Numerical analysis of fume formation mechanism in arc welding

被引:35
|
作者
Tashiro, Shinichi [1 ]
Zeniya, Tasuku [1 ]
Yamamoto, Kentaro [1 ]
Tanaka, Manabu [1 ]
Nakata, Kazuhiro [1 ]
Murphy, Anthony B. [2 ]
Yamamoto, Eri [3 ]
Yamazaki, Kei [3 ]
Suzuki, Keiichi [3 ]
机构
[1] Osaka Univ, Joining & Welding Res Inst, Osaka 5760047, Japan
[2] CSIRO, Mat Sci & Engn, Sydney, NSW 2070, Australia
[3] KOBE STEEL LTD, Kanagawa 2518551, Japan
关键词
GAS TUNGSTEN ARCS; THERMAL PLASMA; METAL VAPOR; SIZE;
D O I
10.1088/0022-3727/43/43/434012
中图分类号
O59 [应用物理学];
学科分类号
摘要
In order to clarify the fume formation mechanism in arc welding, a quantitative investigation based on the knowledge of interaction among the electrode, arc and weld pool is indispensable. A fume formation model consisting of a heterogeneous condensation model, a homogeneous nucleation model and a coagulation model has been developed and coupled with the GTA or GMA welding model. A series of processes from evaporation of metal vapour to fume formation from the metal vapour was totally investigated by employing this simulation model. The aim of this paper is to visualize the fume formation process and clarify the fume formation mechanism theoretically through a numerical analysis. Furthermore, the reliability of the simulation model was also evaluated through a comparison of the simulation result with the experimental result. As a result, it was found that the size of the secondary particles consisting of small particles with a size of several tens of nanometres reached 300 nm at maximum and the secondary particle was in a U-shaped chain form in helium GTA welding. Furthermore, it was also clarified that most part of the fume was produced in the downstream region of the arc originating from the metal vapour evaporated mainly from the droplet in argon GMA welding. The fume was constituted by particles with a size of several tens of nanometres and had similar characteristics to that of GTA welding. On the other hand, if the metal transfer becomes unstable and the metal vapour near the droplet diffuses directly towards the surroundings of the arc not getting into the plasma flow, the size of the particles reaches several hundred nanometres.
引用
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页数:12
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