+高级检索
网刊加载中。。。

使用Chrome浏览器效果最佳,继续浏览,你可能不会看到最佳的展示效果,

确定继续浏览么?

复制成功,请在其他浏览器进行阅读

Effect of Precipitate Phases and Grain Size on Mechanical Properties of Inconel 718 Superalloy After Various Heat Treatments  PDF

  • Zhang Min
  • Ma Chuanchuan
  • Xue Chun
  • Zhong Wenchang
  • Gao Bo
  • Shuai Meirong
  • Tuo Leifeng
  • Chu Zhibing
School of Materials Science and Engineering, Taiyuan University of Science and Technology, Taiyuan 030024, China

Updated:2024-08-09

DOI:10.12442/j.issn.1002-185X.20230684

  • Full Text
  • Figs & Tabs
  • References
  • Authors
  • About
CN CITE
OUTLINE

Abstract

Various heat treatments were conducted on Inconel 718 superalloy, and the resultant microstructures and properties were investigated to analyze the mechanisms of heat treatments. Results show that the type and quantity of precipitate phases and the grain size have different effects on the properties of Inconel 718 superalloy after various heat treatments. The γ" and γ' phases as well as grain size mainly influence the strength, and the δ phase mainly influences the plasticity. Besides, the precipitation of γ" and γ' strengthening phases can improve the yield strength. The alloy strength is inversely proportional to mean grain size when the γ" and γ' phases have similar contents. The plasticity is susceptible to the content and shape of δ phase. A proper amount of δ phase is beneficial to the plasticity, but excessive δ phase degrades plasticity.

Inconel 718 superalloy, one of the precipitate-strengthened nickel-based superalloys, is widely used in the aero-engine, rocket engine, and nuclear reactor under high-temperature conditions[

1–5], owing to its excellent stability in microstructure and mechanical properties at >650 °C. Ref.[6–8] present that the matrix of Inconel 718 superalloy is composed of face-centered cubic (fcc) γ phase, and the precipitate phases mainly consist of body-centered tetragonal γ"-Ni3Nb phase, fcc γ'- Ni3(Al, Ti, Nb) phase, and orthorhombic δ-Ni3Nb phase. Among them, the γ" and γ' phases are the important strengthening phases[9–11]. In addition, the Laves phase and MC carbides also exist in Inconel 718 superalloy. To achieve excellent performance, it is essential to study the precipitates and grain characteristics of the material.

Heat treatment can effectively regulate the precipitates and grain size of the alloy. Ref.[

12–15] demonstrate that the difference in heat treatments results in different micro-structures and grain sizes, which will eventually influence the mechanical properties of alloys. For example, the δ phase affects the strength and plasticity. Huang et al[16] found that the pinning effect results in the δ phase precipitate at the grain boundary during heat treatment. Yadav et al[17] concluded that the coarsened matrix grains can weaken the pinning effect of δ phase and reduce the strength at elevated treatment temper-atures. Zhang et al[18] verified that the δ phase degrades the strength but improves the elongation. Ran et al[19] showed that a large quantity of δ phase is beneficial to improve the plasticity. Liu et al[20] suggested that the strength is increased with the increase in size of γ" and γ' phases. Zhang et al[21] proposed that a certain quantity of γ" phase can improve the transgranular strength. Caliari et al[22] proposed that increasing the grain size can increase the hardness and creep resistance. Ye et al[23] demonstrated that the fine-grained nickel-based superalloys have excellent ductility and good strength at 550 °C, but they fail to serve at even higher temperatures.

The influence mechanisms about the characteristics and effects of precipitate phases and grains on alloys after various heat treatments are still obscure. Therefore, in this research, the changes in precipitate phases and grains were analyzed. The potential relationship among heat treatment, micro-structure, and properties was discussed. This research provided a theoretical basis to regulate the heat treatment.

1 Experiment

The hot-rolled Inconel 718 superalloy plates were used as the experiment materials, and the chemical composition is shown in Table 1. The plate thickness was 3 mm. All specimens were obtained from the plates by wire cutting. Fig.1 presents the schematic diagram of tensile specimen. Several rectangular specimens with dimension of 11 mm× 10 mm were prepared for microstructure observation. The tensile specimens were processed into specific shapes according to ASTM E8/E8M-22 standard[

24] for the evaluation of tensile properties.

Table 1  Chemical composition of hot-rolled Inconel 718 superalloy (wt%)
CSiMnPSCrNiCuTiNbBCoAlCaMoFe
0.08 0.05 0.03 0.003 0.002 19.00 52.50 0.02 0.90 5.1 0.003 0.02 0.50 0.002 3.01 Bal.

Fig.1  Schematic diagram of tensile specimen

The heat treatment experiments were designed according to the SAE AMS 5383 F standard[

25]. In this research, three types of heat treatments were conducted. (1) Double aging (DA): holding at 720 °C for 8 h, furnace cooling to 620 °C at mean cooling rate of 50 °C·s-1, holding at 620 °C for 8 h, and air cooling to room temperature (RT). (2) Standard treatment (ST): solution treatment at 954 °C for 1 h, air cooling to RT, and DA process. (3) High standard treatment (HST): homogenization treatment at 1100 °C for 1 h, air cooling to RT, and ST treatment. During the heat treatments, the heating rates were 5 °C·s-1. The surfaces of the hot-rolled and heat-treated specimens were ground, polished, and chemically etched by Kallings's reagent (5 g CuCl2+100 mL HCl+100 mL CH3CH2OH) for 510 s. The microstructure was observed by optical microscope (OM). The mean grain size was calculated by Image Pro Plus software. The phase composition was identified by energy dispersive spectroscopy (EDS). In addition, the tensile experiments of the hot-rolled and heat-treated specimens were conducted by Gleeble 3800 thermal simulator. The deformation temperature was 650 °C, and the strain rate was 0.001 s-1.

2 Results

2.1 Microstructure

Fig.2a presents the initial microstructure of hot-rolled specimens, which is mainly composed of austenite matrix γ phase, lamellar twins, dispersed carbides, borides, and a small number of γ", γ', and Laves phases. EDS results show that carbides (MC and M23C6, where M element is mainly Cr element) and borides exist in all specimens. The spherical or block carbides are distributed at the grain boundaries and within the grains. The grains around the banded carbides are smaller than those at other areas owing to the pinning effect. In other words, the banded carbides can prevent the grain elongation during heat treatment. However, the dispersion distribution of carbides may ultimately result in the uneven grain size. According to the grain size distribution in Fig.2b, the initial mean grain size (D¯) is 22.35 μm, and the size of most grains is between 10 and 15 μm.

Fig.2  Initial microstructure (a) and grain size distribution (b) of hot-rolled specimen

The treatment temperatures during DA process are 720 and

620 °C, which are both lower than the dissolution temper-atures of γ", γ', and Laves phases. The dissolution and precipitation temperatures of different phases and precipitates are listed in Table 2[

26–27]. δ phase is the γ" phase at stable state.When the aging temperature exceeds 650 °C, the γ" phase is coarsened and transformed into δ phase. According to Fig.3a, the content of γ" and γ' phases in the matrix increases, and the large-sized grains reduce significantly. As shown in Fig.3b, the size of most grains is 5–10 μm or 10–30 μm based on number frequency or area frequency, respectively. The mean grain size (20.42 μm) slightly decreases. Therefore, the static recrystallization (SRX) occurs during DA process, and the overall uniformity improves.

Table 2  Dissolution and precipitation temperatures of dif- ferent phases and precipitates in Inconel 718 super- alloy (°C)[26‒27]
Temperatureγ' phaseγ" phaseδ phasePrecipitate
Dissolution 843–871 870–930 982–1037 1037
Precipitation 593–816 595–870 780–980 -

Fig.3  Microstructure (a) and grain size distribution (b) of specimen after DA process

The temperature of solution treatment (954 °C) is higher than the dissolution temperatures of γ" and γ' phases and the precipitation temperature of δ phase. As shown in Fig.4a, there are a large number of small-sized SRX grains. Most δ phases are in the shape of particles or short rods and precipitated at the grain boundary. Some δ phases are needle-like and often distributed in a linear pattern. According to Fig.4b, the large-sized grains almost disappear. The sizes of most grains are 5–10 μm. There are small-sized SRX grains near the needle-like δ phase. These phenomena all result from the pinning effect of δ phase.

Fig.4  Microstructures (a, c) and grain size distributions (b, d) of specimens after solution treatment (a–b) and double aging treatment (c–d) of ST process

Based on the microstructure after solution treatment in Fig.4c, the main alterations after the complete ST process are the precipitation of γ" and γ' phases and the transformation from γ" phase into δ phase. The contents of δ phase and SRX grains both increase slightly. According to Fig.4d, the large-sized grains further reduce. The mean grain sizes after solution treatment and ST process reduce by about 8.64% and 13.86%, respectively. This is because the hindrance against grain boundary movement is enhanced with the increase in δ phase.

Homogenization treatment, as the first stage of HST process, is conducted at 1100 °C. As shown in Fig.5a, almost all precipitates dissolve, because the temperature exceeds the precipitate dissolution temperature. The grain size increases significantly, compared with that of the initial microstructure. Therefore, both complete recrystallization and grain growth occur. Solution treatment (Fig.5c) and double aging (Fig.5e) are the second and third stages of HST process, respectively. The δ phase is precipitated during the solution treatment, and the γ", γ', and a few δ phases are precipitated during the double aging treatment. The mean grain sizes after the three stages of HST process are 126.21, 113.42, and 103.93 μm, respectively. Therefore, SRX occurs after solid solution and aging treatment. Partial large-sized grains decompose into small-sized grains. Consequently, heat treatment has a little effect on the grain refinement.

Fig.5  Microstructures (a–c) and grain size distributions (d–f) of specimens after homogenization treatment (a, d), solution treatment (b, e), and double aging treatment (c, f) of HST process

2.2 Mechanical properties

The tensile stress-strain curves are shown in Fig.6, and the relevant parameters are shown in Table 3. Each tensile stress-strain curve can be divided into six stages: elastic deforma-tion, yield, work hardening, necking, softening (uneven plastic deformation stage), and fracture. The yield strength of heat-treated specimens is more than two times higher than that of the hot-rolled specimen, presenting significant strength increase. The yield strength of specimen after HST process is lower than that after DA and ST processes. The mechanical properties of specimens after DA process is close to those after ST process. The plasticity after any heat treatment degrades. The elongation and area reduction after DA process are better than those after HST and ST processes. The proper-ties of specimens after HST process are similar to those after ST process. In addition, the length of the uneven plastic deformation stage in Fig.6 can reflect the plasticity. This stage length after DA process is longer than that after ST and HST processes, indicating that the plasticity after DA process is optimal. The occurrence of obvious necking after DA process also supports the analysis results.

Fig.6  Tensile stress-strain curves of specimens under different conditions

Table 3  Mechanical properties of specimens after different treatments
Treatment

Yield

strength/MPa

Tensile

strength/MPa

Elongation/

%

Area

reduction/%

Hot-rolled 523.67 - - -
DA 1250.60 1545.65 26.67 27.18
ST 1276.69 1517.07 22.67 19.18
HST 1079.99 1382.19 23.33 20.03

3 Discussion

3.1 Effect of precipitates and grain size on mechanical properties

The heat treatment temperature and holding time can directly affect the precipitates and grain size and finally influence the mechanical properties. The yield strength significantly improves after various heat treatments due to the γ" and γ' strengthening phases. The yield strength of specimen after DA process is similar to that after ST process, so the δ phase barely has effect on the yield strength. The yield strength after HST process is lower than that after DA and ST processes owing to the dissolution of most Laves phase and the growth of grains. The Laves phase can damage the mechanical properties. The grain refinement can improve the strength of materials[

28–30]. Thus, the effect of δ phase on yield strength is the weakest, the co-effect of Laves phase and grains is in the middle, and the effect of γ" and γ' phases is the most significant.

The plasticity significantly decreases after various heat treatments because the precipitates hinder the dislocations at the grain boundaries. The plasticity of specimen after DA process is better than that after ST and HST processes, owing to the proper amount of δ phase and less needle-like δ phase. Proper δ phase can balance the grain boundary effect and intragranular strength owing to its pinning effect. However, excessive δ phase destroys the balance and reduces the plasticity. In addition, the needle-like δ phase can hinder the grain boundary migration, which is harmful to the ductility[

31–32]. The plasticity of specimen after ST process is similar to that after HST process. Therefore, the co-effect of the Laves phase and grains barely has effect on the plasticity.

3.2 Correlation between grain size and strength

The γ" and γ' phases and grain size play important roles in strength. Due to the similar contents of γ" and γ' phases, the strength variation mechanism mainly focuses on the grain size of specimen after various heat treatments. The Hall-Petch relationship[

33–37] is widely used to simulate the relationship between flow stress and grain size, as follows:

σ0.2=σhp+khpdm (1)

where σ0.2 is the yield strength; d is the mean grain size; σhp and khp are the material parameters; m is the correlation coefficient. The common values of m are -0.5 and -1 in the Hall-Petch relationship.

The σ0.2-d m curves with different m values are plotted in Fig.7. Two sets of related parameters can be obtained by linear fitting, as follows:

σhp=940.07khp=1422.39 m=-0.5 (2)
σhp=1038.05khp=4351.26 m=-1 (3)

Fig.7  Relationship between yield strength and mean grain size with m=-0.5 (a) and m=-1 (b)

Substituting the material parameters into Eq.(1), the σ0.2 value can be obtained, as follows:

σ0.2=940.07+1422.39d-0.5 m=-0.5 (4)
σ0.2=1038.05+4351.26d-1 m=-1 (5)

The root mean squared error (RMSE), average absolute relative error (AARE), and the correlation coefficient (R) can be calculated to evaluate the prediction error of Eq.(45), as follows:

RMSE=i=1N|Mi-Ai|N (6)
AARE=1Ni=1N|Mi-AiAi|×100% (7)
R=i=1N(Mi-M¯)(Ai-A¯)i=1N(Mi-M¯)2i=1N(Ai-A¯)2 (8)

where Mi is the predicted value; Ai is the actual value; N is the number of data; M is the average value of Mi; A is the average value of Ai.

The prediction errors are listed in Table 4. It can be seen that when the m value is -1, RMSE value is small, AARE value is closer to 0, and R value is close to 1. Therefore, the inversely proportional relationship can accurately predict the relationship between yield strength and mean grain size. Due to the good fitting, the strength prediction based on mean grain size is feasible.

Table 4  Strength prediction errors with different m values
mRMSEAARE/%R
-0.5 2.8268 0.2255 0.9993
-1 0.3622 0.0290 0.9999

4 Conclusions

1) During heat treatment, the temperature and holding time affect the precipitates and grain characteristics. On the one hand, the types and contents of the precipitates are different due to various precipitation and dissolution temperatures. On the other hand, the grain may undergo SRX, complete recrystallization, or even grain growth. However, heat treatment barely has effect on the grain refinement.

2) The types and contents of precipitates as well as grain size affect the mechanical properties. The precipitate of γ" and γ' strengthening phases and the small-sized grains are beneficial to obtain high strength. The proper δ phase is conducive to high plasticity. Excessive δ phase and needle-liked δ phase can degrade plasticity. The mechanical properties after DA process are optimal due to the fine grains, precipitation of γ" and γ' phases, and proper δ phase.

3) The effect of δ phase on yield strength is the weakest, the co-effect of Laves phase and grains is in the middle, and the effect of γ" and γ' phases is the most significant. Besides, the strength is inversely proportional to the mean grain size according to the Hall-Petch relationship.

4) The content and shape of the δ phase are primary influence factors for the plasticity. The Laves phase and grains barely have effect on the plasticity.

References

1

Xiao G F, Xia Q X, Zhang Y L et al. International Journal of Advanced Manufacturing Technology[J], 2021, 117: 199 [Baidu Scholar] 

2

Chen J T, Lu J X, Cai W et al. International Journal of Plastic-ity[J], 2023, 163: 103554 [Baidu Scholar] 

3

Han D W, Yu L X, Liu F et al. Acta Metallurgica Sinica (English Letters)[J], 2018, 31(11): 1224 [Baidu Scholar] 

4

Liu T, Cheng X N, Luo R et al. Materials Science & Engineering A[J], 2021, 819: 141533 [Baidu Scholar] 

5

Wang J G, Liu D, Ding X et al. Crystals[J], 2020, 10(4): 303 [Baidu Scholar] 

6

Wei Bo. Research on Heat-Assisted Incremental Bending For-ming Technology of Large Curvature Metal Plates[D]. Guang-zhou: South China University of Technology, 2021 (in Chinese) [Baidu Scholar] 

7

Zheng Xin, Shi Yuying, Chen Yubao. Heat Treatment of Me- [Baidu Scholar] 

tals[J], 2018, 43(6): 162 (in Chinese) [Baidu Scholar] 

8

Jiang S Y, Sun D, Zhang Y Q et al. Metals[J], 2018, 8(4): 217 [Baidu Scholar] 

9

Xia T, Xie Y H, Yang C et al. Materials Characterization[J], 2018, 145: 362 [Baidu Scholar] 

10

Dinh B N N, Bäker M. Metallurgical and Materials Transactions A[J], 2023, 54A: 1857 [Baidu Scholar] 

11

Du J H, Lv X D, Deng Q. Rare Metal Materials and Engineer-ing[J], 2014, 43(8): 1830 [Baidu Scholar] 

12

Ahmad N, Ghiaasiaanb R, Gradl P R et al. Materials Science & Engineering A[J], 2022, 849: 143528 [Baidu Scholar] 

13

Ran R, Wang Y, Zhang Y X et al. Journal of Materials Research and Technology[J], 2022, 20: 1216 [Baidu Scholar] 

14

Yu X F, Hu C Y, Liu H X et al. Journal of Materials Science[J], 2022, 57: 7965 [Baidu Scholar] 

15

Liu Lirong, Jin Tao, Zhao Nairen et al. Rare Metal Materials and Engineering[J], 2006, 35(5): 711 (in Chinese) [Baidu Scholar] 

16

Huang R S, Sun Y A, Xing L L et al. Materials Science & Engineering A[J], 2020, 774: 138913 [Baidu Scholar] 

17

Yadav P C, Sahu S, Subramaniam A et al. Materials Science & Engineering A[J], 2018, 715: 295 [Baidu Scholar] 

18

Zhang C, Yu L M, Wang H et al. Materials[J], 2019, 12(13): 2096 [Baidu Scholar] 

19

Ran R, Wang Y, Zhang Y X et al. Journal of Alloys and Compounds[J], 2022, 927: 166820 [Baidu Scholar] 

20

Liu A Q, Zhao F, Huang W S et al. Crystals[J], 2023, 13(6): 964 [Baidu Scholar] 

21

Zhang Y C, Yang L, Chen T Y et al. Optics and Laser Technology[J], 2017, 97: 172 [Baidu Scholar] 

22

Caliari F R, Candioto K C G, Couto A A et al. Journal of Materials Engineering and Performance[J], 2016, 25: 2307 [Baidu Scholar] 

23

Ye X J, Yang B B, Liu J T et al. Materials[J], 2022, 15(13): 4524 [Baidu Scholar] 

24

ASTM international Committee. ASTM Standard, E8/E8M- [Baidu Scholar] 

22[S], 2022 [Baidu Scholar] 

25

AMS Committee. US Patent, AMS5383[P], 2018 [Baidu Scholar] 

26

Zhu Qiang. Mesoscopic Plastic Deformation Mechanism of GH4169 Nickel-Based Superalloy Thin Sheet[D]. Harbin: Harbin Institute of Technology, 2020 (in Chinese) [Baidu Scholar] 

27

Gai Y C, Zhang R, Yang J X et al. Materials Science & Engineering A[J], 2022, 842: 143079 [Baidu Scholar] 

28

Zhou X, Li X Y, Lu K. Science[J], 2018, 360(6388): 526 [Baidu Scholar] 

29

Zhang Taiquan, Long Benfu, Lin Gaoan. Materials China[J], 2022, 41(6): 466 (in Chinese) [Baidu Scholar] 

30

Li Ting, Du Yu, Qu Lei et al. Titanium Industry Progress[J], 2022, 39(5) 22 (in Chinese) [Baidu Scholar] 

31

Sun W, Chu X, Huang J B et al. Coatings[J], 2022, 12(3): 347 [Baidu Scholar] 

32

Zhang H J, Li C, Guo Q Y et al. Materials Science & Engineering A[J], 2018, 722: 136 [Baidu Scholar] 

33

Liu B B, Han J Q, Zhao R et al. High Temperature Material Processes[J], 2016, 35(10): 989 [Baidu Scholar] 

34

Hansen N, Ralph B. Acta Metallurgica[J], 1982, 30(2): 411 [Baidu Scholar] 

35

Haouala S, Segurado J, Lorca J. Acta Materialia[J], 2018, 148: 72 [Baidu Scholar] 

36

Hall E O. Proceedings of the Physical Society, Section B[J], 1951, 64(9): 747 [Baidu Scholar] 

37

Petch N J. Journal of the Iron and Steel Institute[J], 1953, [Baidu Scholar] 

174(19): 25 [Baidu Scholar]