- About this Journal ·
- Abstracting and Indexing ·
- Aims and Scope ·
- Article Processing Charges ·
- Articles in Press ·
- Author Guidelines ·
- Bibliographic Information ·
- Citations to this Journal ·
- Contact Information ·
- Editorial Board ·
- Editorial Workflow ·
- Free eTOC Alerts ·
- Publication Ethics ·
- Reviewers Acknowledgment ·
- Submit a Manuscript ·
- Subscription Information ·
- Table of Contents

International Journal of Aerospace Engineering

Volume 2011 (2011), Article ID 874375, 7 pages

http://dx.doi.org/10.1155/2011/874375

## Study on Ductility of Ti Aluminide Using Artificial Neural Network

^{1}Materials and Mechanical Entity, Vikram Sarabhai Space Center, Trivandrum 695022, India^{2}National Institute of Hydrology, Roorkee 247667, India^{3}Departement of Metallurgical and Materials Engineering, Indian Institute of Technology, Roorkee 247667, India

Received 25 March 2011; Revised 7 August 2011; Accepted 16 August 2011

Academic Editor: Kenneth M. Sobel

Copyright © 2011 R. K. Gupta 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.

#### Abstract

Improvement of ductility at room temperature has been a major concern on processing and application of Ti aluminides over the years. Modifications in alloy chemistry of binary alloy (Ti48 Al) and processing conditions were suggested through experimental studies with limited success. Using the reported data, the present paper aims to optimize the experimental conditions through computational modeling using artificial neural network (ANN). Ductility database were prepared, and three parameters, namely, alloy type, grain size, and heat treatment cycle were selected for modeling. Additionally, ductility data were generated from the literature for training and validation of models on the basis of linearity and considering the primary effect of these three parameters. Model was trained and tested for three different datasets drawn from the generated data. Possibility of improving ductility by more than 5% is observed for multicomponent alloy with grain size of 10–50 *μ*m following a multistep heat treatment cycle.

#### 1. Introduction

Ti aluminide has been an important aerospace material due to its high temperature properties and lower density as compared to superalloys. The ordered structure of aluminides that make them useful for high temperature applications makes them brittle at ambient temperature [1–3]. Therefore, inspite of having good properties, the usefulness of these alloys has been limited to some specific applications only. Room temperature tensile ductility is maximum (~1.5%) at around Ti-48Al (at%) aluminum, which is insufficient for further processing and applications. Hence, development of Ti aluminides has centered around Ti-48Al (at%) composition. It belongs to the (TiAl) plus (Ti_{3}Al) region of the phase diagram [4–6]. Various methods like alloy addition, controlled processing, heat treatment and so forth, are applied to get optimum combination of strength and ductility. Alloying additions in the range of 1 to 10 at% is studied with Cr, V, Mn, Nb, Ta, W, and Mo [6]. The alloying additions of V, Mn, Ni, and Cr in the range of 2–4 at% have shown enhancement in ductility of the alloy. Effect of microstructure on the mechanical properties was studied and duplex structure with fine grain size has been reported to be optimum for superior strength and ductility [4, 7–9]. To obtain desired microstructures and mechanical properties, the effect of several heat treatment cycles on aluminides has been studied at different temperatures and with varying cooling rates [9–16] and marginal improvement in ductility was reported. In this way several studies have been conducted with limited success in improving ductility of the alloy. However, experimental studies are expensive due to the use of high purity alloying elements and processing under controlled atmosphere. Here, theoretical models are very useful for optimization of process parameters. Experimentation with such optimized parameters shall minimize the number of experimental attempts and could lead to achieve desired ductility.

During the last decade, there has been an increased interest in applying new emerging theoretical techniques such as fuzzy inference system (FIS) and artificial neural network (ANN) for optimization-related problems [17–20]. These are the most common data driven models. These models intend to describe the nonlinear relationship between input (antecedent) and output (consequence) to the real system. In the present paper ductility of Ti aluminide is studied through ANN modeling.

Though ANN modeling is a relatively new technique, there has been an increasing interest in applying this technique in recent times in different fields of material science [21–25]. The basic advantage of employing ANN is that it does not require any external manifestation of parametric relationship. It learns from examples and recognizes patterns in a series of input and output values without any prior assumptions about their nature and interrelations. It consists of a number of interconnected computational elements called neurons. The neurons are arranged in three types of layers—input, hidden, and output. Information processing in a neural network occurs through interaction between these neurons. There is a wide range of ANN architectures [26], among which the three layer (input, hidden, and output) feed-forward architecture is used in the present work. It consists of layers of neurons, with each layer being fully connected to the preceding layer by interconnection weights (). A neural network representation with two inputs and is shown in Figure 1. Each of these input variables is associated with 3 neurons as decided after trial and error. The computations were performed in 5 levels (L1 through L5, which consists of 1 output, 1 input, and 3 hidden layers). Network with three hidden layers (Figure 1) was attempted but the error increased as well as computation time was more, therefore, it was restricted for single hidden layer network. The directions marked in Figure 1 imply the flow of information. The contribution of each rule toward the model output is computed in the fourth level (L4). Overall output of the model is computed at fifth level (L5) by combining the signals received from the previous level. Subsequently models were validated with the literature database using three important indices, that is root mean square error (RMSE), regression coefficient () and the model efficiency criterion of Nash and Sutcliffe [27].

#### 2. Ductility Parameters and Data for Model

Ductility values were consolidated from the literature [5–11, 28–33], and three important parameters, namly alloy chemistry, grain size, and heat treatment cycles were identified, which have major influence in ductility of the alloy. Alloy chemistry, grain size, and heat treatment cycles have important influence on ductility. For example, as content of aluminium increases in the alloy, ductility decreases. Binary alloy has limited ductility, and addition of ternary and quaternary alloying elements improves the ductility of the alloy. Similarly, finer grain size improves the ductility of the alloy through microstructural refinement avoiding segregation of impurities. Heat treatment cycle results in formation of desired phases, which has higher ductility.

Collected data were categorized in 2 types of alloy (2 components and multicomponent alloy), 4 types of grain sizes, and 7 types of heat treatment cycles with certain assumptions (Table 1). Ductility values collected from the literature with various categories of parameters are presented in Table 2, which were further interpolated according to trends in literature values and following the linearity basis. In this way 56 ductility data combinations were generated, in the same order as given in Table 2, for each alloy type and for each grain size in different heat treatment conditions. These values are termed as observed values. Total number of observed values is 56, in which dataset 1 is selected just by picking first 40 values for training and last 16 values for testing. In data set 2, first 10 values from 21 to 30 and from 41 to 50 values have been taken for training and the rest for testing. Data set 3 has picked randomly 43 values from each category for training data and similarly 30 values for testing data. Few data have been considered in both training and testing sets. Data selection for different data set has been given in Table 3. In the present paper, data extracted from the literature are written as observed data.

#### 3. Model Development

Three variables, namly composition, grain size, and heat treatment cycles were considered as antecedent and ductility as consequence during the modeling.

##### 3.1. Formulation of ANN Model

Depending on the data availability, total data has been subdivided into training and testing sets as mentioned in previous section. The number of hidden levels, the number of input and output nodes and the number of nodes in the hidden levels were decided by trial and error method. A schematic diagram of a typical th node is displayed in Figure 2. The inputs to such a node come from system variables or outputs of the other nodes, depending on the levels that the node is located in. These inputs form an input vector . The sequence of weights leading to the node form a weight vector , where represents the connection weight from the ith node in the preceding level to this node.

The output of node, that is, , is obtained by computing the value of function with respect to the inner product of vector and as where is the threshold value, also called the bias, associated with this node. The function is called an activation function. It can be determined with the response of a node with the total number of received input signals.

For selecting number of neurons, models with 3, 4, and 5 number of neurons were tried and RMS error were computed. Although it does not have much difference in RMS error for each type but least error was seen (Figure 3) for 3 neurons in all the cases. Also, with increasing number of neurons becomes more complex therefore three neurons were used in all the analysis.

##### 3.2. Training (Learning) of ANN Model

To generate an output vector as close to the target vector, training process is employed. A network trains by adjusting the weights that link its neurons so as to find optimal weight matrices and bias vectors that minimize a predetermined error function. It is written as where = component of the desired output; = corresponding ANN output; = number of training parameters; = number of output nodes.

A training data set is used to train the network or to determine the interconnection weights such that the response of the ANN clearly matches the observed behavior of the process being modeled. During training, typically mean square error (MSE) is monitored to find the optimal termination point for training. After training, the network is tested with the testing data set to determine how accurately the network can simulate the input-output relationship. If the performance of the ANN on the test data is satisfactory, the network is considered trained, weights are frozen and are used in actual application.

Different network processes have been tried with different sets of training and transfer functions to get optimum solutions. The network, which gives the optimum results with minimum error, could be frozen for testing or validation. The final frozen network contains “trainbr” as transfer function and “tansig” and “purelin” as training functions, as this set of combination with 3 neurons gives the optimum results. Accordingly, “tansig” and “purelin” training functions and “trainbr” transfer function have been fixed with trial and error for entire modeling. Number of experiments was carried out with all three data sets. The required ANN models (best ANN architecture) have been selected based on the training and performance checking of the models. Final architecture for all datasets is shown in Table 4.

##### 3.3. Performance Indices

All models developed with different sets of data were tested and computed ductility was compared with literature-based ductility by means of *RMSE* (*root mean square error*) and *R ^{2}* (

*regression coefficient*) statistics. The models performances were also evaluated by using Nash-Sutcliffe criterion [27] of

*percent variance (VAREX*) as given below: where is number of observations; is observed value at time (m

^{3}/s); is mean of the observed values (m

^{3}/s); and is predicted ductility at time (m

^{3}/s). The value of VAREX ranges from 0 (lowest performance) to 100 (highest performance).

#### 4. Results and Discussion

Artificial intelligence serves as a smooth interface between the qualitative variables and the numerical domains of the inputs and outputs of the model. As seen from the literature database, ductility of Ti aluminide is a function of number of variables, which are qualitative in nature. However, it can be presented mathematically where certain variables have primary effect on ductility of intermetallics and the same has been considered in the present work. The rule-base nature of the model allow the use of qualitative metallurgical relations expressed as general effect of different variables, which makes the model transparent to interpretation and analysis. Among the emerging modeling techniques ANN model has been considered to be very useful. Models are developed with the data generated from literature database with certain realistic assumptions and using different sets of data for training and validation. This makes the model more reliable.

Results of ANN models are presented in Table 5 and Figures 3–6. Figure 3 compares the RMS error for each model. It clearly shows that error is least for dataset 3. Similarly, Figure 4 compares the observed and achieved (modeled) ductility. Predicted ductility values are very close to observed values. Among the comparison of ANN results, data set 3 results are found to be very close to observed values. It also indicates achievable ductility value up to 5.7% in specific combination of parameters, that is, for multicomponent alloy with grain size of 50 *μ*m following heat treatment cycle number-7 (Table 2), that is, heating just below *α* transus temperature (*α*), soaking for 4 hrs → furnace cooling to *α*-50°C and soaking for 4 hrs at this temperature → furnace cooling to room temperature → heating below eutectoid temperature and soaking for 24 hours → air cooling to room temperature.

It is observed that models developed with data set 1 and 2 give results with high errors as compared to the models developed with data set 3. The minimum model error, that is, the difference between observed and modeled values gives the optimized parameters and it is found to be with data set 3. In Figures 5(a), 5(b), and 5(c) maximum error with individual dataset is presented, which is 0.36 for data set 3; 1.8 for data set 1; 2.2 for data set 2. It is purely due to the data selection. It is also noted that model developed with data set 3 give best performance (Figure 6). It shows that if the input data covers as many data as under different conditions then it can develop an efficient model.

The performance of the model has been evaluated by three criteria as *RMSE, regression coefficient, and variance (VAREX*) shown in Table 5. It is clearly seen that *RMSE* is least for data set 3 and *regression coefficient* as well as *VAREX* is highest at 96.91% and 96.8%, respectively. It indicates that all the three performance indicators are close to ideal indices.

Scattering of data values is more with dataset 1 (Figure 5(a)) and least with data set 3 (Figure 5(c)). It also shows predicted ductility is close to observed reported values and it follows a definite trend. Therefore, use of different combinations of data sets for training and validation gives better prediction of property in ANN models. It means that model would be helpful in deriving optimum combination of parameters to obtain highest ductility in Ti aluminide intermetallics.

Analysis of the data has also been attempted through adaptive neuro fuzzy inference system (ANFIS) [19] using Takagi Sugeno model with substractive cluster approach. Through ANIFIS models, prediction accuracy is found to be depending on number of input variables with extent of data mixing [19]. Therefore, it can be inferred that selection of input data decides the output accuracy in ANFIS as well as in ANN models. Prediction from ANFIS approach [19] and present ANN approach is found to be supporting each other. It is also true that, if scattering of data is more, ANN models are more suitable, since it generates output by adjusting the interconnections between the layers. In addition to that, ANN models have less dependency on modeling parameters as noted in ANFIS models [19], so prediction accuracy shall be certainly better with ANN models.

#### 5. Conclusions

(1)Models developed through ANN are giving results close to the observed reported ductility value especially with a wide range of data. (2)It gives very good result with data set 3 when data are randomly selected from entire data, which covers wide range of data.(3)Error (difference between observed and modeled values) is maximum for data set 2 as 2.2, while it is least as 0.36 for data set 3. (4)Regression coefficient is high with dataset 3 in ANN modeling (0.969). (5)Predicted ductility values are very close to observed values. Here achievable ductility value is obtained as 5.7% in specific combination of parameters. ANN predicts one specific combination. It is multicomponent alloy with grain size of 50*μ*m following heat treatment cycle number-7, that is, heating just below

*α*transus temperature (

*α*) → soaking for 4 hrs → furnace cooling to

*α*-50°C and soaking for 4 hrs at this temperature → furnace cooling to room temperature → heating below eutectoid temperature and soaking for 24 hours → air cooling to room temperature.

#### Acknowledgment

The authors extend their thanks to the Director, VSSC, for permitting to publish this paper.

#### References

- H. A. Lipsitt, “High temperature ordered intermetallic alloys,” in
*Materials Research Society Symposium Proceedings*, C. C. Koch, C. T. Liu, and N. S. Stolloff, Eds., vol. 39, p. 351, 1985. View at Google Scholar - A. I. Taub and R. L. Fleischer, “Intermetallic compounds for high-temperature structural use,”
*Science*, vol. 243, no. 4891, pp. 616–621, 1989. View at Google Scholar · View at Scopus - S. C. Huang and J. C. Cheshut,
*Gamma Ti Al and Its Alloys-Intermetallic Compounds*, vol. 2, John Wiley & Sons, Editors: J. H. Westbrook and R. L. Fleischer, 1994. - U. R. Kattner, J. C. Lin, and Y. A. Chang, “Thermodynamic assessment and calculation of the Ti-Al system,”
*Metallurgical Transactions, A*, vol. 23, no. 8, pp. 2081–2090, 1992. View at Google Scholar · View at Scopus - Y. W. Kim and F. H. Froes, “High temperature aluminides and intermetallics,” in
*The Minerals, Metals & Materials Society*, S. H. Whang, C. T. Liu, D. P. Pope, and J. O. Stiegler, Eds., p. 458, 1990. View at Google Scholar - Y. W. Kim and F. H. Froes, “High temperature aluminides and intermetallics,” in
*The Minerals, Metals & Materials Society*, S. H. Whang, C. T. Liu, D. P. Pope, and J. O. Stiegler, Eds., p. 456, 1990. View at Google Scholar - S. C. Huang, E. L. Hall, and D. S. Shih, “Microstructure and ductility of TiAl alloys modified by Cr additions,”
*ISIJ International*, vol. 31, no. 10, pp. 1100–1105, 1991. View at Google Scholar · View at Scopus - Y. W. Kim, “Microstructural evolution and mechanical properties of a forged gamma titanium aluminide alloy,”
*Acta Metallurgica Et Materialia*, vol. 40, no. 6, pp. 1121–1134, 1992. View at Google Scholar - S. C. Huang and E. L. Hall, “Characterization of the effect of vanadium additions to TiAl base alloys,”
*Acta Metallurgica Et Materialia*, vol. 39, no. 6, pp. 1053–1060, 1991. View at Google Scholar · View at Scopus - J. N. Wang and K. Xie, “Refining of coarse lamellar microstructure of TiAl alloys by rapid heat treatment,”
*Intermetallics*, vol. 8, no. 5-6, pp. 545–548, 2000. View at Google Scholar · View at Scopus - V. Seetharaman and S. L. Semiatin, “Microstructures and tensile properties of Ti—45.5Al—2Nb—2Cr rolled sheets,”
*Materials Science and Engineering A*, vol. 299, no. 1-2, pp. 195–209, 2001. View at Publisher · View at Google Scholar · View at Scopus - M. Beschliesser, A. Chatterjee, A. Lorich et al., “Designed fully lamellar microstructures in a
*γ*-TiAl based alloy: Adjustment and microstructural changes upon long-term isothermal exposure at 700 and 800 °C,”*Materials Science and Engineering A*, vol. 329-331, pp. 124–129, 2002. View at Publisher · View at Google Scholar · View at Scopus - V. Imayev, R. Imayev, and A. Kuznetsov, “Mechanical properties of thermomechanically treated Ti-rich
*γ*+*α*2 titanium aluminide alloys,”*Scripta Materialia*, vol. 49, no. 10, pp. 1047–1052, 2003. View at Publisher · View at Google Scholar · View at Scopus - H. Clemens, A. Bartels, S. Bystrzanowski et al., “Grain refinement in
*γ*-TiAl-based alloys by solid state phase transformations,”*Intermetallics*, vol. 14, no. 12, pp. 1380–1385, 2006. View at Publisher · View at Google Scholar · View at Scopus - M. Perez-Bravo, I. Madariaga, K. Ostolaza, and M. Tello, “Microstructural refinement of a TiAl alloy by a two step heat treatment,”
*Scripta Materialia*, vol. 53, no. 10, pp. 1141–1146, 2005. View at Publisher · View at Google Scholar · View at Scopus - J. N. Wang, J. Yang, and Y. Wang, “Grain refinement of a Ti—47Al—8Nb—2Cr alloy through heat treatments,”
*Scripta Materialia*, vol. 52, no. 4, pp. 329–334, 2005. View at Publisher · View at Google Scholar - E. H. Mamdani and S. Assilian, “Experiment in linguistic synthesis with a fuzzy logic controller,”
*International Journal of Man-Machine Studies*, vol. 7, no. 1, pp. 1–13, 1975. View at Google Scholar · View at Scopus - H. R. Maier and G. C. Dandy, “Neural networks for the prediction and forecasting of water resources variables: A review of modelling issues and applications,”
*Environmental Modelling and Software*, vol. 15, no. 1, pp. 101–124, 2000. View at Publisher · View at Google Scholar · View at Scopus - R. K. Gupta, R. Mehta, V. Agarwala, B. Pant, and P. P. Sinha, “Ductility prediction of Ti aluminide intermetallics through neuro-fuzzy set approach,”
*Transactions of the Indian Institute of Metals*, vol. 63, no. 6, pp. 833–839, 2010. View at Publisher · View at Google Scholar - B. Kosko,
*Neural Networks and Fuzzy Systems*, Prentice Hall of India, New Delhi, India, 1996. - A. Y. Badmos, H. K. D. H. Bhadeshia, and D. J. C. MacKay, “Tensile properties of mechanically alloyed oxide dispersion strengthened iron alloys. Part 1: neural network models,”
*Materials Science and Technology*, vol. 14, no. 8, pp. 793–809, 1998. View at Google Scholar - S. Calcaterra, G. Campana, and L. Tomesani, “Prediction of mechanical properties in spheroidal cast iron by neural networks,”
*Journal of Materials Processing Technology*, vol. 104, no. 1, pp. 74–80, 2000. View at Publisher · View at Google Scholar · View at Scopus - J. McBride, S. Malinov, and W. Sha, “Modelling tensile properties of gamma-based titanium aluminides using artificial neural network,”
*Materials Science and Engineering A*, vol. 384, no. 1-2, pp. 129–137, 2004. View at Publisher · View at Google Scholar · View at Scopus - H. S. Rao and A. Mukherjee, “Artificial neural networks for predicting the macromechanical behaviour of ceramic-matrix composites,”
*Computational Materials Science*, vol. 5, no. 4, pp. 307–322, 1996. View at Publisher · View at Google Scholar · View at Scopus - S. Malinov and W. Sha, “Application of artificial neural networks for modelling correlations in titanium alloys,”
*Materials Science and Engineering A*, vol. 365, no. 1-2, pp. 202–211, 2004. View at Publisher · View at Google Scholar · View at Scopus - R. P. Lippmann, “Introduction to computing with neural nets,”
*IEEE ASSP Magazine*, vol. 4, no. 2, pp. 4–22, 1987. View at Google Scholar · View at Scopus - J. E. Nash and J. V. Sutcliffe, “River flow forecasting through conceptual models part I—a discussion of principles,”
*Journal of Hydrology*, vol. 10, no. 3, pp. 282–290, 1970. View at Google Scholar · View at Scopus - S. C. Huang, “Microstructures and property tradeoffs in wrought TiAl-base alloys,”
*Metallurgical Transactions A*, vol. 23, no. 1, pp. 375–377, 1992. View at Publisher · View at Google Scholar · View at Scopus - G. A. Salishchev, R. M. Imayev, O. N. Senkov, and F. H. Froes, “Microstructural control in Ti-Al for enhanced mechanical properties,”
*Journal of the Minerals*, vol. 52, no. 12, pp. 46–48, 2000. View at Google Scholar · View at Scopus - R. Imayev, V. Imayev, and G. Salishchev, “Effects of grain size and grain boundary structure on yield strength of micro- and submicrocrystalline TiAl,”
*Scripta Metallurgica et Materiala*, vol. 29, no. 5, pp. 719–724, 1993. View at Google Scholar · View at Scopus - R. Imayev, V. Imayev, and G. Salishchev, “Effect of grain size on ductility and anomalous yield strength of micro- and submicrocrystalline TiAl,”
*Scripta Metallurgica et Materiala*, vol. 29, no. 5, pp. 713–718, 1993. View at Google Scholar · View at Scopus - D. Hu, “Effect of boron addition on tensile ductility in lamellar TiAl alloys,”
*Intermetallics*, vol. 10, no. 9, pp. 851–858, 2002. View at Publisher · View at Google Scholar · View at Scopus - J. Tang, B. Huang, W. Liu et al., “A high ductility TiAl alloy made by two-step heat treatment,”
*Materials Research Bulletin*, vol. 38, no. 15, pp. 2019–2024, 2003. View at Publisher · View at Google Scholar · View at Scopus