Research Article  Open Access
Florian Nürnberger, Mirko Schaper, FriedrichWilhelm Bach, Iryna Mozgova, Kostjantyn Kuznetsov, Anna Halikova, Olga Perederieieva, "Prediction of Continuous Cooling Diagrams for the Precision Forged Tempering Steel 50CrMo4 by Means of Artificial Neural Networks", Advances in Materials Science and Engineering, vol. 2009, Article ID 582739, 10 pages, 2009. https://doi.org/10.1155/2009/582739
Prediction of Continuous Cooling Diagrams for the Precision Forged Tempering Steel 50CrMo4 by Means of Artificial Neural Networks
Abstract
Quenching and tempering of precision forged components using their forging heat leads to reduced process energy and shortens the usual process chains. To design such a process, neither the isothermal transformation diagrams (TTT) nor the continuous cooling transformation (CCT) diagrams from literature can be used to predict microstructural transformations during quenching since the latter diagrams are significantly influenced by previous deformations and processrelated high austenitising temperatures. For this reason, deformation CCT diagrams for several tempering steels from previous works have been investigated taking into consideration the process conditions of precision forging. Within the scope of the present work, these diagrams are used as input data for predicting microstructural transformations by means of artificial neural networks. Several artificial neural network structures have been examined using the commercial software MATLAB. Predictors have been established with satisfactory capabilities for predicting CCT diagrams for different degrees of deformation within the analyzed range of data.
1. Introduction
Precision forging is a technology for the production of components with nearnetshape geometry such as automotive gears. High precision forging of the geometry enables the overall process chain to be reduced since machining before heat treatment is no longer necessary. This provides the possibility of heat treating directly from the forging heat, socalled integrated heat treatment. The latter is being thoroughly investigated within the collaborative research center CRC 489 “Process Chain for the Production of precisionforged High Performance Components” at the Leibniz University of Hannover, Germany [1, 2].
Microstructural transformations during integrated heat treatment are influenced not only by high austenitising temperatures of about but also by plastic deformations due to the forging process. Thus, neither the usual isothermal transformation diagrams nor continuous cooling transformation diagrams from literature, for example, [3, 4], nor deformation diagrams investigated for rolling processes [5, 6] are suitable for predicting microstructural transformations during tempering from such hotforming temperatures. On account of this, the deformation CCT diagrams for the tempering steels 34CrMo4 (SAE 4135), 42CrMo4 (SAE 4140), 50CrMo4 (SAE 4150), 51CrV4 (SAE 6150), and 34CrNiMo6 (1.6582) were determined in a previous work [7] according to the standards SEP 1680 [8], SEP 1681 [9], and PN68/H04500 [10], respectively. Since such physical experiments are timeconsuming and costly, the capabilities of artificial neural networks were investigated for predicting deformation CCT diagrams with regard to the particular processing in precision forging.
So far, several authors have reported on the successful predictions of CCT or TTT diagrams as a function of chemical composition; however, the influence of deformation conditions, due to precision forging, has yet to be considered. An overview of the different fields of applications for neural networks in materials science is given by [11]. Malinov et al. used a backpropagation, multilayer feedforward network to predict titanium alloy TTT diagrams from their chemical compositions [12, 13]. Calculations of the initial temperatures of bainite and martensite transformations for a huge number of steels have been carried out by GarciaMateo et al. [14]. Using multilayer perceptrons, the austenite decomposition based on a large data base of TTT and CCT diagrams was computed by Doktorowski [15]. Based on a hierarchical feedforward network using backpropagation, Wang et al. [16] have shown the influence of carbon concentration on the transformation characteristics of steels. The capabilities for designing new steels using neural networks have been demonstrated by Trzaska and Dobrzański [17–19].
2. DeformationDependent Microstructural Transformations
To physically simulate the precision forging process, specimens of the investigated melts (see Table 1) were heated to an austenitising temperature of within 30 seconds.

Following isothermal holding for 600 seconds at this temperature, the specimens were deformed by 30% and 60%, respectively (strain rate 1 ). Subsequently these were linearly cooled to room temperature using cooling rates within the range of 80 to 0.02 . As a reference, continuous cooling transformation diagrams without deformation were also determined (see Figure 1). Measurements were carried out using a dilatometer DIL 805 A/D made by the company Baehr Thermoanalyse GmbH.
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Initiating the cooling from temperatures higher than , the steels’ microstructure is austenitic or facecentredcubic (fcc). As the temperature slowly decreases below this value, austenite will then transform into bodycentredcubic (bcc) ferrite containing low concentrations of carbon. As a result of this transformation, the remaining austenite’s carbon content is enriched, and the austenite therefore transforms into bcc pearlite following completion of the ferrite formation. With increasing cooling rates, diffusion decreases due to the falling temperatures, and bainitic structures are formed. With further increase in cooling rates, the diffusionless transformation of austenite into tetragonal distorted martensite occurs. This microstructure typically features very high strength and hardness at the expense of reduced ductility. The aim of the integrated heat treatment of precision forged components, as in many other heat treatments, is to create a martensitic surface layer that will significantly increase wear resistance of highly stressed parts while the core of such components is to simultaneously possess bainitic or ferritic/pearlitic structures to increase the part’s fatigue limit. Knowledge of microstructural transformations as a function of cooling rates thus enables one to realise the aim of an efficient process design.
3. Modeling and Implementation of Artificial Neural Networks
In the following, we consider the task of predicting continuous cooling transformation diagrams as an approximation problem. For this reason, we describe each curve, which indicates the initiation or completion of a microstructural transformation, with a singlevalued functional dependence where is the number of phase transformations, is the time of initiation or completion of a microstructural transformation, is the temperature, and the degree of deformation in percent. Predicting the transformation curves can then be seen as a task of approximating functions. For the solution to this problem, splines, wavelets, and fuzzylogic methods, and so forth, can be used.
The curves for the initiation and completion of microstructural transformations are nontrivial for classical parametric approximation methods. We therefore use feedforward neural networks (FNN) as universal approximators. As shown in [20–22], artificial neural networks with twolayers—where one is a single sigmoidal hidden layer—can approximate any continuous or discontinuous function from . Leshno et al. obtained a generalization of these results for neural networks with arbitrarily limited piecewise continuous activation functions [23]. According to [23], multilayer perceptrons have the capacity to approximate any continuous function to a prescribed accuracy. Similar results were achieved by Huang et al. [24] using artificial neural networks with radialbased functions (RBF). Analysis of the approximation possibilities of artificial neural networks is a common, though challenging task. Figure 2 depicts the model of the feedforward neural network used in this work, with a single hidden layer for approximating curves for the initiation or completion of microstructural transformations for deformation dependent CCT diagrams.
A general schematic of the applied approach for solving the approximation task is given in Figure 3.
4. Data Extension
Every curve of the continuous cooling transformation diagrams, which have different percentages of deformation, has its own time interval. Usually these intervals overlap each other (see Figure 4). We used smooth padding (spd) in order to extend the data to the common argument range. The procedure spd [25] is a linear extension fit to the first two and last two values (see what follows).
For equidistant time steps , a pair of variate times and temperatures , where ; new values are calculated using the following scheme: This method works well for the approximation of equidistant signals [22]. For this purpose the function wextend from the Matlab Wavelet toolbox was used.
From physical experiments, curves were known for three degrees of deformation for each microstructural transformation of one melt. This data is to be approximated for other degrees of deformation in order to generate a generalization. Since the cooling trajectory is linear and starts at an initial temperature of , we transferred the data into a new coordinate system (), where is the cooling rate. For this purpose, we approximated every curve of a microstructural transformation with a cubic spline and determined the intersection of the spline and the cooling trajectory (see Figure 5).
Figure 6(a) shows the curves of martensite initiation temperatures for different degrees of deformation in the new coordinate system. Furthermore, is a new point for 40% deformation which was calculated according to the linear scheme (see Figure 6(b)). The values for the intermediate points; 10%, 20%, 50%, 70%, 80%, and 90% deformation were analogously calculated.
Data inputs and outputs were normalized by a mean shift followed by a decorrelation and a covariance adjustment so that the neural network can learn more accurately.
5. Training Algorithm Selection and Determination of the Optimal Neural Network Architecture
Two categories of algorithms have been used. The methods of the first are based on a heuristic analysis of the behavior of the quickest descent algorithms. This category consists of variable learning rates, backpropagation, and resilient backpropagation. The second category of fast algorithms uses methods of numerical optimization. From this category, we chose three optimization methods for network learning: PowellBeale conjugategradient method, BroydenFletcherGoldfarbShanno quasiNewton, and LevenbergMarquardt. All the algorithms mentioned work in batch mode. The algorithm LevenbergMarquardt showed a good balance between convergence rate and generalization quality. For this reason, all further studies were carried out with this algorithm. Design and learning of artificial neural networks were implemented in MATLAB using the Neural Network Toolbox.
The number of neurons in the single hidden layer was varied within the range of two to fifteen in order to determine an appropriate network architecture. Ten separate training runs were carried out, and the correlation between outputs of the net and values from training sets were calculated for all the curves of microstructural transformations. Figure 7 shows the results for the bainite initiation temperatures for the tempering steel 42CrMo4 with 30% deformation. The red polylineal curve depicts the maximum values of correlation, and the points represent the mean correlation with standard deviations calculated from ten training epochs.
This graph reveals an acceptable correlation rate of about 0.95 for nine neurons in the hidden layer. It can be seen that this correlation does not significantly increase with higher numbers of neurons. It should also be noted that the spread of data decreases at this number of neurons.
Similar results were obtained for other transformations and alloys. Thus, we used feedforward neural networks with two inputs (degree of deformation in percent and time), one hidden layer with nine nodes and one node for output (temperature). We also used individual neural networks for each of the tempering steels and for every transformation curve. Hence, to predict the overall CCT diagram of 50CrMo4, seven neural networks are necessary. In total, the training set of every single neural network consists of 1350 to 2700 triplets (time, deformation, and temperature). The learning process was terminated when the improvement of the mean square error after 100 consecutive epochs fell below 0.01. The best net was then selected from the ten different trained networks.
6. Results
Figure 8 depicts the dynamics of microstructural transformations for the steel 50CrMo4. In the graphs on the left of this figure, the black curves are the network outputs, and the red curves depict the physically measured diagrams. In the graphs on the right, the transformation diagrams for unknown degrees of deformation are shown.
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Figure 9 shows the correlation between measured diagrams and the net outputs.
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Figures 10, 11, 12, and 13 demonstrate the neural networks’ performances for other types of investigated steels. Results show that the artificial neural networks used here are capable of predicting the microstructural transformations within the range of the investigated degrees of deformation.
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For most of the CCT diagrams, a high correlation coefficient can be achieved between the networks’ output data and the experimental data.
An extrapolation beyond strains of 60% is possible; however, with further increases of deformation, the transformation lines depicting the completion of ferrite and the initiation of pearlite then begin to cross each other. This is due to the approach used where every net represents one transformation curve of a CCT diagram separated from the others. Interactions between the nets are not considered and, as a result, the overlaying effect of the curves may be observed for higher (80%) degrees of deformation.
7. Further Research
(1) The next stage of our research will be concerned with the prediction of microstructural transformations of tempering steels with lower austenitising temperatures. This will increase the data base for numerically simulating the processes of precision forging and integrated heat treatment.
Furthermore, artificial neural networks will be used for the prediction of continuous cooling transformation diagrams, not only for specified strains but also for strain rates. Investigations of the CCT diagrams’ strain rate dependence for the tempering steel 42CrMo4 are also planned for the future. These experiments may require changes in the architecture of the neural networks used.
(2) In addition to this, a certain interest lies in an alternative data handling scheme for the CCT diagrams’ transformation curves to reduce the amount of data used in the training set. Therefore an approach similar to [13] will be implemented. However, we propose an application of the curves’ critical points (extrema, inflections, and endpoints) of microstructural transformations.
(3) In order to avoid overfitting effects, we propose applying smoothness criteria to the predicted transformation curves. This should increase the generalization properties of the networks.
(4) The method of data extension of the current work is not applicable for processes with nonlinear cooling. For a universal approach of the diagrams generalization, it is necessary to develop an appropriate method of data extension based on other principles. Such a principle might be an algebraic method suitable for smoothed nonlinear approximated functions.
8. Summary
Curves in CCT diagrams for the initiation and the completion of microstructural transformations were used as training sets for artificial neural networks. Diagrams with different deformations were utilized with regard to the process conditions of precision forging with integrated heat treatment. Predictions could be made within the range of the investigated deformation conditions. An extrapolation beyond deformations of 80% leads to inaccuracies.
Acknowledgment
The authors thank the German Research Foundation for the financial support of the research work within the collaborative research center CRC 489.
References
 B.A. Behrens, E. Doege, S. Reinsch, K. Telkamp, H. Daehndel, and A. Specker, “Precision forging processes for highduty automotive components,” Journal of Materials Processing Technology, vol. 185, no. 1–3, pp. 139–146, 2007. View at: Publisher Site  Google Scholar
 M. Bernard, M. van Well, W. Reimche, and Fr.W. Bach, “Randzonenhärtung von Vergütungsstahl mit Sprühabschreckung—Einfluss der Düsenanordnung auf das Härteergebnis und zerstörungsfreie Bestimmung der Randzonenhärte mittels HarmonischenAnalyse von Wirbelstromsignalen,” HärtereiTechnische Mitteilungen, vol. 60, no. 3, pp. 150–157, 2005. View at: Google Scholar
 F. Wever and A. Rose, Atlas zur Wärmebehandlung der Stähle. Vol. 1, Verein Deutscher Eisenhüttenleute, Stahleisen, Düsseldorf, Germany, 1961.
 G. F. Vander Voort, Atlas of TimeTemperature Diagrams for Irons and Steels, ASM International, Metals Park, Ohio, USA, 1991.
 A. Weise, Entwicklung von Gefüge und Eigenspannungen bei der thermomechanischen Behandlung des Stahls 42CrMo4., dissertation, Technische Universität Chemnitz, Chemnitz, Germany, 1998.
 R. Kaspar, U. Lotter, and C. Biegus, “Influence of thermomechanical treatment on the transformation behaviour of steels,” Steel Research, vol. 65, no. 6, pp. 242–247, 1994. View at: Google Scholar
 K. Kerber and Fr.W. Bach, Eds., “Process chain for the production of precisionforged high performance components,” Work Report and Renewal Proposal 200920102011, Collaborative Research Centre 489, July 2008. View at: Google Scholar
 StahlEisenPrüfblatt. 168061, Aufstellung von ZeitTemperaturUmwandlungsschaubildern für Eisenlegierungen, STAHLEISENPrüfblätter (SEP) des Vereins Deutscher Eisenhüttenleute, 3rd edition, 1990.
 StahlEisenPrüfblatt. 1681, Guidelines for preparation, execution and evaluation of dilatometric transformation test on iron alloys, STAHLEISENPrüfblätter (SEP) des Vereins Deutscher Eisenhüttenleute, 2nd edition, 1998.
 PN68/H04500, “Badania dylatometryczne metali i ich stopów,” 1968. View at: Google Scholar
 H. K. D. H. Bhadeshia, “Neural networks in materials science,” ISIJ International, vol. 39, no. 10, pp. 966–979, 1999. View at: Publisher Site  Google Scholar
 S. Malinov and W. Sha, “Software products for modelling and simulation in materials science,” Computational Materials Science, vol. 28, no. 2, pp. 179–198, 2003. View at: Publisher Site  Google Scholar
 S. Malinov, W. Sha, and Z. Guo, “Application of artificial neural network for prediction of timetemperaturetransformation diagrams in titanium alloys,” Materials Science and Engineering A, vol. 283, no. 12, pp. 1–10, 2000. View at: Publisher Site  Google Scholar
 C. GarciaMateo, C. Capdevila, F. Garcia Caballero, and C. García de de Andrés, “Artificial neural network modeling for the prediction of critical transformation temperatures in steels,” Journal of Materials Science, vol. 42, no. 14, pp. 5391–5397, 2007. View at: Publisher Site  Google Scholar
 A. Doktorowski, Datenbasierte Modellierung der Gefügebildung bei der gamma/alphaUmwandlung von Stählen, dissertation, TU Bergakademie, Freiberg, Germany, 2002.
 J. Wang, P. J. van der Wolk, and S. van der Zwaag, “Effects of carbon concentration and cooling rate on continuous cooling transformations predicted by artificial neural network,” ISIJ International, vol. 39, no. 10, pp. 1038–1046, 1999. View at: Publisher Site  Google Scholar
 J. Trzaska and L. A. Dobrzański, “Modelling of CCT diagrams for engineering and constructional steels,” Journal of Materials Processing Technology, vol. 192193, pp. 504–510, 2007. View at: Publisher Site  Google Scholar
 L. A. Dobrzański and J. Trzaska, “Application of neural networks to forecasting the CCT diagrams,” Journal of Materials Processing Technology, vol. 157158, pp. 107–113, 2004. View at: Publisher Site  Google Scholar
 L. A. Dobrzański and J. Trzaska, “Application of neural networks for the prediction of continuous cooling transformation diagrams,” Computational Materials Science, vol. 30, no. 34, pp. 251–259, 2004. View at: Publisher Site  Google Scholar
 K. Hornik, M. Stinchcombe, and H. White, “Multilayer feedforward networks are universal approximators,” Neural Networks, vol. 2, no. 5, pp. 359–366, 1989. View at: Publisher Site  Google Scholar
 K. Hornik, “Approximation capabilities of multilayer feedforward networks,” Neural Networks, vol. 4, no. 2, pp. 251–257, 1991. View at: Publisher Site  Google Scholar
 G. Cybenko, “Approximation by superpositions of a sigmoidal function,” Mathematics of Control, Signals, and Systems, vol. 2, no. 4, pp. 303–314, 1989. View at: Publisher Site  Google Scholar
 M. Leshno, V. Ya. Lin, A. Pinkus, and S. Schocken, “Multilayer feedforward networks with a nonpolynomial activation function can approximate any function,” Neural Networks, vol. 6, no. 6, pp. 861–867, 1993. View at: Publisher Site  Google Scholar
 G.B. Huang, L. Chen, and C.K. Siew, “Universal approximation using incremental constructive feedforward networks with random hidden nodes,” IEEE Transactions on Neural Networks, vol. 17, no. 4, pp. 879–892, 2006. View at: Publisher Site  Google Scholar
 G. Strang and T. Nguyen, Wavelets and Filter Banks, WellesleyCambridge Press, Wellesley, Mass, USA, 1996.
Copyright
Copyright © 2009 Florian Nürnberger et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.