1School of Materials Science and Engineering, Xi'an University of Technology, Xi'an 710048, China 2Science and Technology on Advanced High Temperature Structural Materials Laboratory, AECC Beijing Institute of Aeronautical Materials, Beijing 100095, China
Cite this article:
ZHANG Leilei, CHEN Jingyang, TANG Xin, XIAO Chengbo, ZHANG Mingjun, YANG Qing. Evolution of Microstructures and Mechanical Properties of K439B Superalloy During Long-Term Aging at 800oC. Acta Metall Sin, 2023, 59(9): 1253-1264.
The K439B alloy is a novel equiaxed superalloy and is used for producing hot section components that need to resist high temperatures in aero engines and gas turbines as its temperature capacity exceeds 800oC. In this study, the evolution of the microstructure and mechanical properties of K439B equiaxed superalloy after being subjected to long-term aging at 800oC for 3000 h was examined. The predominant deformation mechanisms affecting room-temperature tensile and stress rupture properties at 815oC and under 379 MPa stress following different aging durations for the K439B alloy were investigated.Results indicate that for heat-treated alloy, the morphology of the γ' phase is spherical, MC carbide is generated in the interdendritic region and grain boundaries, while M23C6 carbide is in the grain boundaries. During long-term aging at 800oC, γ′ precipitates conform to the Ostwald ripening mechanism for growth and tend to take a cubic form; the coarsening rate of the γ′ phase is calculated to be 71.7 nm3/h; Additionally, the MC carbide deteriorates while the content of M23C6 carbide gradually increases. After long-term aging for 3000 h, the precipitated grain boundary phase comprises MC carbide, γ′ phase, and M23C6 carbide; the orientation relationship between γ′ phase and M23C6 carbide can be described as [111] γ' //[111] MC and () γ′ //() MC. The heat-treated alloy demonstrates room-temperature tensile and yield str-engths of 1159.0 MPa and 911.5 MPa, respectively. Meanwhile, the stress rupture life at 815oC and under 379 MPa stress is 150.4 h. As the size of γ′ precipitates increases, the dominant deformation mechanism shifts from dislocation slipping in the matrix to dislocation cutting through the γ′ phase after long-term aging, resulting in superior stacking faults appeared in the γ′ phase. Consequently, the room-temperature tensile strength and stress rupture life show reduction at 815oC and under 379 MPa stress.
Fund: National Science and Technology Major Project of China(J2019-VI-0004-0117);National Key Research and Development Program of China(2022YFB3706804);Science and Technology on Advanced High Temperature Structural Materials Laboratory Fund(6142903210104);Science and Technology on Advanced High Temperature Structural Materials Laboratory Fund(6142903220101);AECC Science and Technology Innovation Platform Project(CXPT-2018-006)
Fig.1 Low (a, c, e) and high (b, d, f) magnified OM images of microstructures of K439B alloy subjected to long-term aging at 800oC for 0 h (a, b), 1000 h (c, d), 3000 h (e, f) (GB—grain boundary)
Fig.2 Typical microstructures of γ′ precipitates in the dendrite core of K439B alloy subjected to long-term aging at 800oC for 0 h (a), 100 h (b), 500 h (c), 1000 h (d), 2000 h (e), and 3000 h (f)
Fig.3 Size distributions of γ′ precipitates in the dendrite core of K439B alloy subjected to long-term aging at 800oC for 0 h (a), 100 h (b), 500 h (c), 1000 h (d), 2000 h (e), and 3000 h (f)
Aging
Average
Volume
Feret ratio
time / h
size / nm
fraction / %
0
47.0 ± 1.9
22.9 ± 1.2
1.09 ± 0.03
100
51.8 ± 1.4
23.4 ± 0.9
1.29 ± 0.02
500
74.3 ± 2.3
23.7 ± 1.0
1.34 ± 0.01
1000
92.4 ± 2.5
23.1 ± 0.8
1.36 ± 0.01
2000
112.6 ± 3.5
23.2 ± 1.6
1.39 ± 0.01
3000
120.3 ± 2.2
24.5 ± 1.7
1.42 ± 0.01
Table 1 Size, volume fraction, and shape factor of γ′ precipitates in the dendrite core of K439B alloy subjected to long-term aging at 800oC
Fig.4 Relationship between size of γ′ precipitates in the dendrite core and aging time of K439B alloy at 800oC (—average radius of γ′ after aging for 0 h; —average radius of γ′ after aging for time t; k—LSW theory coarsening rate constant; R2—coefficient of determination)
Fig.5 Evolution of carbide distributed in the interdendritic region (a, c, e) and at the grain boundary (b, d, f) of K439B alloy subjected to long-term aging at 800oC for 0 h (a, b), 1000 h (c, d), and 3000 h (e, f)
Fig.6 Carbide in the heat-treated K439B alloy (a) MC carbide distributed in the interdendritic region (b) HRTEM image from the edge of the MC carbide (marked with an arrow in Fig.6a) and the atomic-scale HRTEM images from the regions 1# and 2# with corresponding fast Fourier transform (FFT) patterns (insets) (c, d) MC carbide (c) and M23C6 carbide (d) at the grain boundary with corresponding SAED patterns (insets)
Fig.7 Grain boundary precipitated phase, SAED patterns of regions 1#-3#, and EDS compositional mapping of K439B alloy subjected to long-term aging at 800oC for 3000 h
Aging time
Interdendritic region
Grain boundary
h
%
%
0
-
20.86
100
-
23.64
500
-
25.98
1000
2.34
29.40
2000
6.58
36.43
3000
10.19
38.93
Table 2 Contents of M23C6 carbide in the interdendritic region and at grain boundary of K439B alloy subjected to long-term aging at 800oC
Fig.8 Room temperature tensile properties (a) and 815oC, 379 MPa stress rupture properties (b) of K439B alloy subjected to long-term aging at 800oC (σb—tensile strength, σp0.2—yield strength, δ—elongation, τ—stress rupture life )
Fig.9 Dislocation structures near room temperature tensile fracture surface of K439B alloy subjected to long-term aging at 800oC for 0 h (a, b), 1000 h (c, d), and 3000 h (e, f)
Fig.10 Dislocation structures near 815oC, 379 MPa stress rupture fracture surface of K439B alloy subjected to long-term aging at 800oC for 0 h (a-c) and 3000 h (d-f)
Fig.11 Schematics of microstructural evolution of K439B alloy during long-term aging at 800oC for 0 h (a), 1000 h (b), and 3000 h (c) (ID—interdendritic region)
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