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基于离散单元法的铁路板结道床动力特性分析

崔旭浩,肖宏

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崔旭浩, 肖宏. 基于离散单元法的铁路板结道床动力特性分析[J]. 江南娱乐网页版入口官网下载安装学报, 2021, 56(6): 1197-1204. doi: 10.3969/j.issn.0258-2724.20200113
引用本文: 崔旭浩, 肖宏. 基于离散单元法的铁路板结道床动力特性分析[J]. 江南娱乐网页版入口官网下载安装学报, 2021, 56(6): 1197-1204.doi:10.3969/j.issn.0258-2724.20200113
CUI Xuhao, XIAO Hong. Dynamic Characteristics Analysis of Hardening Railway Ballast Bed Based on Discrete Element Method[J]. Journal of Southwest Jiaotong University, 2021, 56(6): 1197-1204. doi: 10.3969/j.issn.0258-2724.20200113
Citation: CUI Xuhao, XIAO Hong. Dynamic Characteristics Analysis of Hardening Railway Ballast Bed Based on Discrete Element Method[J].Journal of Southwest Jiaotong University, 2021, 56(6): 1197-1204.doi:10.3969/j.issn.0258-2724.20200113

基于离散单元法的铁路板结道床动力特性分析

doi:10.3969/j.issn.0258-2724.20200113
基金项目:中央高校基本科研业务费专项资金(2019YJS112)
详细信息
    作者简介:

    崔旭浩(1994—),男,博士研究生,研究方向为轨道工程,E-mail:xhcui01@126.com

    通讯作者:

    肖宏(1978—),男,教授,研究方向为轨道工程与工务管理, E-mail:xiaoh@bjtu.edu.cn

  • 中图分类号:U213.7

Dynamic Characteristics Analysis of Hardening Railway Ballast Bed Based on Discrete Element Method

  • 摘要:

    为研究铁路有砟道床板结对其自身动力特性的影响,利用离散单元法并考虑道砟颗粒的真实外形建立了板结道床的仿真分析模型,分析了脏污板结及板结程度对有砟道床动态响应的影响,并探讨了板结引起道床弹性损失、刚度变大的细观机理. 研究结果表明:道床板结会增大道床中道砟颗粒的振动水平,并且板结越严重影响越明显,板结可将道砟颗粒的振动加速度增大20%~30%;板结会加强列车荷载对道床的冲击作用,增大道砟颗粒之间的接触力容易引起道砟颗粒破碎劣化;板结会放大不同位置处道床工作性能的差异,增大道床刚度的不均匀性;道砟颗粒之间的脏污板结材质会抑制道砟颗粒的相对移动,可将道砟颗粒的滑动分数降低至正常的50%左右,减小列车荷载作用下道床整体的宏观变形,从而呈现出刚度增大的特性.

  • 图 1道砟颗粒建模

    Figure 1.Ballast particle modeling

    图 2有砟轨道离散元整体模型(单位:m)

    Figure 2.Discrete element model of ballast bed (unit:m)

    图 3板结道床局部模型

    Figure 3.Local model of hardening ballast bed

    图 4道床振动加速度

    Figure 4.Ballast bed vibration acceleration

    图 5道砟颗粒振动加速度矢量图

    Figure 5.Vector diagram of ballast particle vibration acceleration

    图 65号轨枕下方道砟颗粒振动加速度时程曲线

    Figure 6.Time history curves of ballast particle vibration acceleration under No. 5 sleeper

    图 7道砟颗粒振动加速度幅值

    Figure 7.Peak vibration acceleration of ballast particles

    图 8道砟颗粒接触力均值时程曲线

    Figure 8.Time history curves of mean contact force of ballast particles

    图 9道砟颗粒平均接触力峰值

    Figure 9.Peak of average contact force of ballast particles

    图 10道砟颗粒滑动分数

    Figure 10.Slip fraction of ballast particles

    图 11单一时步中道砟颗粒切向滑动位移

    Figure 11.Sliding displacement of ballast particles in a single time step

    图 12道砟颗粒运动示意

    Figure 12.Schematic diagram of the ballast particles movements

    表 1计算工况

    Table 1.Calculation conditions

    工况编号 道床 板结程度/% 脏污颗粒数量/粒
    1 洁净道床 0 0
    2 板结道床 25 17605
    3 板结道床 50 35213
    4 板结道床 100 70427
    下载: 导出CSV

    表 2离散元模型计算参数

    Table 2.Parameters of DE model

    参数 取值
    道砟颗粒法向刚度/(N•m−1 5.0 × 108
    道砟颗粒切向刚度/(N•m−1 5.0 × 108
    道砟颗粒摩擦系数 0.55
    道砟颗粒密度/(kg•m−3 2 500
    脏污颗粒密度/(kg•m−3 2500
    钢轨密度/(kg•m−3 1029.5
    轨枕密度/(kg•m−3 3025.8
    脏污颗粒黏结强度/MPa 0.5
    黏结半径比例系数 1.0
    下载: 导出CSV
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出版历程
  • 收稿日期:2020-03-24
  • 修回日期:2020-06-03
  • 网络出版日期:2020-07-07
  • 刊出日期:2020-07-07

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