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LIBRARY ı6ıul 0) - Cranfield University

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data. Measurements of resistance between the contact tip and the workpiece showed<br />

that in dip mode of metal transfer the resistance calculated during the short circuiting<br />

phase has a strong correlation with the stand-off. This was also observed by Philpott<br />

[ref. 21], who used the term dip resistance to designate such resistance. Based on this<br />

observation, a method was devised to calculate the dip resistance using the<br />

windowing technique developed by Chawla [ref. 161] together with the standard<br />

statistical features extracted from each window of data (see section 2.6.3).<br />

In the dip mode of metal transfer, a short circuiting phase is characterised by<br />

the extinction of the welding arc which occurs when the electrode wire touches the<br />

weld pool and transfers the molten droplet to the pool. During this time, the wire<br />

forms a continuous bridge between the contact-tip and the workpiece. The short<br />

circuiting phase can be detected by analysing the welding voltage transient waveform<br />

and identifying the periods when the voltage falls steeply to a value close to zero (see<br />

Figure 6.10). In this work, in order to make sure that the measured resistance would<br />

correspond to a real short circuit, only the voltage samples with magnitude equal to or<br />

smaller than the background voltage were considered for calculation purposes. The<br />

dip resistance for a window of data was obtained as the average of all the resistances<br />

calculated for voltage samples complying with VS Vbk. Equations (6.7) and (6.8)<br />

show the method explicitly.<br />

where<br />

Vk<br />

DipA 1'ý<br />

k<br />

[Vk E[], 2,..., N l; Vk _

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