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Advanced Welding Processes: Technologies and Process Control

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Water<br />

cooling<br />

6.7 Dual-shielded GTAW.<br />

<strong>Advanced</strong> gas tungsten arc welding 85<br />

steel, carbon steel <strong>and</strong> non-ferrous materials including aluminium. At low<br />

currents (20 to 50 A), the process gives improved arc stability <strong>and</strong> the mean<br />

current required is 30 to 40% lower than that required for conventional<br />

GTAW. On thicknesses up to 3 mm in aluminium alloys <strong>and</strong> 4 mm in steel,<br />

square butt preparations may be used <strong>and</strong> welding speed increases of up to<br />

20% compared with conventional GTAW are possible. If the current is increased<br />

to 335 A <strong>and</strong> above keyhole (see Chapter 8), welding is possible on plate<br />

thicknesses from 4 to 6 mm.<br />

Physical constriction of the GTAW arc by a water-cooled copper nozzle,<br />

as shown in Fig. 6.8, will produce an even higher current density <strong>and</strong> arc<br />

core temperature for a given mean current. When this technique is used, the<br />

process is referred to as the plasma process [97] (see also Chapter 1).<br />

6.3.7 Plasma welding<br />

In plasma welding, the arc is formed between the tip of a non-consumable<br />

electrode <strong>and</strong> either the workpiece or the constricting nozzle. Again, it is<br />

possible to select different shielding <strong>and</strong> plasma-forming gases, although<br />

argon is commonly used as the central plasma gas whilst argon or argon/<br />

hydrogen (where appropriate) may be used for the outer shielding medium.<br />

Two basic operating modes are possible for plasma welding. These are:<br />

∑ the transferred arc mode;<br />

∑ the non-transferred arc mode.<br />

Concentric<br />

shield gas<br />

Outer shield<br />

gas

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