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D.H. Lammlein PhD Dissertation - Vanderbilt University

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Figure 106: Dynamometer data for a butted configuration, sphere weld (1000rpm,<br />

10.4ipm, 0.095” depth) using a 100º conical tool (snub-cup). The weld is a full<br />

circumferential weld and the eccentricity of the setup can be seen in the lower frame,<br />

which shows the vertical position of the tool relative to the machine stage. The<br />

eccentricity was generally around 0.02” but varied in its manifestation from weld to<br />

weld. The desired torque is closely maintained. From approximately 159 to 203 seconds<br />

the spinning tool is being gradually lowered (plunged) into the material at approximately<br />

0.002” per second. From 203 to 209 seconds the vertical and rotary (traverse) motors<br />

are stopped during a brief dwell period prior rotary motor engagement. Reductions in<br />

axial force from 188 to 203 seconds are due to material softening [27].<br />

Accounting for system eccentricity in the experimental setup for the cupped<br />

shoulder, threaded probe tool was done by mapping the eccentricity prior to the weld via<br />

a series of auto-zeroing procedures as both force and torque control proved to be<br />

inconsistent for this particular tool. The relative height of the butted hemisphere surface<br />

to the system was obtained at 60° intervals for each weld sample prior to the weld and a<br />

vertical position path was programmed into the computer for welding at the desired<br />

depth. The tool was brought from the current vertical position to the desired vertical<br />

position (moving from calibration point to calibration point around the sphere) via a<br />

linear function with parabolic blends as described in Chapter 7 of Craig [28]. In these<br />

120

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