论文

等离子弧焊接小孔形状和穿孔过程的数值分析

  • 武传松 ,
  • 霍玉双 ,
  • 陈茂爱
展开
  • 1. 山东大学材料液固结构演变与加工教育部重点实验室, 济南 250061
    2. 山东建筑大学材料科学与工程学院, 济南 250101
霍玉双, 女, 1973年生, 博士

收稿日期: 2011-01-07

  修回日期: 2011-05-11

  网络出版日期: 2011-06-11

基金资助

国家自然科学基金重点资助项目50936003

NUMERICAL SIMULATION OF KEYHOLE SHAPE AND TRANSFORMATION FROM PARTIAL TO OPEN STATES IN PLASMA ARC WELDING

  • WU Zhuan-Song ,
  • SUO Yu-Shuang ,
  • CHEN Mao-Ai
Expand
  • 1. Key Lab for Solid–Liquid Structure Evolution and Materials Processing (Ministry of Education), Shandong University, Jinan 250061
    2. School of Materials Science and Engineering, Shandong Jianzhu University, Jinan 250101

Received date: 2011-01-07

  Revised date: 2011-05-11

  Online published: 2011-06-11

Supported by

Supported by Key Project of National Natural Science Foundation of China (No.50936003)

摘要

根据小孔壁面上的力学平衡条件, 建立了穿孔等离子弧焊(PAW)的小孔模型. 利用该模型, 对6 mm厚不锈钢板PAW准稳态小孔的形成过程进行了数值计算, 得到了不同工艺参数下准稳态小孔的形状和尺寸. 根据达到准稳态时小孔壁面的受力状态, 对PAW过程中小孔从盲孔到穿孔的转变机制进行了探讨, 分析计算了小孔壁面上各区域的作用力大小. 随着焊接电流的升高, 小孔的深度呈现非线性增大; 存在一个小孔在熔池内由盲孔突然转变为穿孔状态的焊接电流临界值; 等离子弧力在小孔底部急剧集中是导致小孔深度突变的主要原因. 通过穿孔PAW焊接工艺实验, 对数值计算结果进行了实验验证.

本文引用格式

武传松 , 霍玉双 , 陈茂爱 . 等离子弧焊接小孔形状和穿孔过程的数值分析[J]. 金属学报, 2011 , 47(6) : 706 -712 . DOI: 10.3724/SP.J.1037.2011.00012

Abstract

It is of great significance to develop a mathematical model of keyhole shape and dimension in order to widen the process parameter window and improve the process stability in keyhole plasma arc welding (PAW). In this study, a keyhole model was developed according to the force–balance conditions on the keyhole wall. The establishing process of quasi–steady state keyhole was numerically simulated for stainless steel plates of 6 mm thickness, and the keyhole shapes and dimensions were obtained under different welding process parameters. The transformation mechanism of the keyhole from blind (partial) to open (complete) states in PAW process was analyzed based on the calculated action forces on the keyhole wall. The values of action forces at different locations on the keyhole wall were calculated. With increasing of welding current, the keyhole depth rised in a nonlinear way. There existed a critical value of welding current, i.e., if welding current was a little bit hgher than this value, the keyhole inside the weld pool would suddenly transform from partial state (blind keyhole) ino complete state (open keyhole). The fast centralization of the plasma arc force at the keyhole bottom region resulted in the sudden transformation from a partial keyhole to an open keyhole. The keyhole PAW experiments were conducted to validate the numerical analyss results.

参考文献

[1] Lucas W. In: Japan Welding Society ed., Proc 8th Int Welding Symposium, Osaka, Japan: Japan Welding Society, 2008: 189

[2] Zhang Y M, Zhang S B. Weld J, 1999; 75: 53s

[3] Wu C S, Jia C B, Chen M A. Weld J, 2010; 89: 225s

[4] Dong C L, Wu L, Shao Y C. China Mech Eng, 2000; 11: 577

(董春林, 吴林, 邵亦陈. 中国机械工程, 2000; 11: 577)

[5] Keanini R G, Rubinsky B. Int J Heat Mass Transfer, 1993; 36: 3283

[6] Fan H G, Kovacevic R. J Phys, 1999; 32D: 2902

[7] Li L, Hu S S. J Tianjin Univ, 2007; 40: 260

(李力, 胡绳荪. 天津大学学报, 2007; 40: 260)

[8] Metcalfe J C, Quigley M B C. Weld J, 1975; 54: 99s

[9] Wu C S, Hu Q X, Gao J Q. Comp Mater Sci, 2009; 46: 167

[10] Hu Q X, Wu C S, Zhang Y M. China Weld, 2007; 16: 55

[11] Huo Y S, Wu C S. China Weld, 2009; 18: 12

[12] Nehad A K. Int Comm Heat Mass Transfer, 1995; 22: 779

[13] Wang X J, Wu C S, Chen M A. Acta Metall Sin, 2010; 46: 984

(王小杰, 武传松, 陈茂爱. 金属学报, 2010; 46: 984)

[14] Toit M D, Pistorius P C. Weld J, 2007; 86: 222s

[15] Sahoo P, DebRoy T, McNallan M J. Metal Trans, 1988; 19B: 483
文章导航

/