Elsevier

Materials & Design

Volume 59, July 2014, Pages 115-123
Materials & Design

Constitutive models for high-temperature flow behaviors of a Ni-based superalloy

https://doi.org/10.1016/j.matdes.2014.02.041Get rights and content

Highlights

  • The hot deformation behavior of a typical Ni-based superalloy is investigated.

  • New phenomenological constitutive models are developed.

  • The coupled effects of deformation parameters on material constants are considered.

  • The proposed constitutive models correlate well with the experimental results.

Abstract

The high-temperature deformation behaviors of a typical Ni-based superalloy are investigated by hot compression tests under the strain rate of 0.001–1 s−1and temperature of 920–1040 °C. The experimental results show that the deformation behaviors of the studied superalloy are significantly affected by the deformation temperature, strain rate and strain. The flow stress increases with the increase of strain rate or the decrease of deformation temperature. The flow stress firstly increases with the strain to a peak value, showing the obvious work hardening behaviors. Then, the stress decreases with the further straining, indicating the dynamic flow softening behaviors. Considering the coupled effects of deformation temperature, strain rate and strain on the hot deformation behaviors of the studied Ni-based superalloy, the phenomenological constitutive models are established to describe the work hardening-dynamic recovery and dynamic softening behaviors. In the established models, the material constants are expressed as functions of the Zener–Hollomon parameter. The established constitutive models can give good correlations with the experimental results, which confirm an accurate and precise estimation of the flow stress for the studied Ni-based superalloy.

Introduction

During the hot forming process, the high-temperature deformation behaviors of metals and alloys are very complex [1], [2]. On the one hand, the hot deformation behaviors are significantly influenced by the thermo-mechanical parameters, such as deformation temperature, strain rate and strain [3], [4], [5]. On the other hand, the working hardening [6], [7], dynamic recovery and recrystallization [8], [9] happen during the hot deformation, which result in the complex microstructural evolution and simultaneously affect the plastic deformation behaviors of metals and alloys [10], [11]. Therefore, understandings of the high-temperature deformation behaviors of metals and alloys are very important for designers of hot forming processes to improve the mechanical properties of products [12], [13].

In order to obtain the optimal hot forming processing parameters of metals and alloys, considerable efforts have been made on their high-temperature deformation behaviors by a series of experiments, such as hot compression, tension and torsion tests [1], [14]. Based on the experimental results, some constitutive models are proposed to accurately describe the plastic deformation characteristics of metals and alloys, and these constitutive models are critical for the correct numerical simulation and the reasonable optimization of hot forming process [1], [15]. Based on the recent researches, Lin and Chen [1] presented a critical review on constitutive descriptions for metals and alloys under hot working, and they divided the constitutive models into three categories, including the phenomenological models [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35], [36], [37], [38], [39], [40], [41], [42], [43], [44], [45], [46], [47], [48], physically-based models [49], [50], [51], [52], [53] and artificial neural network models [54], [55], [56], [57], [58]. Considering the effects of strain on material constants, Lin et al. [16] proposed a revised hyperbolic sine constitutive equation to describe the high-temperature deformation behaviors of 42CrMo steel. Also, some similar phenomenological models were proposed to predict the plastic deformation behaviors of the commercial purity aluminum [17] and aluminum alloys (2124-T851 aluminum alloy [18], cast A356 aluminum alloy [19], spray-deposited Al–Zn–Mg–Cu alloy [20], Al–Zn–Mg–Zr alloy [21], Al–3Cu–0.5Sc alloy [22], and 6061 aluminum alloy [23]), magnesium alloys (AZ61 magnesium alloy [24] and as-cast AZ80 magnesium alloy [25]), steels (Aermet 100 steel [26], B1500HS steel [27], T24 ferritic steel [28], as-cast 21Cr economical duplex stainless steel [29], GCr15 steel [30], A286 iron-base superalloy [31], Sanicro-28 super-austenitic stainless steel [32], and 9Cr–1Mo steel [33], [34]), commercially pure titanium (CP–Ti) [35] and Ti-based alloys (Ti–6Al–4V alloy [36] and Ti–6Al–7Nb alloy [37]). On analysis of the test data, Cui et al. [38] proposed the cubic piecewise functions of strain to ensure the high precision of Arrhenius-type hyperbolic sine model. Guo et al. [39] established the modified Voce type model and Arrhenius-type equation to describe the hot deformation behavior of 3003 aluminum alloy. Considering the coupled effects of strain, strain rate and forming temperature on the hot deformation behaviors of Al–Zn–Mg–Cu and Al–Cu–Mg alloys, Lin et al. [40], [41], [42], [43] proposed new phenomenological constitutive models to describe the thermo-viscoplastic response of Al–Zn–Mg–Cu and Al–Cu–Mg alloys under hot working condition. In their proposed models, the material constants are presented as functions of strain rate, forming temperature and strain. Also, some modified Johnson–Cook model were established to predict the hot deformation behaviors of 20CrMo alloy steel [44], 42CrMo steel [45], boron steel sheet [46], Ti–6Al–4V alloy [47], and titanium matrix composites [48]. Based on the classical stress–dislocation relation and the kinetics of dynamic recrystallization, the physically-based constitutive equations were established to describe the work hardening–dynamic recovery and dynamic recrystallization behaviors of 42CrMo steel [49], typical superalloys [50], [51], as-cast 21Cr economical duplex stainless steel [52], and 55SiMnMo bainite steel [53]. In addition, a number of researchers developed some artificial neural network constitutive models to predict the high-temperature flow behaviors of 42CrMo steel [54], as-cast Ti–6Al–2Zr–1Mo–1V alloy [55], A356 aluminum alloy [56], as-cast Ti60 titanium alloy [57], and 12Cr3WV steel [58].

Due to excellent high temperature characteristics, good fatigue and corrosion resistance, Ni-based superalloys are widely applied in aerospace and energy industries [50], [51], [59]. The comprehensive investigations of the high-temperature deformation behaviors are particularly important due to the narrow deformation temperature range and large deformation resistance of Ni-based superalloys [60]. Wang et al. [61] studied the effects of δ phase on DRX behaviors of GH4169 alloy during hot compression deformation, and found that the evolution of δ phase is sensitive to the deformation temperature and strain rate. Lin et al. [62], [63] studied the hot tensile deformation behaviors and fracture characteristics of a typical Ni-based superalloy (GH4169), and found that the typical DRX characteristics appear under relatively high deformation temperatures (1010 and 1040 °C). Also, δ phase (Ni3Nb) can cause the obvious work hardening at the beginning of hot deformation, and then accelerates the flow softening by promoting the dynamic recrystallization with further straining. With the increase of initial δ phase, the strain rate sensitivity coefficient decreases firstly and then increases. Meanwhile, the increase of initial δ phase increases the density of nucleus for the formation of microvoids, and promotes the nucleation and coalescence of microvoids. Wen et al. [64] established the processing map to optimize the hot working processing for a typical Ni-based superalloy (GH4169), and found that the changes of instability domains may be related to the evolution of δ phase during hot deformation. Wang et al. [66] found that the existence of δ phase can lead to an increase of strain rate sensitivity exponent and activation energy of GH4169 superalloy. Additionally, the high-temperature deformation behaviors of Ni-based superalloys were also studied by Yao et al. [66], Sun et al. [67], Etaati et al. [68], Ning et al. [69], etc. Although some studies have been conducted to investigate the high-temperature deformation behaviors of Ni-based superalloys, the constitutive models are still not advanced enough to account for the whole complex dynamic mechanisms.

In this study, the high-temperature deformation behaviors of a typical Ni-based superalloy with δ phase (Ni3Nb) are investigated by hot compression tests under the wide ranges of deformation temperature and strain rate. The phenomenological constitutive models are established to describe the coupled effects of deformation temperature, strain rate, and strain on the high-temperature deformation behaviors of the studied Ni-based superalloy.

Section snippets

Experiments and results

A typical Ni-based superalloy with compositions (wt%) of 52.82Ni–18.96Cr–5.23Nb–3.01Mo–1.00Ti–0.59Al–0.01Co–0.03C–(bal.) Fe was used in this study. The metastable body-centered tetragonal coherent precipitate γ″ phase (Ni3Nb) and the face-centered cubic coherent precipitate γ′ phase (Ni3Al) are the strengthening phases. Furthermore, γ is the major strengthening phase which may transform to δ phase (Ni3Nb) in equilibrium [60], [61], [62], [63], [64], [65]. Cylindrical specimens were machined

Constitutive model to describe work hardening and dynamic recovery behaviors

Generally, the flow stress during the work hardening–dynamic recovery period can be predicted by the following equation [70].σσp=εεpexp1-εεpc1where σp is the peak stress (MPa), ɛp is the peak strain, c1 is the material constant.

From Eq. (1), it can be known that the peak stress and peak strain should be firstly obtained before predicting the flow stress. Generally, the peak stress can be evaluated through the following hyperbolic-sine Arrhenius equation:ε̇=AF(σp)exp(-Q/RT)where,F(σp)=σpnασp<0.8

Effects of strain on material constant C2

In order to guarantee the high prediction accuracy of the developed constitutive model during the dynamic flow softening stage, the method for evaluating the optimal value of material constant c2 should be further investigated. From Eq. (15) and Fig. 9, it can be found that the material constant c2 is significantly affected by the thermo-mechanical parameters. In the previous analysis, the strain of 0.5 and the corresponding flow stress (σ) are used to evaluate the values of material constant c2

Conclusions

In this paper, the high-temperature deformation behaviors of a typical Ni-based superalloy are investigated by the compression test over practical ranges of temperature and strain rate. Based on the experimental data, phenomenological constitutive models are established to describe the work hardening–dynamic recovery and dynamic flow softening behaviors of the studied Ni-based superalloy. In the developed models, the coupled effects of deformation temperature and strain rate on the material

Acknowledgements

This work was supported by National Natural Science Foundation of China (Grant No. 51375502), 973 program (No. 2013CB035801), Key Laboratory of Efficient & Clean Energy Utilization, College of Hunan Province (No. 2014NGQ001), and Sheng-hua Yu-ying Program of Central South University.

References (71)

  • Y.C. Lin et al.

    Constitutive modeling for elevated temperature flow behavior of 42CrMo steel

    Comp Mater Sci

    (2008)
  • H.R. Rezaei Ashtiani et al.

    Constitutive equations for elevated temperature flow behavior of commercial purity aluminum

    Mater Sci Eng A

    (2012)
  • Y.C. Lin et al.

    Constitutive descriptions for hot compressed 2124–T851 aluminum alloy over a wide range of temperature and strain rate

    Comp Mater Sci

    (2010)
  • N. Haghdadi et al.

    The flow behavior modeling of cast A356 aluminum alloy at elevated temperatures considering the effect of strain

    Mater Sci Eng A

    (2012)
  • Y.D. Jia et al.

    Hot deformation behavior of spray-deposited Al–Zn–Mg–Cu alloy

    Mater Des

    (2014)
  • G.F. Xu et al.

    Constitutive relationship for high temperature deformation of Al–3Cu–05Sc alloy

    T Nonferr Metal Soc

    (2013)
  • C.H. Liao et al.

    Strain-dependent constitutive analysis of extruded AZ61 Mg alloy under hot compression

    Mater Sci Eng A

    (2013)
  • G.L. Ji et al.

    A comparative study on arrhenius-type constitutive model and artificial neural network model to predict high-temperature deformation behaviour in Aermet100 steel

    Mater Sci Eng A

    (2011)
  • H.P. Li et al.

    Constitutive relationships of hot stamping boron steel B1500HS based on the modified arrhenius and Johnson–Cook model

    Mater Sci Eng A

    (2013)
  • H.Y. Li et al.

    Constitutive modeling for hot deformation behavior of T24 ferritic steel

    Comp Mater Sci

    (2012)
  • D.N. Zou et al.

    Deformation characteristic and prediction of flow stress for as-cast 21Cr economical duplex stainless steel under hot compression

    Mater Des

    (2013)
  • F. Yin et al.

    Constitutive modeling for flow behavior of GCr15 steel under hot compression experiments

    Mater Des

    (2013)
  • H. Dehghan et al.

    On the constitutive modeling and microstructural evolution of hot compressed A286 iron-base superalloy

    J Alloys Compd

    (2013)
  • A. Mirzaei et al.

    Constitutive description of high temperature flow behavior of Sanicro-28 super-austenitic stainless steel

    Mater Sci Eng A

    (2014)
  • D. Samantaray et al.

    Constitutive analysis to predict high-temperature flow stress in modified 9Cr–1Mo (P91) steel

    Mater Des

    (2010)
  • J. Peng et al.

    An improved constitutive description of tensile behavior for CP–Ti at ambient and intermediate temperatures

    Mater Des

    (2013)
  • X. Peng et al.

    Constitutive equations for high temperature flow stress of TC4-DT alloy incorporating strain, strain rate and temperature

    Mater Des

    (2013)
  • F. Pilehva et al.

    Flow behavior modeling of a Ti–6Al–7Nb biomedical alloy during manufacturing at elevated temperatures

    Mater Des

    (2013)
  • J.H. Guo et al.

    Modeling the hot deformation behavior of Al alloy 3003

    J Alloys Compd

    (2013)
  • Y.C. Lin et al.

    A new phenomenological constitutive model for hot tensile deformation behaviour of a typical Al–Cu–Mg alloy

    Mater Des

    (2013)
  • Y.C. Lin et al.

    A phenomenological constitutive model for high temperature flow stress prediction of Al–Cu–Mg alloy

    Mater Sci Eng A

    (2012)
  • A. He et al.

    A comparative study on Johnson–Cook, modified Johnson–Cook and Arrhenius-type constitutive models to predict the high temperature flow stress in 20CrMo alloy steel

    Mater Des

    (2013)
  • Y.C. Lin et al.

    A combined Johnson–Cook and Zerilli–Armstrong model for hot compressed typical high-strength alloy steel

    Comp Mater Sci

    (2010)
  • N. Kotkunde et al.

    Microstructure study and constitutive modeling of Ti–6Al–4V alloy at elevated temperatures

    Mater Des

    (2014)
  • W.D. Song et al.

    A modified Johnson–Cook model for titanium matrix composites reinforced with titanium carbide particles at elevated temperatures

    Mater Sci Eng A

    (2013)
  • Cited by (0)

    View full text