2022
DOI: 10.1007/s10853-021-06859-1
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Recrystallization in non-conventional microstructures of 316L stainless steel produced via laser powder-bed fusion: effect of particle coarsening kinetics

Abstract: Alloys processed by laser powder-bed fusion show distinct microstructures composed of dislocation cells, dispersed nanoparticles, and columnar grains. Upon post-build annealing, such alloys show sluggish recrystallization kinetics compared to the conventionally processed counterpart. To understand this behavior, AISI 316L stainless steel samples were constructed using the island scan strategy. Rhodonite-like (MnSiO3) nanoparticles and dislocation cells are found within weakly-textured grains in the as-built co… Show more

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Cited by 35 publications
(16 citation statements)
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“…It appeared SRX nucleation takes place inhomogeneously within the as-built microstructure (Figures 5(c) and (d)), preferentially on laser beam tracks due to higher local stored energy (dislocation density) imposed by the L-PBE process, as reported elsewhere. [6] The SRX grains largely have equiaxed morphology, free of dislocations and promote the formation of low energy CSL boundaries (i.e., P 3 and P 9) through multiple twinning (Figures 5(c) to (f)). Therefore, the partial recrystallization of the microstructure at 1000 °C resulted in a significant change in the misorientation angle distribution, revealing a relatively strong peak at ~60 deg and a small peak at ~39 deg (Figure 4 3 boundaries; this is known as twin multiplication.…”
Section: Resultsmentioning
confidence: 99%
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“…It appeared SRX nucleation takes place inhomogeneously within the as-built microstructure (Figures 5(c) and (d)), preferentially on laser beam tracks due to higher local stored energy (dislocation density) imposed by the L-PBE process, as reported elsewhere. [6] The SRX grains largely have equiaxed morphology, free of dislocations and promote the formation of low energy CSL boundaries (i.e., P 3 and P 9) through multiple twinning (Figures 5(c) to (f)). Therefore, the partial recrystallization of the microstructure at 1000 °C resulted in a significant change in the misorientation angle distribution, revealing a relatively strong peak at ~60 deg and a small peak at ~39 deg (Figure 4 3 boundaries; this is known as twin multiplication.…”
Section: Resultsmentioning
confidence: 99%
“…The current AM process is known to create materials with a high dislocation density (i.e., ~10 14 m À2 ), [5,6] appearing as dislocation cells. The dislocation substructure originates from thermal distortions during printing, primarily initiated by constraints surrounding the melt pool, very rapid cooling and subsequent alternating heating/cooling cycles.…”
Section: Resultsmentioning
confidence: 99%
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