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切削式吸能的惯性效应

刘国伟 夏茜 王千叶 董茹玲

刘国伟, 夏茜, 王千叶, 董茹玲. 切削式吸能的惯性效应[J]. 交通运输工程学报, 2015, 15(3): 62-70. doi: 10.19818/j.cnki.1671-1637.2015.03.008
引用本文: 刘国伟, 夏茜, 王千叶, 董茹玲. 切削式吸能的惯性效应[J]. 交通运输工程学报, 2015, 15(3): 62-70. doi: 10.19818/j.cnki.1671-1637.2015.03.008
LIU Guo-wei, XIA Qian, WANG Qian-ye, DONG Ru-ling. Inertia effects of cutting energy absorption[J]. Journal of Traffic and Transportation Engineering, 2015, 15(3): 62-70. doi: 10.19818/j.cnki.1671-1637.2015.03.008
Citation: LIU Guo-wei, XIA Qian, WANG Qian-ye, DONG Ru-ling. Inertia effects of cutting energy absorption[J]. Journal of Traffic and Transportation Engineering, 2015, 15(3): 62-70. doi: 10.19818/j.cnki.1671-1637.2015.03.008

切削式吸能的惯性效应

doi: 10.19818/j.cnki.1671-1637.2015.03.008
基金项目: 

国家自然科学基金项目 51275532

国家自然科学基金项目 U1334208

详细信息
    作者简介:

    刘国伟(1955-), 男, 湖南长沙人, 中南大学教授, 从事轨道车辆结构研究

  • 中图分类号: U270.1

Inertia effects of cutting energy absorption

More Information
  • 摘要: 在考虑切削热影响的基础上, 采用数值模拟研究了切削式吸能过程的惯性效应, 计算了不同初始撞击条件下的稳定切削力、切削位移、最高温度、热耗散能量和热耗散能量比例。计算结果表明: 初始撞击能量为20 kJ时, 切屑生成时切削力未出现明显的初始峰值, 稳定切削力变化范围为63.0~63.8 kN, 变化规律相同, 变化趋势一致; 撞击质量为200 kg, 撞击速度变化范围为3~10 m·s-1时, 稳定切削力变化范围为63.0~64.4 kN; 撞击速度为10 m·s-1, 撞击质量由0.4 t增加至3.2 t时, 热耗散能量由4.12 kJ增加到36.64 kJ, 热耗散能量随撞击质量的增大而增大, 最高温度变化范围为586℃602℃, 热耗散能量比例变化范围为20.6%~23.2%, 稳定切削力的变化范围为63.0~64.1 kN。可见, 在切削深度和刀具几何参数不变的条件下, 初始撞击能量、撞击质量和撞击速度对切削力影响很小, 切削式吸能过程的惯性敏感性弱, 切削式吸能结构属于第Ⅰ类, 而且, 切削热占能量耗散比例大, 撞击速度对其影响程度大。

     

  • 图  1  切削式吸能过程

    Figure  1.  Cutting energy-absorbing process

    图  2  网格模型

    Figure  2.  Mesh model

    图  3  初始动能恒定时的稳定切削力

    Figure  3.  Stable cutting force based on constant initial kinetic energy

    图  4  初始动能恒定时的切削位移

    Figure  4.  Cutting displacement based on constant initial kinetic energy

    图  5  初始动能恒定时的最高温度

    Figure  5.  Maximum temperature based on constantinitial kinetic energy

    图  6  初始动能恒定时的热耗散能量

    Figure  6.  Thermal dissipation energy based onconstant initial kinetic energy

    图  7  初始动能恒定时的热耗散能量比例

    Figure  7.  Percentage of thermal dissipation energy based onconstant initial kinetic energy

    图  8  定初始动能时的切削力曲线

    Figure  8.  Cutting force curves based on constant initial kinetic energy

    图  9  初始动能变化时的稳定切削力

    Figure  9.  Stable cutting force based on changinginitial kinetic energy

    图  11  初始动能变化时的最高温度

    Figure  11.  Maximum temperature based on changinginitial kinetic energy

    图  10  初始动能变化时的切削位移

    Figure  10.  Cutting displacement based on changinginitial kinetic energy

    图  12  初始动能变化时的热耗散能量

    Figure  12.  Thermal dissipation energy based onchanging initial kinetic energy

    图  13  初始动能变化时的热耗散能量比例

    Figure  13.  Percentage of thermal dissipation energybased on changing initial kinetic energy

    图  14  撞击速度不变时的稳定切削力

    Figure  14.  Stable cutting force based onconstant impact speed

    图  15  撞击速度不变时的切削位移

    Figure  15.  Cutting displacement based onconstant impact speed

    图  16  撞击速度不变时的最高温度

    Figure  16.  Maximum temperature based onconstant impact speed

    图  17  撞击速度不变时的热耗散能量

    Figure  17.  Thermal dissipation energy based onconstant impact speed

    图  18  撞击速度不变时的热耗散能量比例

    Figure  18.  Percentage of thermal dissipation energybased on constant impact speed

    图  19  切削式吸能装置

    Figure  19.  Cutting energy-absorbing device

    图  20  切削力曲线

    Figure  20.  Cutting force curve

    图  21  动能曲线

    Figure  21.  Kinetic energy curve

    表  1  材料参数

    Table  1.   Material parameters

    表  2  初始动能不变时的组合工况

    Table  2.   Combined conditions based on constantinitial kinetic energy

    表  3  初始动能变化时的组合工况

    Table  3.   Combined conditions based on changinginitial kinetic energy

    表  4  撞击质量不同时的组合工况

    Table  4.   Combined conditions based on changing impact mass

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  • 收稿日期:  2014-12-23
  • 刊出日期:  2015-06-25

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