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Fachzeitschrift_OeGS_03_04_2019

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Mechanical properties and microstructural study of homogeneous<br />

and heterogeneous laser welds in α, β, and<br />

α + β titanium alloys<br />

• L. Weiss, J. Zollinger, P. Sallamand, E. Cicala, A. Mathieu,<br />

E. Fleury<br />

Heterogeneous welding has been investigated for three different<br />

couples of titanium alloys: α/α + β, α/β, and α + β/β.<br />

Plates of 100 × 60 mm and 1.6 or 1.8 mm thick were welded<br />

with a Yb:YAG laser. Tensile tests show that the resistance<br />

of the heterogeneous welded specimens was generally<br />

controlled by those of the weakest material except for<br />

the α + β/β where the ultimate tensile strength was approximately<br />

equal to the average value of both materials. In<br />

every case, the elongation of the welded sample was found<br />

to be smaller than that of the base metals. The rupture generally<br />

took place outside the weld metal and was found to<br />

be most of the time located in the alloy having the lowest<br />

mechanical properties. Nevertheless, a few large-size porosities<br />

detected by tomography in the α + β/β couple could<br />

explain why rupture for these samples occurred in the weld<br />

bead. For each couple, the porosities were situated at the<br />

board between the heat-affected zone and the molten<br />

zone. EBSD maps and EDX enabled the observation of different<br />

microstructures, which could be correlated to the<br />

heterogeneous composition and diffusion into the melted<br />

bath. When the stable microstructure of one of the couple<br />

alloys is the β phase, the molten zone of the bead consists<br />

of an alternative disposition of thin layers made of large<br />

equiaxed β grains and nano-martensite α′. That is explained<br />

by the weak diffusion of the alloying elements.<br />

Liquid interlayer formation during friction stir spot welding<br />

of aluminum/copper<br />

• A. Regensburg, F. Petzoldt, T. Benss. J.P. Bergmann<br />

The fabrication of dissimilar aluminum/copper joints for<br />

electrical application raises the challenges for conventional<br />

joining technologies. Within the solid-state processes, friction<br />

stir welding (FSW) provides numerous advantages to<br />

realize different joint configurations, especially by minimizing<br />

the heat input and hence the formation of brittle intermetallic<br />

phases. However, the joints also have to provide a<br />

high contact interface with firm bonding in order to provide<br />

a minimal contact resistance. Therefore, joints of 1 mm EN-<br />

CW0<strong>04</strong>A and EN AW1050A with a controlled melt layer formation<br />

were produced by friction stir spot welding (FSSW).<br />

By using a pinless tool and the positioning of copper as the<br />

upper joining partner, local melt formation at the interface<br />

with a eutectic composition was promoted without significant<br />

intermixing, resulting in wetting of the aluminum and<br />

a contact area increase. The rotational speed was varied<br />

between 1800–2400 rpm, in which range samples with up<br />

to 300-μm-thick melt layers were produced. The wetting<br />

effect at the interface shows a positive influence on the<br />

shear strength with ductile failure behavior even at high<br />

layer thickness. The microstructural composition at the interface<br />

showed a eutectic composition for small layer thickness<br />

and an inhomogeneous composition with hypo- and<br />

hypereutectic solidification structures for higher thickness<br />

values. However, the formation of intermetallic compounds<br />

other than CuAl2 was mostly inhibited by the short process<br />

times and high cooling rate.<br />

Welding design methodology for optimization of phase<br />

balance in duplex stainless steels during autogenous<br />

arc welding under Ar–N 2<br />

atmosphere<br />

• A. Rokanopoulou, P. Skarvelis, G. D. Papadimitriou<br />

This study deals with the selection of appropriate welding<br />

parameters during autogenous arc welding of duplex stainless<br />

steels in order to achieve an optimum phase balance of<br />

austenite and ferrite in the as-welded microstructure. Specimens<br />

of duplex stainless steel 2205 with dimensions<br />

(40 × 40 × 10) mm 3 were welded using autogenous arc welding<br />

under 95% Ar + 5% vol. N 2<br />

atmosphere. The weld pool<br />

temperature was measured by non-contact infrared temperature<br />

measurement, the weld bead dimensions were determined<br />

using scanning electron micrographs, and the final<br />

nitrogen concentration was evaluated by optical emission<br />

spectroscopy. The kinetics of nitrogen absorption and desorption<br />

in molten duplex stainless steel was discussed and<br />

all the relevant variables were presented. The effect of welding<br />

current and speed on the final nitrogen concentration<br />

was also discussed. Finally, based on this analysis, a method<br />

was set up which can be used to optimize the phase balance<br />

by using predictive methods of the Ferrite Number, such as<br />

the Welding Research Council (WRC)-92 diagram.<br />

Numerical investigations on the thermal efficiency in<br />

laser-assisted plasma arc welding<br />

• S. Jäckel, M. Trautmann, M. Hertel, U. Füssel, D. Hipp,<br />

A. Mahrle, E. Beyer<br />

Numerical investigations on the thermal efficiency in laserassisted<br />

plasma arc welding (LAPAW) have been carried out<br />

by the combination of a magneto-hydrodynamic (MHD) arc<br />

model and a smoothed-particle-hydrodynamics (SPH) model<br />

of the weld pool. The comparison of the calculated weld<br />

seam cross-sections gained from numerical simulation as<br />

well as experimental examinations shows a good agreement.<br />

By the use of the weld pool model, the sensitivity of<br />

different influencing variables was investigated. The analysis<br />

clearly reveals the major influence of the central heat flux<br />

density on the penetration profile and on the thermal efficiency<br />

of the process. The higher the heat flux of the laser<br />

beam and the higher the constriction of the heat flux profile<br />

of the arc, the higher the thermal efficiency of the process.<br />

SCHWEISS- und PRÜFTECHNIK <strong>03</strong>-<strong>04</strong>/<strong>2019</strong> 67

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