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Materials Science in Additive Manufacturing                      Customized scans and dwell time on AM 316L




                         A
                                                                    B














                         C
                                                                    D
















            Figure 4. Scanning electron microscopy micrographs of S1 (A and B) and S4 (C and D) printed samples showing the presence of both elongated cell
            structure and equiaxed substructure along the build direction. Magnification: (A and C): ×1500; (B and D): ×5000.

            Table 3. Energy dispersive X‑ray spectroscopy spot analysis   lower peak count and higher intensity, in contrast to the
            of the S1 and S4 samples                           S1 bottom section (Figure 6A) where smaller grain size,
                                                               higher grain count, and lower intensities are observed,
            Spot no.              Elements (wt. %)             consistent with findings by Pathak  et al.  Comparable
                                                                                                 10
                      Fe     Cr    Ni     Mo     Si    Mn      differences between the top and bottom sections are
            1         60.2   20.3  14.3   2.5    2.2   0.6     observed in Figure 6C and D for S4 sample. In addition,
            2         64.8   18.4  13.7   0.4    1.3   1.3     the top sections of S1 and S4  samples reveal multiple
            3         62.7   18.2  11.0   1.8    3.2   3.2     intense peaks, suggesting the presence of grain sizes larger
            4         65.0   17.4  14.1   1.9    0.9   0.8     than those in the bottom sections. The presence of intense
            5         64.5   19.6  12.2   2.1    0.7   0.9     peaks can be attributed to the processing conditions and
            6         64.7   18.5  13.2   2.2    0.8   0.6     cooling rates of the interlayer, whose temperature increases
                                                                                 10
                                                               through the deposition.  Without preheating the substrate,
                                                               the initial deposition of the print layer experiences a
            identified at 2θ angles of 43.61°, 50.68°, 74.57°, and 90.50°,   relatively lower temperature. As the build layers increase,
            respectively. Using the Nelson–Riley and Williamson–Hall   heat accumulates, resulting in higher temperatures at the
            extrapolation methods, the lattice constants and micro-  top section of the print samples. This may potentially lead
            strains for S1 were determined to be 3.57 ± 0.003 Å and   to larger grain sizes at the top section than at the bottom
            3.61 × 10 , respectively, and the corresponding values for   section of the print samples. 10,29
                   −3
            S4 were 3.59 ± 0.028 Å and 3.05 × 10 , respectively.
                                         −3
              The pole figure of the {111} peak with a strong intensity   3.4. Internal defects analysis using X-ray micro-CT
            at 2θ = 43.5° for various sections of the 316L metallic sample   X-ray computed tomography was employed for internal
            includes S1 bottom and top sections (Figure 6A and B) and   defects analysis of the printed samples before tensile testing.
            S4 bottom and top sections (Figure 6C and D, respectively.   The reconstructed 3D images of the fracture sections of the
            The {111} peak texture of the S1  sample’s top section   S1 sample (Figure 7A) and the S4 sample (Figure 7B), with
            (Figure  6B) displays a larger grain size, evident from a   emphasis on the bulk part to highlight low-density internal



            Volume 3 Issue 1 (2024)                         5                       https://doi.org/10.36922/msam.2676
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