Beam-based additive manufacturing (AM) is an innovative technique in which parts are built layerwise, starting from the material in powder form. As a developing manufacturing technique, achievement of excellent mechanical properties in the final part is of paramount importance for the mainstream adoption of this technique in industrial manufacturing lines. At the same time, AM offers an unprecedented opportunity to precisely control the manufacturing conditions locally within the part during build, enabling local influence on the formation of the texture and microstructure. In order to achieve the control of microstructure by tailoring the AM machine parameters, a full understanding and modeling of the heat transfer and microstructure evolution processes is needed. Here, we show the implementation of the non-equilibrium equations for phase formation and dissolution in an AM modeling framework. The model is developed for the Ti6Al4V alloy and allows us to show microstructure evolution as given by the AM process. The developed capability is applied to the cases of electron beam melting and selective laser melting AM techniques to explain the significantly different microstructures observed in the two processes.
INTRODUCTIONRapid prototyping differs from additive manufacturing (AM) in that the former is concerned with geometrical accuracy, while the latter adds a stringent requirement for the part's mechanical properties.1 This requirement arises from the fact that AM parts not only need to be built but also to be put into service with an expected performance similar to, if not better than, corresponding cast parts (if available).2 In AM, several factors contribute to the ultimate mechanical properties of the part, including the manufacturing technique, 3 the presence of porosity, including incomplete melting, 4 proper thermal control to avoid balling/overmelting, 5 and the quality of the powder feedstock. 6 Moreover, even at optimal build conditions, in which the former issues are minimized, a large role is played by the actual metal microstructure, which represents the ultimate factor that dictates the mechanical properties of the part.Ti6Al4V is a pseudo-binary alloy with rich equilibrium 7 and non-equilibrium 8 phase diagrams. The main phases are represented by b, which is stable above 1000°C (beta transus), 7 a, which is a diffusion-controlled phase stable below the beta transus, and martensite a 0 , which is a-competing and originates from diffusionless transformation of b under specific circumstances. From a traditional metallurgy point of view, Ti6Al4V has been extensively studied and significant works on it have been published.9-11 For example, Lü tjering et al. have shown that the thickness of the a lath is the primary factor influencing strength and ductility. 12 In turn, the a lath thickness is controlled by the cooling rate after solidification, where faster cooling rates correspond to thinner a laths. 13 Moreover, rapid quenching below the so-called martensite start temperature (T ms ) originates the ...