高速列车车体底架厚板多层多道焊的焊接变形数值模拟分析

Numerical Simulation Analysis of Welding Deformation in Multi-layer and Multi-pass Thick-plate Welding of High-speed Train Carbody Underframe

  • 摘要:
    目的 针对高速列车车体底架中厚壁铝合金型材与板材的焊接变形问题,有必要通过数值模拟仿真,对比分析不同焊接工艺参数下的热输入量与变形差异,为优化焊接工艺、控制焊接变形提供理论依据与实践指导,以提升车体制造精度。
    方法 采用ABAQUS有限元分析软件建立了三维仿真模型。基于实际生产过程中的2层3道与3层6道焊接工艺,采用双椭球热源模型模拟MIG(熔化极惰性气体保护焊)焊接过程,通过ELM(单元生死技术)实现焊道逐道激活。模型采用六面体网格划分,焊缝区域网格尺寸为1 mm,母材区域最大网格尺寸为5 mm。数值模拟采用顺序耦合法,先进行非线性瞬态热分析,再将温度场结果作为初始条件进行热弹塑性应力场计算。
    结果及结论  2层3道工艺熔池峰值温度达1 557.0℃,显著高于3层6道工艺的879.3℃;2层3道工艺的最大焊接变形量为2.518 mm,明显大于3层6道工艺的1.146 mm,二者相差54.48%。变形差异主要由于热输入量、焊接工艺参数与结构拘束度的耦合作用。3层6道工艺通过分散热输入、增加层道拘束实现了自拘束效应,可有效抑制焊接变形。在实际工程应用中,若对尺寸精度要求严格,应优先选用3层6道工艺。

     

    Abstract:
    Objective In view of the welding deformation problems of medium- and thick-walled aluminum alloy profiles and plates in high-speed train carbody underframe, it is necessary to conduct numerical simulation analysis to comparatively study the heat input and deformation differences under different welding process parameters. This provides a theoretical basis and practical guidance for optimizing welding processes and controlling welding deformation, thereby improving the carbody manufacturing accuracy.
    Method A three-dimensional simulation model is established using ABAQUS finite element analysis software. Based on the 2-layer 3-pass and 3-layer 6-pass welding processes used in actual production, a double-ellipsoidal heat source model is adopted to simulate the MIG (metal inert gas) welding process, and the pass-by-pass weld activation is realized through the ELM (element life and death method). Hexahedral meshing is applied to the model, with a mesh size of 1 mm in the weld zone and a maximum mesh size of 5 mm in the base material. A sequentially coupled method is employed in the numerical simulation: the nonlinear transient thermal analysis is first performed, and the resulting temperature field is then used as the initial condition for thermo-elastoplastic stress field calculation.
    Result & Conclusion  For the 2-layer 3-pass process, the peak molten pool temperature reached 1 557.0 °C, significantly higher than the 879.3 °C obtained with the 3-layer 6-pass process. The maximum welding deformation of the 2-layer 3-pass process was 2.518 mm, markedly greater than 1.146 mm of the 3-layer 6-pass process, with a difference of 54.48% between them. The deformation difference is mainly attributed to the coupled effects of heat input, welding process parameters, and structural restraint. The 3-layer 6-pass process achieves a self-restraint effect by dispersing heat input and increasing inter-layer and inter-pass restraint, thereby effectively suppressing welding deformation. In practical engineering applications, when strict dimensional accuracy is required, the 3-layer 6-pass process should be preferentially adopted.

     

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