分析模型

    Figure  7.  Rail deformation analysis model based on classical continuum mechanics

    图  8  轮轨全滑动状态下的质点位移和计算误差曲线

    Figure  8.  Particles displacements curves and calculation error curve under wheel full sliding state

    图  9  轮轨接触应力分布

    Figure  9.  Distributions of wheel-rail contact stresses

    图  10  钢轨质点的键伸长率分布

    Figure  10.  Distributions of bond stretch rates of rail particles

    图  11  荷载作用在轨枕位置时的键伸长率分布(车轮无摩擦状态)

    Figure  11.  Distribution of bond stretch rate when load is applied to the sleeper position (wheel frictionless state)

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  • 收稿日期:  2020-12-18
  • 网络出版日期:  2021-08-27
  • 刊出日期:  2021-08-27

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