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PNNL-13501 - Pacific Northwest National Laboratory

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Figure 2. Schematic of experimental apparatus and photo of<br />

sample tested<br />

surrounding the fractures were characterized using a<br />

strain grid analysis system. This system determined the<br />

magnitude of strains that developed in the specimen in the<br />

region around the failure. Each of the originally 2.54 mm<br />

square grids characterized in the area surrounding fracture<br />

were identified as necked if the nodes near the failure<br />

showed elevated levels of local strain (necking) in the<br />

grid, or the fracture had penetrated under (undercut) the<br />

grid surface. These types of forming limit definitions<br />

must be defined and applied in the finite element analysis<br />

in order to accurately capture the material limits of<br />

formability.<br />

Welding Experiments and Modeling<br />

The experimental fixture shown in Figure 3 was<br />

constructed for use in validating the weld modeling. An<br />

automated TIG welding system was used to provide<br />

accurate control of the welding parameters (electrode<br />

speed, welding current, and voltage). Their parameters<br />

were recorded at selected intervals and used as inputs to<br />

the finite element weld models.<br />

Figure 3. Experimental fixture for use in validating the weld<br />

modeling<br />

Welds were performed in the circumferential direction on<br />

6-inch outside diameter by 0.125-inch wall thickness<br />

6061-T6 aluminum tubing. Thermocouples were located<br />

at various distances from the weld. The weld was also<br />

monitored with strain gauges located opposite the weld.<br />

Data were recorded to characterize the temperature profile<br />

and development of distortions in the tube. Data were<br />

also recorded periodically during cool down after the<br />

weld was completed. The gross distortion in the tube was<br />

measured at the end of the test for comparison with the<br />

modeling results.<br />

Finite element analyses of the experimental welds on the<br />

aluminum tubes were performed using MARC analysis.<br />

A three-dimensional shell model representing the tube<br />

was constructed. The weld was modeled in two steps, a<br />

thermal analysis followed by a structural analysis with the<br />

loading provided by the temperatures from the thermal<br />

analysis. The heat input to the thermal model was based<br />

on the voltage, current, and electrode speed used during<br />

the experiment. Figure 4 shows the comparison of the<br />

analytically determined temperatures with the<br />

thermocouple data. Strains from the structural model<br />

were compared to the strain gauge data taken during the<br />

test. The final distortion was then compared with the<br />

experimentally determined deformation.<br />

Temperature (C)<br />

Temperature (C)<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

00:00.0 02:00.0 04:00.0 06:00.0 08:00.0 10:00.0<br />

Time (min:sec:tenths)<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

0<br />

00:00.0 02:00.0 04:00.0 06:00.0 08:00.0 10:00.0<br />

Time (min:sec:tenths)<br />

Summary and Conclusions<br />

T/C 1<br />

T/C 2<br />

T/C 3<br />

T/C 5<br />

T/C 6<br />

T/C 8<br />

T/C 9<br />

Loc 1<br />

Loc 2<br />

Loc 3<br />

Loc 5<br />

Loc 6<br />

Loc 8<br />

Loc 9<br />

Figure 4. Comparison of the analytically determined<br />

temperatures with the thermocouple data<br />

We developed computational methods and simulation<br />

tools for predicting weld durability of hydroformed thinwalled<br />

aluminum alloy extrusions and tube assemblies<br />

Design and Manufacturing Engineering 177

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