• Chinese Journal of Lasers
  • Vol. 49, Issue 14, 1402201 (2022)
Dawei Wang1, Yangping Dong1, Yanhong Tian2, Yunjie Bi3, and Ming Yan1、*
Author Affiliations
  • 1Department of Materials Science and Engineering, College of Engineering, Southern University of Science and Technology, Shenzhen 518055, Guangdong, China
  • 2State Key Laboratory of Advanced Welding and Joining, Harbin Institute of Technology, Harbin 150001, Heilongjiang, China
  • 3Ji Hua Laboratory, Foshan 528200, Guangdong, China
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    DOI: 10.3788/CJL202249.1402201 Cite this Article Set citation alerts
    Dawei Wang, Yangping Dong, Yanhong Tian, Yunjie Bi, Ming Yan. Influencing Mechanisms of Reactive Atmospheres in Laser Additive Manufacturing of Metallic Materials[J]. Chinese Journal of Lasers, 2022, 49(14): 1402201 Copy Citation Text show less
    Schematic of two mainstream categories of LAM technologies[19]. (a) LMD; (b) LPBF
    Fig. 1. Schematic of two mainstream categories of LAM technologies[19]. (a) LMD; (b) LPBF
    Schematic of metalatmosphere reactions during LAM processing. (a) Direct-deposition LAM[34];(b) powder-bed-based LAM[28]
    Fig. 2. Schematic of metalatmosphere reactions during LAM processing. (a) Direct-deposition LAM[34];(b) powder-bed-based LAM[28]
    Influence of shielding atmospheres on the 2Cr13 melting tracks[36]. (a) Melting track deposited in pure Ar; (b) melting track deposited in pure N2
    Fig. 3. Influence of shielding atmospheres on the 2Cr13 melting tracks[36]. (a) Melting track deposited in pure Ar; (b) melting track deposited in pure N2
    Pure Ti LPBF-printed in Ar-N2 hybrid reactive atmosphere[28]. (a) 3D-reconstruction of defects in Ti samples printed by the same laser parameters but in different shielding atmospheres; (b) 3D-atom probe analysis results of one-dimensional profiles of N, O, and C and nearest neighbor distribution of N atoms (GB is acronym of grain boundary, and blue region represents the nearest neighbor analyzed region)
    Fig. 4. Pure Ti LPBF-printed in Ar-N2 hybrid reactive atmosphere[28]. (a) 3D-reconstruction of defects in Ti samples printed by the same laser parameters but in different shielding atmospheres; (b) 3D-atom probe analysis results of one-dimensional profiles of N, O, and C and nearest neighbor distribution of N atoms (GB is acronym of grain boundary, and blue region represents the nearest neighbor analyzed region)
    Microstructural images of Ti-6Al-4V LPBF-printed in pure Ar and in Ar-N2 hybrid reactive atmospheres[41]. (a) Sample printed in pure Ar; (b) sample printed in low-N2-containing atmosphere; (c) sample printed in medium-N2-containing atmosphere; (d) sample printed in high-N2-containing atmosphere; (e)-(h) magnifications of graphs Fig. 5(a)-(d)
    Fig. 5. Microstructural images of Ti-6Al-4V LPBF-printed in pure Ar and in Ar-N2 hybrid reactive atmospheres[41]. (a) Sample printed in pure Ar; (b) sample printed in low-N2-containing atmosphere; (c) sample printed in medium-N2-containing atmosphere; (d) sample printed in high-N2-containing atmosphere; (e)-(h) magnifications of graphs Fig. 5(a)-(d)
    Microstructure and performance of Ti-6Al-4V+TiC composite LPBF-printed in Ar-CH4 hybrid reactive atmosphere[32]. (a) TEM image and EDS analyzed region; (b)-(f) EDS mapping of C, Ti, Al, and V elements; (g)-(k) high-resolution TEM images of TiC nano-grains and corresponding FFT patterns; (l) HV hardness of Ti-6Al-4V and Ti-6Al-4V+TiC composites; (m) room temperature uniaxial compressive curves of three materials
    Fig. 6. Microstructure and performance of Ti-6Al-4V+TiC composite LPBF-printed in Ar-CH4 hybrid reactive atmosphere[32]. (a) TEM image and EDS analyzed region; (b)-(f) EDS mapping of C, Ti, Al, and V elements; (g)-(k) high-resolution TEM images of TiC nano-grains and corresponding FFT patterns; (l) HV hardness of Ti-6Al-4V and Ti-6Al-4V+TiC composites; (m) room temperature uniaxial compressive curves of three materials
    316L stainless steel LPBF-printed in Ar-O2 and Ar-N2 hybrid reactive atmospheres (TS, YS, Elong, and IE are acronyms of tensile strength, yield strength, elongation at fracture, and Charpy impact energy, respectively)[44]. (a) Mechanical properties of 316L printed in Ar-O2 atmospheres; (b) mechanical properties of 316L printed in Ar-N2 atmospheres; (c) oxide particles in 316L printed in an Ar-O2 atmosphere; (d) nitride particles in 316L printed in Ar-N2 atmosphere
    Fig. 7. 316L stainless steel LPBF-printed in Ar-O2 and Ar-N2 hybrid reactive atmospheres (TS, YS, Elong, and IE are acronyms of tensile strength, yield strength, elongation at fracture, and Charpy impact energy, respectively)[44]. (a) Mechanical properties of 316L printed in Ar-O2 atmospheres; (b) mechanical properties of 316L printed in Ar-N2 atmospheres; (c) oxide particles in 316L printed in an Ar-O2 atmosphere; (d) nitride particles in 316L printed in Ar-N2 atmosphere
    CoCrFeMnNi high entropy alloy LPBF-printed in pure Ar (N-0) and Ar-50%N2 (N-50) hybrid reactive atmospheres[31]. (a)(b) Dislocation cell structure in samples printed in pure Ar and in Ar-50%N2 atmospheres; (c)-(f) high-resolution TEM images and schematic of ordered nitrogen complex; (g) room-temperature uniaxial tensile curves of two types of samples
    Fig. 8. CoCrFeMnNi high entropy alloy LPBF-printed in pure Ar (N-0) and Ar-50%N2 (N-50) hybrid reactive atmospheres[31]. (a)(b) Dislocation cell structure in samples printed in pure Ar and in Ar-50%N2 atmospheres; (c)-(f) high-resolution TEM images and schematic of ordered nitrogen complex; (g) room-temperature uniaxial tensile curves of two types of samples
    TEM images of AlCu5MnCdVA alloy LPBF-printed in Ar-O2 hybrid reactive atmospheres[50]. (a)(b) Oxide particles in samples printed in high- and low-O2-containing atmospheres; (c)(d) magnifications and SAED patterns of oxide nano particles
    Fig. 9. TEM images of AlCu5MnCdVA alloy LPBF-printed in Ar-O2 hybrid reactive atmospheres[50]. (a)(b) Oxide particles in samples printed in high- and low-O2-containing atmospheres; (c)(d) magnifications and SAED patterns of oxide nano particles
    Images of LMD-printed 316L sample using Ar-air mixture as shielding atmosphere[34]. (a) SEM image; (b) TEM image with SAED pattern; (c) diameter distribution of oxide particles; (d) room-temperature uniaxial tensile curves of four types of samples
    Fig. 10. Images of LMD-printed 316L sample using Ar-air mixture as shielding atmosphere[34]. (a) SEM image; (b) TEM image with SAED pattern; (c) diameter distribution of oxide particles; (d) room-temperature uniaxial tensile curves of four types of samples
    Microstructural images of Ti-6Al-4V and TNZT alloys, LMD-printed in various shielding atmospheres[56]. (a) Ti-6Al-4V printed in pure Ar; (b) Ti-6Al-4V printed in pure N2; (c) TNZT printed in pure Ar; (d) TNZT printed in pure N2; (e) nano-scale precipitates within the sample shown in Fig. 11(d)
    Fig. 11. Microstructural images of Ti-6Al-4V and TNZT alloys, LMD-printed in various shielding atmospheres[56]. (a) Ti-6Al-4V printed in pure Ar; (b) Ti-6Al-4V printed in pure N2; (c) TNZT printed in pure Ar; (d) TNZT printed in pure N2; (e) nano-scale precipitates within the sample shown in Fig. 11(d)
    A compositional-modified 316L, atomized and LPBF-printed in pure N2 and standard 316L LPBF-printed in pure Ar[64].(a) Room temperature uniaxial tensile curves; (b) current/potential curves tested in the 0.5 mol/L H2SO4 solution
    Fig. 12. A compositional-modified 316L, atomized and LPBF-printed in pure N2 and standard 316L LPBF-printed in pure Ar[64].(a) Room temperature uniaxial tensile curves; (b) current/potential curves tested in the 0.5 mol/L H2SO4 solution
    Ti powder modified in pure N2 reactive atmosphere[67-69]. (a) Schematic of heat treatment modification; (b) effects of powder modification; (c) room temperature uniaxial tensile properties of LPBF-printed samples using various N2-modified Ti feedstock powders
    Fig. 13. Ti powder modified in pure N2 reactive atmosphere[67-69]. (a) Schematic of heat treatment modification; (b) effects of powder modification; (c) room temperature uniaxial tensile properties of LPBF-printed samples using various N2-modified Ti feedstock powders
    Influence of ball milling in Ar-air hybrid reactive atmosphere on the feedstock Ti powder and the corresponding bulk samples[23]. (a) Unmodified HDH Ti powder with no oxidized nanocrystalline shell and modified ball milling Ti powder with oxidized nanocrystalline shell; (b) microstructural comparison between LPBF-printed samples using two types of feedstock Ti powders
    Fig. 14. Influence of ball milling in Ar-air hybrid reactive atmosphere on the feedstock Ti powder and the corresponding bulk samples[23]. (a) Unmodified HDH Ti powder with no oxidized nanocrystalline shell and modified ball milling Ti powder with oxidized nanocrystalline shell; (b) microstructural comparison between LPBF-printed samples using two types of feedstock Ti powders
    Influence of dissolved oxygen on the deformation behaviors of pure Ti and TiZrHfNb high entropy alloy (OOC is acronym of ordered oxygen complex)[45,82]. (a) Compression curves of Ti single crystals with various O mass fraction and corresponding TEM images before and after compressing; (b) TEM image demonstrating dislocation pinning effect of OOCs in TiZrHfNb sample; (c) schematic of effects of OOCs on dislocation behavior in TiZrHfNb sample
    Fig. 15. Influence of dissolved oxygen on the deformation behaviors of pure Ti and TiZrHfNb high entropy alloy (OOC is acronym of ordered oxygen complex)[45,82]. (a) Compression curves of Ti single crystals with various O mass fraction and corresponding TEM images before and after compressing; (b) TEM image demonstrating dislocation pinning effect of OOCs in TiZrHfNb sample; (c) schematic of effects of OOCs on dislocation behavior in TiZrHfNb sample
    Composites in metal matrix and their influence[68,72,84]. (a) NbC precipitation particles in maraging steel; (b)(c) oxidized film of Cu powder after reactive atmospheric modification and oxides within film; (d) effect of N content on grain sizes of three LPBF-printed Ti samples
    Fig. 16. Composites in metal matrix and their influence[68,72,84]. (a) NbC precipitation particles in maraging steel; (b)(c) oxidized film of Cu powder after reactive atmospheric modification and oxides within film; (d) effect of N content on grain sizes of three LPBF-printed Ti samples
    AlloyMicrohardness /HVWear track depth /mmWear track width /μmWear factor /(mm3·N-1·m-1)
    Ti-6Al-4V-Ar419±3220.3±0.7715±39(6.4±0.2)×10-4
    Ti-6Al-4V-N21047±29330±15
    TNZT-Ar288±213.9±0.4420±20(5.3±0.3)×10-5
    TNZT-N2518±35312±11
    Table 1. Comparison of hardness and wear properties of Ti-6Al-4V and TNZT alloys, LMD-printed in different shielding atmospheres[56]
    MaterialAtmosphereMethodYS before modification /MPaYS after modification /MPaTS before modification /MPaTS after modification /MPaOther effectRef.
    316LAr-airAtmospheric LMD500600700650Significantly enhanced ductility[34]
    Modified 316LN2Feedstock nitriding+atmospheric LPBF440778(as-printed)5731079 (as-printed)Enhanced ductility and corrosion resistance[64]
    458(solution annealed)786 (solution annealed)
    SV30N2Feedstock nitriding+atmospheric LPBFEnhanced fatigue strength[65]
    TNZT,Ti-6Al-4VN2Atmospheric LMDEnhanced wear resistance[56]
    TiAr-N2Atmospheric LPBF5337977141014Slightly enhanced ductility[28]
    TiAr-N2Feedstock Nitriding337-350600-1148394-398622-1217Strength highly-adjustable[68]
    TiAr-airFeedstock oxidizing5207856701057Enhanced ductility[76]
    Ti-6Al-4VAr-N2Atmospheric LPBF1122133612421418Slightly deceased ductility[30]
    Ti-6Al-4VAr-CH4Atmospheric LPBF1090 (compression)1120-1230(compression)1700(compression)1850-2180(compression)Significantly enhanced hardness[32]
    Ti-6Al-4VAr-airFeedstock oxidizing900-1180940-1300Notable strength-ductility trade-off[75]
    AlSi10MgN2Atmospheric LPBF341 (normal)346 (normal)445 (normal)459 (normal)Slightly enhanced ductility[33]
    323 (remelt)324 (remelt)489 (remelt)500 (remelt)
    AlCu5MnCdVAAr-O2Atmospheric LPBF156159317286Deceased ductility[50]
    CoCrFeMnNiAr-N2Atmospheric LPBF565650634690Enhanced ductility[31]
    FeCoNiCrN2Feedstock nitriding+atmospheric LPBF520650600853Enhanced ductility[66]
    CuAirFeedstock oxidizing250 (150 ℃ oxidized)Significantly enhanced laser absorptivity[72]
    345 (200 ℃ oxidized)
    Table 2. Representative metallic materials fabricated using reactive atmospheric LAM and their variations in properties
    Dawei Wang, Yangping Dong, Yanhong Tian, Yunjie Bi, Ming Yan. Influencing Mechanisms of Reactive Atmospheres in Laser Additive Manufacturing of Metallic Materials[J]. Chinese Journal of Lasers, 2022, 49(14): 1402201
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