1. Improved Collision Welding Process Windows via Elementary Shock Models at the Upper Impact Velocity Limit and Analysis of Associated Damage Mechanisms
- Author
-
Barnett, Blake Daniel
- Subjects
- Materials Science, Mechanics, Solid State Welding, Collision Welding, Impact Welding, Explosion Welding, Vaporizing Foil Actuator Welding, Laser Impulse Welding, Process Modeling, Impact Physics, Shock Waves, Thermomechanics, Process Optimization, Dissimilar Metal Welding
- Abstract
Collision welding or impact welding is a solid-state welding technique which enables unique materials joining opportunities. The high velocities and short timescales of the welding process lead to extreme peak collision pressures, high strain rates, low heat inputs, steep thermal gradients, and narrow thermo-mechanically affected zones (TMAZ). These features can be advantageous in the joining of traditionally unweldable materials such as 2XXX or 7XXX series aluminum alloys, and for the joining of dissimilar metals which would form unwanted phases under traditional fusion welding. However, these same features can also make impact welding challenging to control and characterize. Analytic process limits have been developed to calculate limiting flyer velocities and impact angles for welding success as functions of the weld member properties based on the physical mechanisms that enable joining.The maximum impact velocity for a weld is determined by a dynamic solidification cracking mechanism: reflected dynamic tensile stresses arrive to the nascent weld interface prior to full interface cohesion, which is mediated by the presence of interfacial melting. However, current analytic models for the upper limit of the collision welding window were developed for autogenous welds, which develop symmetric stress conditions at impact. In this thesis, we develop alternative formulations to the analytical upper limit of the welding window which better support dissimilar welding. Shock-informed calculation of the asymmetric stress and thermal partitioning between dissimilar weld members is achieved through the application of modified Rankine-Hugoniot relations. We compare the application of the shock-informed upper limit to the existing upper limits in the context of historical data.The shock upper limit is further validated experimentally through the use of The Ohio State University Impulse Manufacturing Laboratory’s (IML) Laser Impact Welding (LIW) and Vaporizing Foil Actuator Welding (VFAW) facilities. LIW use a short duration pulse laser, both with and without chemical augmentation, to launch metal flyers to impact welding targets at velocities up to 1 km/s through the generation of ablation and detonation pressures behind the flyer in conjunction with a transparent pressure confinement backer. VFAW generates pressure pulses for flyer acceleration through capacitive discharge into consumable aluminum foils, which burst due to extremely rapid superheating well beyond the melting point.We briefly describe the IML LIW facilities including weld sample configuration, velocity profiles, and weld diagnostics including photon Doppler velocimetry (PDV) flyer acceleration the impact plane. We investigate the upper welding limit of dissimilar welds using commercially pure titanium flyers and tin targets as a model system for which the upper weld limit is within range of the IML facility flyer velocities.VFAW of a medium entropy alloy system (equimolar CrCoNi) is also utilized to demonstrate instability-driven defects’ role in failure initiation in welds that survive the impact process. These investigations show the preservation of bulk microstructures to enable advanced materials joining in conjunction with the mechanisms that can generate TMAZ defects and their associated failure modes. Together, they provide a pathway to designing weld processes to produce higher quality impact welds in thin weld members where shock propagation and instability-driven localized melting dominate the stress and thermal interactions which generate TMAZ flaws and failures.
- Published
- 2023