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Materials Science in Additive Manufacturing                           AM-produced CoCrFeMnNi properties




                         A                                  B












            Figure 13. Tensile properties of selective laser melting produced CoCrFeMnNi at 450 and 750 mm/s scanning speeds before and after heat treatment.
            (A)  Room temperature stress-strain curves; (B) ultimate tensile strength and elongation.



















            Figure 14. Microhardness results for selective laser melting-produced   Figure 15. Energy absorption during  Charpy test  for  selective laser
            CoCrFeMnNi at 450 and 750 mm/s scanning speeds before and after heat   melting-produced CoCrFeMnNi at 450 and 750 mm/s scanning speeds
            treatment, along with the microhardness values reported in literature. [66-69]  before and after heat treatment, along with the reported absorption
                                                               energies in literature [22,71] . Note that the DED result  was obtained at 0°C.
                                                                                               [71]
            by 15.6%, while that for the 750 mm/s samples increased
            by 11.1%. The absorbed impact energy of both HT    are cleavage facets whose presence indicates brittle type
            and untreated samples are noticeably smaller than   fracture [43,71] . Cleavage facets are surrounded by region
            the energy absorbed by VIM-produced CoCrFeMnNi     that consists of dimples and microvoid coalescence of a
            (approximately 200 J)  which, in turn, is half that of the   submicron size. Abundance of dimple pattern is a typical
                             [22]
            forged Al CoCrFeNi . On the other hand, Charpy results   characteristic of ductile fracture,  which is  related  to the
                            [70]
                   x
            of the current study are significantly higher compared to   coalescence of microvoids. The microvoids can form due to
            CoCrFeMnNi sample made by DED whose impact energy   decohesion between second-phase particle and matrix .
                                                                                                           [43]
            was  measured  to  be  only  50  J at  0°C .  This toughness   High magnification image in Figure 16B of dimple pattern
                                           [24]
            reduction of SLM-produced samples compared to the cast   shows that they were formed by both normal and shear
            samples can be attributed to the presence of defects, such   ruptures. When the SEM electron probe hits inclined edge
            as pores, impurities, and brittle, non-equilibrium phases.   of a dimple, more of secondary electrons escape from it
            The latter two were not observed in the present work but   than from the flat surface of cleavage facets. This leads to
            the existence of defects, such as LOF and micro-cracks,   so-called edge effect leading to brighter appearance of the
            described above may explain such toughness reduction.  region that surrounds cleavage facets . Figure 16C and D
                                                                                            [72]
              To better understand the impact behavior, fracture   shows two cleavage facets whose size differs roughly by
            surface images of 450 and 750 mm/s samples, both before   an order of magnitude. The smaller one demonstrates
            and after heat treatment, were studied. Higher magnification   clearly defined cleavage steps, river pattern and dimples
            SEM images reveal features that are characteristic for both   surrounding the cleavage area, which are similar to the
            ductile and brittle fracture. For instance, Figure 16A shows   features observed on the fracture surface of AlCoCrCuFeNi
            that vast area of fracture surface is dominant by large dark   HEA . Besides, unmelted powder particles are observed
                                                                   [71]
            islands with average size of 50 – 150 μm surrounded by a   on fracture surface of all studied samples. In most cases,
            texture that appears brighter. The observed flat dark islands   they  are  found in  a  colony  of  conglomerated  particles,


            Volume 2 Issue 1 (2023)                         12                       https://doi.org/10.36922/msam.42
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