Effects of Oxygen Increasing/Decreasing Processes on Surface Characteristics of Superalloy Powders and Properties of Their Bulk Alloy Counterparts: Powders Storage and Degassing
ZHENG Liang1(), ZHANG Qiang1,2, LI Zhou1, ZHANG Guoqing1()
1Advanced High Temperature Structural Materials Laboratory, Beijing Institute of Aeronautical Materials, Beijing 100095, China 2Beijing Advanced Innovation Center for Materials Genome Engineering, University of Science and Technology Beijing, Beijing 100083, China
Cite this article:
ZHENG Liang, ZHANG Qiang, LI Zhou, ZHANG Guoqing. Effects of Oxygen Increasing/Decreasing Processes on Surface Characteristics of Superalloy Powders and Properties of Their Bulk Alloy Counterparts: Powders Storage and Degassing. Acta Metall Sin, 2023, 59(9): 1265-1278.
Oxygen content of Ni-based superalloy powders is higher than those of their bulk alloy counterparts due to the larger specific surface area of the former, which is detrimental to the performance of powder metallurgy (PM) and additive manufacturing (AM) superalloys. Therefore, at present, research in this field is primarily focused on understanding the mechanism of oxygen content increase of the powders and approaches of oxygen decrease. Storage and degassing treatment are typical processes of increasing and decreasing of oxygen content in superalloy powders, respectively. Studying the effects of these processes is of great significance for guiding the optimization of powder treatment processes and further improving alloy properties. The original surface state of powders with different narrow particle size ranges, as well as the effects of oxygen increasing/decreasing processes, i.e. storage and degassing, on the microstructure and mechanical properties of alloys were investigated using field emission scanning electron microscopy (FESEM), X-ray photoelectron spectroscopy (XPS), focused ion beam (FIB), high-angle annular dark field scanning transmission electron microscopy (HAADF-STEM), and temperature programmed desorption with mass spectrometry (TPD-MS). The results indicate that the surface composition of the original powders with different particle sizes has no significant difference, all samples exhibit NiO/Ni(OH)2, TiO2, CoO, and Cr2O3 on their surfaces. The average thickness of the surface oxide layer for 0-15 μm fine and 150-180 μm coarse powders is 3.32 and 10.90 nm, respectively. The oxygen content of the 0-15 μm fine powders and 150-180 μm coarse powders gradually increases in ambient air environment and stabilize at about 250 × 10-6 and 40 × 10-6, respectively, within 3-10 d. The oxygen content of the bulk alloy consolidated from the post-storage powders (0-53 μm) increased compared to that of the alloy from pre-storage powders, and the tensile strength at room temperature, 650oC, and 750oC showed minor changes, but the ductility decreased and the stress rupture properties of the alloy at 650oC, 890 MPa and 750oC, 530 MPa decreased. During the heating process from room temperature (~25oC) to 1000oC, the gas desorption occurred on the 0-15 μm fine powders, with desorption peaks of CO2, H2O, and H2 observed. The gas desorption mainly occurred on the powders surface in the range of 100-600oC, and the desorption peaks are mainly located within 300-600oC. However, the desorption peaks were not obvious during the heating of the 150-180 μm coarse powders. The oxygen content of the alloy consolidated from powders with particle size range of 0-53 μm decreased from 195 × 10-6 in the initial state to 113 × 10-6 after the (300oC + 600oC) combined degassing process. Alloys prepared from powders that underwent combined degassing exhibited higher mechanical properties, with the performance improvement mainly reflected in the ductility index of the alloy. The oxygen increase mechanism of superalloy powders mainly includes surface oxidation and surface adsorption, while the oxygen decreases mainly due to the desorption of oxygen-bearing gases on the powder surface. The temperatures of the peak position in the desorption curves of superalloy powders were selected to accurately customize the holding temperature of the degassing process. As a result, through multi-stage degassing treatment at 25oC + 150oC + 310oC + 470oC, the oxygen content of the powders (0-53 μm) stored in ambient air was further reduced to within (87-96) × 10-6.
Fund: National Natural Science Foundation of China(52071310);National Natural Science Foundation of China(52127802);National Science and Technology Major Project(Y2019-VII-0011-0151);Key Laboratory Fund(6142903200303);Key Laboratory Fund(6142903220302)
Corresponding Authors:
ZHANG Guoqing, professor, Tel: (010)62496137, E-mail: g.zhang@126.com; ZHENG Liang, senior research engineer, Tel: (010)62498268, E-mail: liang.zheng@biam.ac.cn
Fig.1 Surface morphologies of FGH96 superalloy powders with different narrow particle size ranges (a) 0-15 μm (b) 75-100 μm (c) 150-180 μm
Fig.2 XPS survey spectra of FGH96 superalloy powders with different narrow particle size ranges
Fig.3 Detailed XPS high-resolution spectra of Ni2p (a), Ti2p (b), Co2p (c), Cr2p (d), C1s (e), and O1s (f) on the surface of FGH96 superalloy powders with different narrow particle size ranges
Fig.4 XPS etch depth analyses of different elemental concentrations for FGH96 superalloy powders with different narrow particle size ranges (a) 0-15 μm (b) 150-180 μm
Fig.5 Relative intensity (I / Iω ) of Ni-metal (Nimet) and oxygen (O) with different ion etching depths by XPS, indicating surface NiO/Ni(OH)2 layer thickness of FGH96 superalloy powders with narrow particle size ranges of 0-15 μm (a) and 150-180 μm (b)(I—intensity of Nimet or O at different etch depth, Iω —intensity of Nimet or O at etch depth of 50 nm)
Fig.6 Cross-sectional images of high-angle annular dark field scanning transmission electron microscopy (HAADF-STEM) (left) and energy dispersive spectrum (EDS) elemental mapping (right) on surface oxide layer of FGH96 superalloy powders with different particle size ranges (a) 0-15 μm (b) 150-180 μm
Fig.7 Curves of oxygen content of FGH96 superalloy powders with different narrow particle size ranges stored in ambient air (20oC, 40%-50%R.H.) for different time
Fig.8 SEM images (a, d), EBSD images (b, e), and average grain sizes (c, f) of hot isostatic pressed (HIPed) bulk alloys consolidated from original (HIP-1, with oxygen content of about 120 × 10-6) (a-c) and stored (in the atmospheric environment for 90 d, HIP-2, with oxygen content of about 200 × 10-6) (d-f) FGH96 superalloy powders with particle size range of 0-53 μm (PPB—prior particle boundary)
Fig.9 Tensile stress-strain curves (a) and mechanical properties of HIP-1 and HIP-2 bulk alloys at ambient temperature (25oC) (b), 650oC (c), and 750oC (d) (YS—yield strength, UTS—ultimate tensile strength, El—elongation, A—reduction of area)
Fig.10 Low (left) and high (right) magnified SEM images of tensile fracture surfaces of HIP-1 (a, c, e) and HIP-2 (b, d, f) bulk alloys at ambient temperature (25oC) (a, b), 650oC (c, d), and 750oC (e, f)
Stress rupture condition
Alloy
Rupture life / h
El / %
A / %
650oC, 890 MPa
HIP-1
29.1 ± 1.2
27.7 ± 1.1
25.2 ± 0.9
HIP-2
22.0 ± 0.5
22.5 ± 1.9
21.6 ± 1.2
750oC, 530 MPa
HIP-1
32.4 ± 0.8
14.1 ± 0.3
16.3 ± 0.4
HIP-2
28.1 ± 0.6
10.1 ± 1.7
10.9 ± 1.3
Table 1 Stress rupture properties of HIP-1 and HIP-2 bulk alloys at 650oC, 890 MPa and 750oC, 530 MPa
Fig.11 Temperature programmed desorption with mass spectrometry (TPD-MS) degassing curves of FGH96 superalloy powders with different narrow particle size ranges at heating rate of 20oC/min
Sample
Degassing parameter
Oxygen content / 10-6
25oC degassing
25oC, 2 h
195
300oC degassing
25oC, 2 h + 300oC, 5 h
140
600oC degassing
25oC, 2 h + 600oC, 5 h
124
300oC + 600oC degassing
25oC, 2 h + 300oC, 5 h + 600oC, 5 h
113
Table 2 Degassing parameter setup of FGH96 superalloy powders (0-53 μm original powders stored in ambient for 15 d, degassing vacuum condition ≤ 10-3 Pa) and the oxygen contents of relative alloys
Fig.12 Microstructures of HIPed alloys consolidated from FGH96 superalloy powders with different degassing processes, indicating the severity of PPBs defects (a) 25oC degassing (b) 300oC degassing (c) 600oC degassing (d) 300oC + 600oC degassing
Fig.13 Tensile properties of FGH96 alloy at ambient temperature (25oC) (a), 650oC (b), and 750oC (c) HIP consolidated from powders with different degassing processes
Fig.14 Tensile fracture surfaces of HIPed FGH96 alloy consolidated from air stored powders after 25oC (a, b, e, f, i, j) and 300oC + 600oC (c, d, g, h, k, l) degassing (a-d) 25oC tensile (e-h) 650oC tensile (i-l) 750oC tensile
Fig.15 Optimization and precise customization of multi-stage degassing process parameters for Ni-based superalloy powders and oxygen content of the manufactured alloys
1
Pollock T M, Tin S. Nickel-based superalloys for advanced turbine engines: Chemistry, microstructure and properties [J]. J. Propuls. Power, 2006, 22: 361
doi: 10.2514/1.18239
2
Reed R C. The Superalloys: Fundamentals and Applications [M]. Cambridge: Cambridge University Press, 2006: 2
3
Zhang G Q, Zhang Y W, Zheng L, et al. Research progress in powder metallurgy superalloys and manufacturing technologies for aero-engine application [J]. Acta Metall. Sin., 2019, 55: 1133
Bai Q, Lin J, Tian G, et al. Review and analysis of powder prior boundary (PPB) formation in powder metallurgy processes for nickel-based super alloys [J]. J. Powder Metall. Min., 2015, 4: 127
5
Tan L M, Li Y P, Liu C Z, et al. The evolution history of superalloy powders during hot consolidation and plastic deformation [J]. Mater. Charact., 2018, 140: 30
doi: 10.1016/j.matchar.2018.03.039
6
Rao G A, Srinivas M, Sarma D S. Effect of oxygen content of powder on microstructure and mechanical properties of hot isostatically pressed superalloy Inconel 718 [J]. Mater. Sci. Eng., 2006, A435-436: 84
7
Zheng B L, Ashford D, Zhou Y Z, et al. Influence of mechanically milled powder and high pressure on spark plasma sintering of Mg-Cu-Gd metallic glasses [J]. Acta Mater., 2013, 61: 4414
doi: 10.1016/j.actamat.2013.04.011
8
Dai D H, Gu D D. Influence of thermodynamics within molten pool on migration and distribution state of reinforcement during selective laser melting of AlN/AlSi10Mg composites [J]. Int. J. Mach. Tools Manuf., 2016, 100: 14
doi: 10.1016/j.ijmachtools.2015.10.004
9
Hryha E, Gierl C, Nyborg L, et al. Surface composition of the steel powders pre-alloyed with manganese [J]. Appl. Surf. Sci., 2010, 256: 3946
doi: 10.1016/j.apsusc.2010.01.055
10
Chasoglou D, Hryha E, Norell M, et al. Characterization of surface oxides on water-atomized steel powder by XPS/AES depth profiling and nano-scale lateral surface analysis [J]. Appl. Surf. Sci., 2013, 268: 496
doi: 10.1016/j.apsusc.2012.12.155
11
Karlsson H, Nyborg L, Berg S. Surface chemical analysis of prealloyed water atomised steel powder [J]. Powder Metall., 2005, 48: 51
doi: 10.1179/0032589005X37675
12
Wendel J, Shvab R, Cao Y, et al. Surface analysis of fine water-atomized iron powder and sintered material [J]. Surf. Interface Anal., 2018, 50: 1065
doi: 10.1002/sia.v50.11
13
Riener K, Oswald S, Winkler M, et al. Influence of storage conditions and reconditioning of AlSi10Mg powder on the quality of parts produced by laser powder bed fusion (LPBF) [J]. Addit. Manuf., 2021, 39: 101896
14
Hryha E, Shvab R, Bram M, et al. Surface chemical state of Ti powders and its alloys: Effect of storage conditions and alloy composition [J]. Appl. Surf. Sci., 2016, 388: 294
doi: 10.1016/j.apsusc.2016.01.046
15
Zhang Q, Zheng L, Yuan H, et al. Influence of storage conditions on powder surface state and hot deformation behavior of a powder metallurgy nickel-based superalloy [J]. Adv. Eng. Mater., 2022, 24: 2101615
doi: 10.1002/adem.v24.8
16
Zhang Q, Zheng L, Yuan H, et al. Effect of humid atmosphere on the microstructure and mechanical properties of a PM Ni-based superalloy: From powders to bulk alloys [J]. Mater. Charact., 2023, 202: 113019
doi: 10.1016/j.matchar.2023.113019
17
Whitman C A, O’Flynn J T, Rayner A J, et al. Determining the oxidation behavior of metal powders during heating through thermogravimetric and evolved gas analysis using a coupled thermogravimetry-gas chromatography-mass spectrometry technique [J]. Thermochim. Acta, 2016, 638: 124
doi: 10.1016/j.tca.2016.06.019
18
Estrada J L, Duszczyk J, Korevaar B M. Gas entrapment and evolution in prealloyed aluminium powders [J]. J. Mater. Sci., 1991, 26: 1431
doi: 10.1007/BF00544650
19
Yamasaki M, Kawamura Y. Changes in the surface characteristics of gas-atomized pure aluminum powder during vacuum degassing [J]. Mater. Trans., 2006, 47: 1902
doi: 10.2320/matertrans.47.1902
20
Iwamoto K, Yamasaki M, Kawamura Y. Vacuum degassing behavior of rapidly solidified Al-Mn-Zr alloy powders [J]. Mater. Sci. Eng., 2007, A449-451: 1013
21
Yamasaki M, Kawamura Y. Effect of vacuum degassing on surface characteristics of rapidly solidified Al-based alloy powders [J]. Mater. Trans., 2004, 45: 1335
doi: 10.2320/matertrans.45.1335
22
Nagaishi Y, Yamasaki M, Kawamura Y. Effect of process atmosphere on the mechanical properties of rapidly solidified powder metallurgy Al-Ti-Fe-Cr alloys [J]. Mater. Sci. Eng., 2007, A449-451: 794
23
Zhang Q, Zheng L, Yuan H, et al. Effects of composition and particle size on the surface state and degassing behavior of nickel-based superalloy powders [J]. Appl. Surf. Sci., 2021, 556: 149793
doi: 10.1016/j.apsusc.2021.149793
24
Luo X J, Zhang L C, Li Z, et al. The study on degassing behavior of nickel-base superalloy FGH96 powder [J]. Powder Metall. Ind., 2021, 31(4): 16
Zheng L, Zhang G Q, Gorley M J, et al. Effects of vacuum on gas content, oxide inclusions and mechanical properties of Ni-based superalloy using electron beam button and synchrotron diffraction [J]. Mater. Des., 2021, 207: 109861
doi: 10.1016/j.matdes.2021.109861