2015
DOI: 10.1016/j.ijmachtools.2014.09.010
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Tailoring surface quality through mass and momentum transfer modeling using a volume of fluid method in selective laser melting of TiC/AlSi10Mg powder

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Cited by 211 publications
(62 citation statements)
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“…Similarly, for a medium scanning velocity (1200 mm/s), the Ra decreases first with an increase in laser power from 50 W to 60 W. However, the roughness saturated before increasing again along with an increase in laser power between 70 W and 100 W. is difference in behavior with 1200 mm/s can be attributed to the reduction in the lifetime of the molten pool and the fluid flow strength while the scanning velocity increases from 400 mm/s to 1200 mm/s. If the fluid flow strength is insufficient to overcome the viscous drag, there will be inefficient spreading of the molten pool, followed by a formation of surface asperities [18]. When the laser power increases, the melted powder volume increases, resulting in a greater demand for the flow driving forces and lifetime of the molten pool.…”
Section: Resultsmentioning
confidence: 99%
“…Similarly, for a medium scanning velocity (1200 mm/s), the Ra decreases first with an increase in laser power from 50 W to 60 W. However, the roughness saturated before increasing again along with an increase in laser power between 70 W and 100 W. is difference in behavior with 1200 mm/s can be attributed to the reduction in the lifetime of the molten pool and the fluid flow strength while the scanning velocity increases from 400 mm/s to 1200 mm/s. If the fluid flow strength is insufficient to overcome the viscous drag, there will be inefficient spreading of the molten pool, followed by a formation of surface asperities [18]. When the laser power increases, the melted powder volume increases, resulting in a greater demand for the flow driving forces and lifetime of the molten pool.…”
Section: Resultsmentioning
confidence: 99%
“…However, the molten material in the center of the melt pool leans toward the back section (creating materials bump and stacks on the surface) after further increase of the P / v to 750 J m −1 (Figure c). Excessive increase of P / v to 1500 J m −1 causes a severe material evaporation and leads to an unsmooth, lowered and interrupted melt spread, forming discontinuous scan tracks, and surface balls (Figure d) …”
Section: Mmcs From Conventional Techniques To Powder Additive Manufacmentioning
confidence: 99%
“…Schematics of the change in the melting pool dynamics and the top surface morphologies during and after SLM of AlSi10Mg/TiC composite parts with increasing the energy density: a) P = 150 W, v = 400 mm s −1 , P/v = 375 J m −1 ; b) P = 150 W, v = 300 mm s −1 , P/v = 500 J m −1 ; c) P = 150 W, v = 200 mm s −1 , P/v = 750 J m −1 ; and d) P = 150 W, v = 100 mm s −1 , P/v = 1500 J m −1 , as adapted from ref. .…”
Section: Mmcs From Conventional Techniques To Powder Additive Manufacmentioning
confidence: 99%
“…12 Whereas when considerably elevated LED of 22?5 kJ m 21 is applied, the maximum operating temperature in the molten pool is as high as 1834?8 K. The length of the molten pool exceeds the circumference, 24 resulting in the formation of the Plateau-Rayleigh instability. 18 Therefore, the melt tends to splash due to a high capillary instability of the melt in the overheating local regions. The typical metallurgical defect of the SLM process, ''balling'' effect, is likely to occur in this instance, thereby significantly influencing the thermodynamic and kinetic characteristics during the laser irradiation.…”
Section: Temperature Distributions In Molten Poolmentioning
confidence: 99%