空心钨极与实心钨极电弧物理特性分析

Analysis of arc physical characteristics of hollow tungsten electrode and solid tungsten electrode

  • 摘要:
    目的  旨在探究空心钨极与实心钨极2种钨极特征下的电弧物理场分布特征。
    方法 利用COMSOL6.0数值模拟软件分别建立了实心钨极与空心钨极电弧的磁流体模型。系统分析了焊接电流从100 A提高至500 A时,实心钨极稳态电弧与空心钨极稳态电弧的电弧温度、压力、流速及电势差异,指出了钨极特征对电弧不同物理量的影响规律及形成机制。
    结果 焊接电流从100 A增加到500 A时,实心钨极电弧与空心钨极电弧的最大物理量差值随着焊接电流的增加呈逐渐增加趋势;当焊接电流增加至500 A时,空心钨极最高电弧温度和最大电弧压力只有实心钨极的64.5%和14.2%。
    结论 相较于实心钨极,焊接电流增加时空心钨极电弧电势、温度、流速和电弧压力均对焊接电流变化不敏感;空心钨极末端环状电子发射特征是空心钨极电弧物理场在空间分布较为均匀的根本原因。

     

    Abstract: Objective The aim was to explore distribution characteristics of arc physical field under two characteristics of hollow tungsten electrode and solid tungsten electrode. Methods MHD models of solid tungsten electrode and hollow tungsten electrode arc were established by COMSOL6.0 numerical simulation software. Differences of arc temperature, pressure, flow rate and potential between solid tungsten electrode steady-state arc and hollow tungsten electrode steady-state arc were systematically analyzed when welding current increased from 100 A to 500 A, and influence law and formation mechanism of tungsten electrode characteristics on different physical quantities of arc were pointed out. Results When welding current increased from 100 A to 500 A, the maximum physical quantity difference between solid tungsten electrode arc and hollow tungsten electrode arc increased gradually with the increase of welding current. When welding current increased to 500 A, the maximum arc temperature and pressure of hollow tungsten electrode were only 64.5% and 14.2% those of solid tungsten electrode. Conclusion Compared with solid tungsten electrode, arc potential, temperature, flow rate and arc pressure of hollow tungsten electrode were not sensitive to the change of welding current when welding current increased. Characteristic of annular electron emission at the end of hollow tungsten electrode was the fundamental reason for uniform spatial distribution of arc physical field of hollow tungsten electrode.

     

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