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Advanced Welding Processes: Technologies and Process Control

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138<br />

<strong>Advanced</strong> welding processes<br />

8.2 Plasma keyhole welding<br />

The principles of plasma welding have been described in Chapter 6. The<br />

same transferred arc operating system is used for plasma keyhole welding,<br />

but the plasma gas flow <strong>and</strong> current are usually increased <strong>and</strong> the orifice size<br />

may be reduced. The exact current where the keyhole mode is initiated will<br />

depend on the torch geometry <strong>and</strong> the joint material <strong>and</strong> thickness, but<br />

currents of over 200 A <strong>and</strong> plasma gas flows of 3 to 4 1 min –1 are typical with<br />

a 2 to 3 mm diameter constricting orifice. Under these conditions high arc<br />

pressures are generated by electromagnetic constriction.<br />

The thermal efficiency of the process is high <strong>and</strong> it has been estimated<br />

that the heat transferred to the workpiece from a 10 kW plasma arc can be as<br />

high as 66% of the total process power [145].<br />

8.2.1 <strong>Control</strong> of plasma keyhole welding<br />

The parametric relationships for plasma keyhole welding are complicated by<br />

variations due to torch geometry <strong>and</strong> it is likely that parameters developed<br />

using a specific torch will not be transferable to a torch of a different design.<br />

The control variables may be divided, as shown in Table 8.1, into those<br />

normally used to match the conditions to the application, the primary controls,<br />

<strong>and</strong> those normally chosen <strong>and</strong> fixed before adjustment of the process, the<br />

secondary factors.<br />

The influence of the main control parameters on process performance<br />

may be summarized as follows.<br />

Mean welding current<br />

The arc force produced by magnetic constriction is proportional to the square<br />

of the mean current. With high currents, very high arc forces are generated<br />

<strong>and</strong> undercut or humping may occur (see Chapter 6). The current must,<br />

however, be controlled in conjunction with welding speed to produce the<br />

required bead profile.<br />

Table 8.1 Plasma keyhole control factors<br />

Primary Secondary<br />

Current Orifice shape/type<br />

Travel speed Orifice diameter<br />

Plasma gas flow Electrode vertex angle<br />

Electrode set back<br />

Shielding <strong>and</strong> plasma gas type<br />

Torch st<strong>and</strong> off

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