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Advanced Welding Processes: Technologies and Process Control

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High-energy density processes 159<br />

pressure at 3.5 ¥ 1010 W m –2 has been calculated as 10 7 N m –2 . Although it<br />

is not possible to equate these forces directly, the surface tension force for a<br />

0.5 mm diameter keyhole would be only just over 7 ¥ 10 3 N m –2 .<br />

Under these circumstances, very deep penetration keyhole welds can be<br />

made with EBW, although the general form of the speed/penetration curve<br />

(Fig. 8.16) is similar to that found with both laser <strong>and</strong> keyhole plasma welds.<br />

8.4.3 <strong>Control</strong> of EBW<br />

Primary <strong>and</strong> secondary control variables may be identified for electron beam<br />

welding as shown in Table 8.3. However, although the inter-relationship<br />

between beam power–travel speed <strong>and</strong> thickness is clearly established, the<br />

welding performance may be changed significantly by means of the secondary<br />

controls. In particular, beam focus <strong>and</strong> deflection may be used to control the<br />

depth-to-width ratio of the welds <strong>and</strong> intentional defocusing may be used to<br />

enable cosmetic finishing runs to be made after completion of the penetration<br />

weld.<br />

8.4.4 Applications<br />

The EBW process has been used for joining a wide range of materials including<br />

alloy steels, nickel alloys, titanium, copper <strong>and</strong> dissimilar metals in thicknesses<br />

Travel speed (m min –1 )<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

60 kW Carbon steel<br />

100 kW Aluminium<br />

0<br />

0 100 200 300 400 500 600 700<br />

Thickness (mm)<br />

8.16 Thickness versus travel speed for electron beam welding of<br />

various materials.<br />

Table 8.3 <strong>Control</strong> parameters for EBW<br />

Primary variables Secondary variables<br />

Filament current Beam focus<br />

Voltage Beam deflection<br />

Travel speed Power supply<br />

Vacuum

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