Journal
OPTICS AND LASER TECHNOLOGY
Volume 171, Issue -, Pages -Publisher
ELSEVIER SCI LTD
DOI: 10.1016/j.optlastec.2023.110378
Keywords
Selective laser melting; Laser energy; Layer thickness; Single track; Melt pool; Defects
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This study investigates the evolution of track morphology, melt pool characteristics, and defects in additively manufactured mold steel under different layer thicknesses and laser energy densities. The results show that the morphology of single tracks and the characteristics of the melt pool change with the increase in line energy density. Furthermore, an increase in layer thickness leads to the occurrence of certain defects.
Large layer thickness is essential to increase building rate, but excessive layer thickness easily lead to defects which negatively affect component quality. The evolution of track morphology, melt pool characteristics and defects of additively manufactured mold steel by using various larger layer thickness (60 and 90 mu m) while also varying the laser energy density was investigated systematically. Results indicated that the morphologies of single tracks shifted sequentially from discontinuousness to continuous irregularity and continuous regularity with the increasing line energy density at 60 mu m layer thickness. The width and depth of melt pool increased substantially with the line energy density increased from 0.4 to 1.3 J/mm, while the height of melt pool was nearly constant. Correspondently, transition of the melt pool based on the depth-to-width ratio from balling to conduction and keyhole modes was observed. When the layer thickness increased from 60 to 90 mu m, the average build percentage of the single tracks decreased by 43 % with increasing line energy density from 0.26 to 0.51 J/ mm, and more spatters around the surface of tracks were found at 0.8 J/mm. Interestingly, the average width of the melt pool decreased by 37 mu m, while the height of melt pool increased by 45 mu m. More small spherical gas pores (5-15 mu m) occurred in bottom of keyhole due to trapped vapor at high energy density. The decrease in melt width with increased layer thickness is most likely due to the weakened Marangoni convection. Finally, for-mation mechanism of lack-of-fusion defects and gas pores with larger layer thickness processing were analyzed based on melt pool characteristics, such as spheroidization, keyhole and spatters.
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