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LIBRARY ı6ıul 0) - Cranfield University

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eceptor. The sensors can also be built in such a way as to perform both the emission<br />

and reception of the ultrasound, resulting in very compact designs.<br />

These kind of sensors can be used for seam tracking by either oscillating them<br />

over the joint and measuring the distances on various crossing positions, or by using<br />

two sensors mounted at 90 degrees, in the case of a fillet joint.<br />

2.6.1.3.4 Through-the-arc sensing<br />

Through-the-arc sensing involves the analysis of the welding current and<br />

voltage signals of processes such as gas metal arc welding (GMAW) and gas tungsten<br />

arc welding (GTAW) for joint tracking. The arc sensing method requires no additional<br />

equipment at the welding head and is applicable to a large number of welding tasks,<br />

particularly single pass fillet welds, heavy-section V butt and narrow-gap welding<br />

situations on steel. This section will only focus on the through-the-arc sensing<br />

techniques<br />

for gas metal arc welding.<br />

Through-the-arc sensing is based on the principle that, for a constant voltage<br />

power source and constant wire feed speed, a change in the torch-to-workpiece<br />

distance's results in a change in the welding current, which can be measured.<br />

According to equation (2.2), the melting rate (wm) depends on the joule<br />

heating in the electrode stick-out and on the heat generated by the arc. The joule<br />

heating depends on the electrode resistance, which in turn depends on the electrode<br />

cross sectional area (A, ), resistivity (r) and length (Le). Since the welding voltage and<br />

the wire feed speed are pre-set welding parameters, it is possible to calculate the<br />

distance from the contact-tip to the workpiece, SO.<br />

Since the process is in steady state, it can be assumed that the melting rate<br />

(wm) is equal to the wire feed speed (WFS) [refs. 128,129]. Hence the wire extension<br />

(Le) could be calculated by substituting wfor WFS in equation (2.2) and arranging its<br />

terms according to equation (2.8).<br />

Lý =<br />

WFS-al (2.8)<br />

ß1Z<br />

In order to 'obtain the contact tip-to-workpiece distance it is also necessary to<br />

calculate the arc length. It is possible to estimate this by using an empirical formula<br />

which establishes a relationship between the arc length (L. ), the welding current (1)<br />

and the arc voltage (Va). The empirical formula is shown in equation (2.9). It was<br />

obtained experimentally for the GTAW process but can also be applied in the case of<br />

GMAW [refs. 128,129].<br />

V. =K, La+K2+K31+ 14<br />

(2.9)<br />

18 This can be measured either by the stand-off (distance between the gas nozzle and the workpiece)<br />

or by the contact tip-to-workpiece distance. The difference between both is just a constant.<br />

33

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