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Figure 1 A simple rectangular laser pulse waveform.
Figure 2 Distribution of peak temperature (ºC) one second after the start of welding.
Figure 3 Predicted thermal cycles at two monitoring locations.
Computational Modeling-based Thermal Management for Pulsed Laser Welding of Small-Scale DevicesWei Zhang, Engineering Team Leader, Materials & Structural Integrity
Pulsed laser welding is a widely used process to produce a hermetic seal for the enclosure of sensitive components in containers of small-scale devices such as those found in the medical and electronic industries. Through the nature of the welding process there is a local increase in temperature that must be dissipated through conduction of heat into the body of the component and convection and radiation into the surrounding environment. The resulting temperature increases may cause damage to some sensitive components. Figure 1 shows a simple rectangular laser pulse waveform, where Pmax is the peak laser power, ton is the laser-on time, and ta is the total time of a pulse. The pulsed laser welding procedure can be characterized by three parameters: pulse energy (Pmax × ton), pulse frequency (1/ta), and travel speed. EWI has developed a computational modeling-based framework to accurately predict the temperature to which sensitive components may be exposed during welding. Approach Case Study - Pulsed Laser Welding of Flat Titanium Sheets Interestingly, it is noted that the heat-affected zone for set A is much smaller than that for set B. In other words, if a sensitive component is placed at the same distance from the weld center line, it will experience much lower temperature for set A than set B. This phenomenon is more clearly illustrated in Figure 3, where the thermal cycles at 0.6 and 1.0 mm away from the weld center line are plotted. As shown in this figure, the individual laser pulses lead to oscillation in the temperature profile. When the laser pulse is on, the temperature rises and vice versa. The closer to the weld center, the larger the temperature oscillation occurs. Since set A has a much lower pulse frequency, it provides sufficient time for the heat to dissipate into the plate. As a result, there is a lower heat build-up near the weld. On the other hand, set B constantly puts heat into the weld, and there is not enough time for the heat conduction away from the weld region. Therefore, there is extensive heat accumulation near the weld. The predicted thermal history indicates that set A can effectively decrease the peak temperature experienced by sensitive components located in the vicinity of the weld. Summary and Conclusions For more information, please contact Wei Zhang at 614.688.5163 or wei_zhang@ewi.org. |
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