Three-dimensional thermo-elastic–plastic finite element modeling of quenching process of plain-carbon steel in couple with phase transformation
Introduction
Quenching is one of manufacturing processes to improve mechanical properties of mechanical components for automobiles, aircrafts, and machines subjected to high load and impact. The cooling rate and temperature variation within the steel during the quenching process results in microstructural evolution and have a significant effect on the final shape and dimension of mechanical parts. Effective control of such a phase transformation can lead to make these steel parts with better mechanical properties, microstructures, and final dimensional accuracies required. With increasing use of the finite element (FE) analysis as an effective controlling tool of phase transformation, mathematical modeling of phase transformation has been important for accurately analyzing the quenching process.
Johnson and Mehl [1] and Avrami [2], [3] proposed an analytical equation for diffusional transformation under the isothermal condition. Together with this equation, Scheil's additive rule [4] has been widely adopted to describe a non-isothermal cooling process like quenching by subdividing the cooling curve into various small isothermal steps. For handling a diffusionless transformation like an austenite–martensite transformation, Koistinen and Marburger [5] proposed an empirical model which can be used to predict the volume fraction of the martensite after rapid quenching. After these pioneering works, many investigations by Inoue and Raniecki [6], Rammerstorfer et al. [7], Fernandes et al. [8], Denis et al. [9], Agarwal and Brimacombe [10], Nagasaka et al. [11], Hawbolt et al. [12], Sjöström [13], and Kang and Im [14] have been made for modeling of the phase transformation to improve the accuracy of numerical simulations.
Due to the thermal strain resulted from the temperature variation during the quenching process, a dimensional change of the steel specimen takes place. However, it was well known that additional strains such as phase transformation strain and transformation-induced plasticity (TRIP) due to the difference and generation rate in the volume fraction of each phase and applied stress also have the significant effect on the final geometry of the mechanical part. Especially, microstructural plastic behavior, that is, TRIP occurs in the weaker phase, even though the external load lower than the yield strength of the weaker phase is applied. Some researchers such as Greenwood and Johnson [15], Leblond et al. [16], [17], Taleb et al. [18], [19], Fischer et al. [20], and Coret et al. [21] have analyzed this kind of microstructural transformation induced plasticity obtained from experimental or theoretical approaches in order to consider its effect in FE simulations.
In this study, the numerical phase transformation models such as Johnson–Mehl–Avrami–Kolmogorov (JMAK) model for the diffusional transformation and Koistinen and Marburger (KM) model for the diffusionless transformation were employed to investigate a dimensional change during the quenching process. During phase transformation, the volume fraction of each phase transformed and stress applied lead to the microstructural plasticity in the weaker phase as mentioned earlier. In order to consider the microstructural plasticity in the weaker phase according to the volume fraction of each phase transformed and stress applied during the quenching process, the numerical model proposed by Leblond et al. [16], [17] and modified by Taleb et al. [18], [19] was employed. Also, generation of the latent heat released due to the phase transformation inducing the temperature increase was considered in this work.
Even though the constitutive equation was introduced in many papers, most of these papers have offered no or a little information in the derivation procedure of the constitutive equation including the phase transformation effect. Using the constitutive equation in couple with the phase transformation, a FE program was developed and used to predict distributions of the temperature, volume fraction of each phase, and stress and dimensional change of the cylindrical specimen, shaft with key groove, and cam-lobe made of carbon steel. From this study, it was found out that numerically obtained values such as temperature history and stress distribution were in good agreement with the data available in the literature for the cylindrical carbon steel specimen and three-dimensional thermo-elastic–plastic FE program developed can be a useful tool in investigating design parameters for the quenching process.
Section snippets
Phase transformation model
Quenching results in phase change of the steel part according to the temperature variation. Various microstructures present differently according to the cooling rate, temperature, and carbon content. In this study, diffusional and diffusionless transformation models were used to predict the volume fraction of each phase such as austenite, ferrite, pearlite, and martensite obtained during the phase transformation.
The schematic time–temperature–transformation (TTT) diagram of eutectoid steel is
Thermo-elastic–plastic constitutive equation coupled with the phase transformation
Since large temperature variation and phase transformation take place during the quenching process, the steel part generally undergoes the plastic deformation. Thus, coupling among the temperature, phase transformation, mechanical behavior, and chemical composition should be considered in the finite element formulation as shown in Fig. 2. According to the cooling rate and temperature variation, different kinds of phases are generated and their volume fractions become different at every point of
Thermal formulation
During the continuous cooling process, the governing equation for the heat transfer analysis coupling with the phase transformation can be expressed as energy equilibrium with boundary conditions.Here, T, k, ρ, Cp, and are the temperature, thermal conductivity, density, specific heat, and heat generation rate in that order. Thermal properties such as k, ρ, and Cp are dependent on the carbon content and
Simulation results
In order to validate the thermo-elastic–plastic FE program coupled with the phase transformation developed in this study, the predicted temperature history and stress distribution were compared to the experimental data available in the literature for the cylindrical eutectoid steel. Thermal properties such as the thermal conductivity, density, specific heat, and thermal expansion coefficient of the material were dependent on the carbon content and temperature. For this, the thermal
Conclusions
This study discussed the FE investigation of the quenching process which is commonly applied to improve the mechanical properties such as strength, hardness, and wear/fatigue resistances. The detail procedure of the thermo-elastic–plastic FE formulation considering the phase transformation during the process was made based on JMAK and KM equations for the diffusional and diffusionless transformations, respectively, to predict the temperature variation, volume fraction of each phase transformed,
Acknowledgments
The authors wish to thank the Grant of National Research Laboratory Program of the Ministry of Science and Technology through the Korea Engineering Science and Engineering Foundation and the technical support of Dr. Il-Heon Son, Messrs. Ho-Won Lee, Hyun-Cheol Lee and Young-Gwan Jin for preparing the manuscript without which this work was not possible.
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