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June 2015

AFRICAN FUSION

25

arc [9]. In the low-current case (170 A), globular transfer occurs.

As can be seen in Figure 2, the temperature distribution of the

MIG arc changes with the detachment of a metal droplet from

the wire tip. In contrast at the higher current (250 A), spray

transfer occurs. The liquid metal at the wire tip is elongated

toward the pool like sharpened pencil. The arc plasma shape

appears not to change, and its temperature field is less varied

bymoltendropbehaviour. Fluidity, surface tension and viscos-

ity of the liquid metal govern the shape and/or size of metal

drop at the wire tip. As is well known, the electromagnetic

force depends significantly on the current path flowing in the

liquid metal. This means that the shape of the arc plasma

touchedwith liquidmetal plays an important role on dynamic

behaviour of metal transfer.

In other words, the metal transfer mode is varied by

physical properties such as thermal conductivity and electri-

cal conductivity of the arc plasma. Accordingly, the composi-

tion of the shielding gas is one of the important variables for

controlling metal transfer. With this established, the change

in a gas shielded metal arc across a metal transfer cycle can

be predicted with aid of numerical simulation.

Concluding remarks

The essential components of the gas shielded arcwelding pro-

cess include theweldingmachine, electrodewire and shielding

Figure 2: Changes of the arc-plasma temperature field and drop shape for the open arc, argon-shielded GMAW process. (a): Welding current

of 170 A. (b): Welding current of 250 A.

(b) 250 A.

(a) 170 A.

gas. In addition to universities and national institutes, welding

machine makers, consumable makers and gas suppliers have

been putting effort into the research and development of de-

vices, consumables and newGMAWprocesses in collaboration

with various fabricators. Some of these developments have

been carried out based on visual observationwith recent high

performance digital cameras, along with knowledge derived

from numerical results of theoretical model.

References

1 H Maruo, Y Hirata, Y Noda: Quarterly Journal of the Japan

Welding Society, Vol.2 (1984) No.1.

2 H Maruo, Y Hirata: Quarterly Journal of the Japan Welding

Society, Vol.3 (1985) No.2.

3 H Maruo, Y Hirata: Doc.80-436 of Technical Commission on

Welding Arc Physics in Japan Welding Society(1980).

4 A Okada, H Yamamoto, W Nishikawa: Doc.80-437 of Techni-

cal Commission of Welding Arc Physics of Japan Welding

Society(1980).

5 T Ueguri, et al: Doc.80-446 of Technical Commission of Weld-

ing Arc Physics of Japan Welding Society(1980).

6 K Hashimoto, Y Hirata: IIW Doc. 212-1300-13(2013)

7 G Huismann: IIW Doc.212-952-99(1999).

8 K Himmelbauer: IIW Doc.XII-1875-05(2005).

9 Y Ogino, Y Hirata: IIW Doc.212-1324-14(2014).

GMAW: current progress