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Materials Science in Additive Manufacturing                           AM-produced CoCrFeMnNi properties



            of chosen values revealed only the  latter two regions of   is a steep thermal gradient that develops due to the high
            energy density domain as explained above. As shown in   energy input and causes the higher cooling rate. As a
            Figure  4A, laser scanning at slower than 400 mm/s resulted   result, the molten material does not have enough driving
            in severe porosity. Notice the top surfaces of the samples are   force and time to spread to become flattened. This leads
            not flat. This is a result of high energy density input used   to a big wavy surface at the top of samples . Figure 4B
                                                                                                  [49]
            to produce samples in Figure 4. High energy input causes   summarizes the quantitative characterization by means
            two phenomena that take place  in a molten  pool. First,   of measured density of cubic samples and visual analysis
            the liquid viscosity is too low to keep up the integrity of   of percent porosity as observed on their cross section. An
            the melt pool . Melt pool agitates violently which results   overall trend can be observed, that is, higher scanning
                       [47]
            in a non-uniform top surface . Second phenomenon   speeds (within the investigation range) are beneficial for
                                     [48]
                         A































                         B
























            Figure 4. Effect of scanning speed on density and porosity of selective laser melting-produced CoCrFeMnNi. (A) Optical micrographs showing cross
            sections of printed cubes for process optimization, and (B) density of the cubes measured according to ASTM B962 and porosity measured through image
            processing.


            Volume 2 Issue 1 (2023)                         6                        https://doi.org/10.36922/msam.42
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