Next Article in Journal
Controllable Preparation of Spherical Molybdenum Nano-Powders by One-Step Reduction of APM in Radio Frequency Hydrogen Plasma
Next Article in Special Issue
Establishment of Analytical Model for CFRP Cutting Force Considering the Radius of the Edge Circle
Previous Article in Journal
The Influence of the Deformation Method on the Microstructure and Properties of Magnesium Alloy Mg-Y-RE-Zr
Previous Article in Special Issue
Optimizing Friction Stir Welding of Dissimilar Grades of Aluminum Alloy Using WASPAS
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Multi-Response Optimization of Al2O3 Nanopowder-Mixed Wire Electrical Discharge Machining Process Parameters of Nitinol Shape Memory Alloy

1
Department of Mechanical Engineering, School of Technology, Pandit Deendayal Energy University, Raisan, Gandhinagar 382007, India
2
Department of Solar Engineering, School of Technology, Pandit Deendayal Energy University, Raisan, Gandhinagar 382007, India
3
Department of Automated Mechanical Engineering, South Ural State University, Lenin Prosp. 76, 454080 Chelyabinsk, Russia
4
School of Mechanical and Design Engineering, University of Portsmouth, Portsmouth PO1 3DJ, UK
*
Authors to whom correspondence should be addressed.
Materials 2022, 15(6), 2018; https://doi.org/10.3390/ma15062018
Submission received: 18 February 2022 / Revised: 7 March 2022 / Accepted: 8 March 2022 / Published: 9 March 2022
(This article belongs to the Special Issue Machining and Machinability of Advanced Materials and Composites)

Abstract

:
Shape memory alloy (SMA), particularly those having a nickel–titanium combination, can memorize and regain original shape after heating. The superior properties of these alloys, such as better corrosion resistance, inherent shape memory effect, better wear resistance, and adequate superelasticity, as well as biocompatibility, make them a preferable alloy to be used in automotive, aerospace, actuators, robotics, medical, and many other engineering fields. Precise machining of such materials requires inputs of intellectual machining approaches, such as wire electrical discharge machining (WEDM). Machining capabilities of the process can further be enhanced by the addition of Al2O3 nanopowder in the dielectric fluid. Selected input machining process parameters include the following: pulse-on time (Ton), pulse-off time (Toff), and Al2O3 nanopowder concentration. Surface roughness (SR), material removal rate (MRR), and recast layer thickness (RLT) were identified as the response variables. In this study, Taguchi’s three levels L9 approach was used to conduct experimental trials. The analysis of variance (ANOVA) technique was implemented to reaffirm the significance and adequacy of the regression model. Al2O3 nanopowder was found to have the highest contributing effect of 76.13% contribution, Ton was found to be the highest contributing factor for SR and RLT having 91.88% and 88.3% contribution, respectively. Single-objective optimization analysis generated the lowest MRR value of 0.3228 g/min (at Ton of 90 µs, Toff of 5 µs, and powder concentration of 2 g/L), the lowest SR value of 3.13 µm, and the lowest RLT value of 10.24 (both responses at Ton of 30 µs, Toff of 25 µs, and powder concentration of 2 g/L). A specific multi-objective Teaching–Learning-Based Optimization (TLBO) algorithm was implemented to generate optimal points which highlight the non-dominant feasible solutions. The least error between predicted and actual values suggests the effectiveness of both the regression model and the TLBO algorithms. Confirmatory trials have shown an extremely close relation which shows the suitability of both the regression model and the TLBO algorithm for the machining of the nanopowder-mixed WEDM process for Nitinol SMA. A considerable reduction in surface defects owing to the addition of Al2O3 powder was observed in surface morphology analysis.

1. Introduction

A new group of alloys, also known as smart materials, are gaining popularity due to their unique feature of remembering their shape throughout their lifecycle. These are also termed shape memory alloys (SMAs) which mutate back to their original shape on heating after deformation under load [1,2]. In addition, SMAs also possess generic properties such as superelasticity, favorable microstructure, and pseudoelasticity [3,4]. The reversible martensitic phase transformation enables SMAs to generate higher work output and higher stress and strain actuation [5]. Several alloys and their combinations, such as Nickel–Titanium (NiTi), CuAlNi, Au–Cd, etc., have been developed showing shape memory effects [6,7]. Among various applications of SMAs, the most popular uses include the following: biomedical, aerospace, automotive, robotics, etc., in addition to the exploration of newer engineering fields [8,9]. The release of Ni ions in biofluid is prevented by the formation of a protective TiO2 layer which is formed from titanium material present in Nitinol [10,11]. This leads to Nitinol`s suitability for biomedical applications. The hardening of Nickel-based alloys is comparatively faster owing to the presence of an austenitic matrix which is the biggest hindrance to the machining ease of alloys [12,13]. Additionally, the pseudoelasticity and higher ductility properties of Nitinol pose a challenge for the machining of Nitinol. Several causes that obstruct the machining of SMAs via conventional methods include excessive time for machining, formation of burrs, excessive tool wear, inferior cutting efficiency, and unacceptable surface quality [14,15]. This makes non-conventional machining techniques fairly suitable for SMAs, especially for Nitinol. To achieve dimensional precision and reasonable surface integrity, surface roughness (SR), high production rate, and thin recast layer thickness (RLT) become mandatory to achieve during the manufacturing of instruments for biomedical applications given the nature of intricacy. Researchers are in pursuit of the same.
Non-contact operation of the wire electrical discharge machining (WEDM) technique, among work material and machining tool (wire), extensively reduces the difficulties of conventional machining methods [16,17]. Complex shape implants and structures are one of the key requirements for biomedical applications [18]. WEDM is an advanced machining process capable of producing complex shape geometries [19]. During the process, serial sparks are formed between tool and component which erodes the little amount of material through melting and vaporization [20,21]. Dielectric fluid is used in the machining zone which helps to remove the eroded material particles [22]. This phenomenon of dielectric flushing and sparking forms a hard and uneven machined surface [23]. Thus, SR becomes a crucial response variable during the WEDM process. The WEDM method involves a multiple and complex control of parameters for obtaining a better surface [24]. For the industry, higher productivity is also of prime importance, in addition to the excellent machined surface which can be achieved by enhancing the material removal rate (MRR) and concurrently decreasing SR and RLT. One of the ways to achieve this is to mix nanopowder in dielectric fluid during the WEDM process.
The current trend suggests that powder-mixed dielectric fluid is most popular among researchers for obtaining optimum parametric settings to achieve multiple objectives [25,26]. A series of research studies using Al, CNT, Cr, etc., as additives have been experimented by researchers with dielectric fluid for the EDM process [27,28]. For this process, different parameters for powder characteristics, including powder concentration, powder size, thermal and electrical conductivity, and powder density, have a significant effect on the process [28]. Anil Kumar et al. [29] implemented Grey–Taguchi’s combined approach for the powder-mixed EDM (PMEDM) process. Improvement in all responses has been found after the addition of powder with dielectric fluid. Prakash et al. [30] studied the effect of Si powder on the EDM process of titanium alloys. Their results depicted the improvement in MRR along with the reduction in tool wear rate (TWR). They also observed reduction in the recast layer thickness (RLT) and reduction in surface defects at Si powder concentration of 4 g/L. Amit et al. [31] analyzed the effect of the PMEDM process by adding Al2O3 nanopowder along with dielectric fluid for obtaining a better machining output. Both the response variables (MRR and SR) were improved to a large extent with the modified dielectric fluid along with better sparking stability of the nanopowder-mixed EDM (NPMEDM) process. Sahu and Mandal [32] analyzed the influence of Al2O3 PMEDM for the EDM process of Nimonic-263. They observed improvement in the surface morphology of machined surfaces with the use of Al2O3 PMEDM. Kumar et al. [33] used Al2O3 nanopowder to study the performance of the EDM process on MRR and SR. They compared the performance of the Al2O3 nanopowder with the conventional EDM process and observed an improvement of 44% and 51% in MRR and SR, respectively, with the use of nanopowder. Tan and Yeo [34] observed a substantial reduction in RCL with the use of nanopowder concentration in dielectric fluid. Aiyeshah et al. [35] obtained a minimum SR of 3.107 µm and RCL of 14.92 µm with the use of Si powder for Nimonic-90 superalloy. Pulse-on time (Ton), pulse-on time (Toff), current, and amount of Si powder were found to be the most contributing factors for obtaining the desired levels of SR and RLT. Vinay et al. [36] used aluminum oxide powder in EDM machining of Inconel 825. SR of the machined samples improved with the addition of powder concentration. Another study, conducted by Sagar et al. [37], used Al2O3 powder in EDM for Inconel 718 and reported that the response variables depend on the EDM machining variables. Little effect of Al2O3 powder was seen on the response variables. It becomes essential to control all the machining variables simultaneously to achieve optimal levels of multiple response variables.
On detailed examination of relevant literature, researchers used different powders for the machining of various alloys. Researchers have given more attention to the improvement of responses such as MRR, SR, and TWR. However, very limited work was carried out on other useful output parameters such as RLT and surface morphology of the machined surface. To the best of our knowledge, the effect of Al2O3 nanopowder and simultaneous optimization of WEDM parameters using the Teaching–Learning-Based Optimization (TLBO) algorithm for Nitinol SMA has not yet been reported. In the current study, a handful of work considering Ton, Toff, and amount of Al2O3 nanopowder as the input variables along with MRR, SR, and RLT as the response variables of Ni55.8Ti SMA has been reported. Experiments were conducted using Taguchi’s L9 orthogonal arrays. Analysis of variance (ANOVA) was used to check the adequacy and significance of the variables. Taguchi’s approach has a limitation of attaining only one response variable at a time. In addition, the TLBO algorithm was implemented for simultaneous optimization of output responses of MRR, SR, and RLT. Lastly, the surface morphology of the machined surface was reported by SEM analysis. The authors strongly consider this study to be very useful for industrial applications.

2. Preparation of Al2O3 Nanopowder

The chemical reagents aluminum nitrate nanohydrate (Al(NO3)3·9H2O), citric acid (C6H8O7), triethanolamine (N(CH2CH2OH)), and ethylene glycol (EG) were purchased from Sigma Aldrich Inc. and were used without further purification. Ultrapure water with resistivity 18.2 MΩ-cm was used throughout the experiments. In a typical process, aluminum nitrate nanohydrate was dissolved in deionized water and stirred at medium speed to obtain a uniform mixture. Subsequently, triethanolamine was added dropwise in the solution. Later, citric acid was slowly added to this solution and stirred at 75 °C for 45 min; the color of the sols changed and the obtained sols were then heated up to 150 °C for 90 min, resulting in the viscous gels. For complete drying, the sol was thermally heated in an inert atmosphere at 600 °C for 3 h to produce Al2O3 nanopowders. The synthesized Al2O3 nanopowders were characterized with scanning electron microscopy (Zeiss Ultra 55 at 5 kV), X-ray diffraction (XRD) (Panalytical X’pert Pro with the source of Cu-Kα radiation of 0.154 nm, λ = 1.54 Å and acceleration voltage of 45 kV and 40 mA) in a range from 10 to 90°, and Raman Spectroscopy (using a laser of wavelength 532 nm).

3. Experimental Plan and Methods

3.1. Experimental Details

In the present study, experimentation was accomplished with Ni55.8Ti SMA, 6 mm in diameter. Molybdenum wire was used as an electrode. The chemical composition contains the major elements Ni (55.78%) and Ti as a remainder. Al2O3 nanopowder was mixed along with EDM oil in a tank with various amounts, as per the experimental plan. The stirrer was used for uniform mixing of Al2O3 nanopowder in dielectric fluid. This will not allow nanopowder to settle at bottom of the tank. The Al2O3-mixed dielectric fluid was sprayed through nozzles in the machining zone. Three useful input parameters, namely Ton, Toff, and amount of Al2O3 nanopowder, were varied during the experimental trials. Experiments were performed by using Taguchi’s L9 orthogonal arrays. Slices of 1.5 mm in length were cut from the rod following the experimental matrix generated using Taguchi’s design. Table 1 shows the experimental conditions of the PMWEDM operation. Process parameters and their levels were selected, as per the literature studies, pilot tests, and machining limits. In the current study, MRR, SR, and RLT are considered response variables. Two or more repetitions are mandatory for each trial to assess the experimental error and provide the conditions required to test the hypothesis [38,39]. All the experiments were repeated three times in the current study and the average value of the obtained results was considered for analysis. Minitab v17 was employed to analyze the experimental results.
The MRR was measured (gram/minute) by determining the weight of the machined components, as per Equation (1).
M R R = ( W b m W a m ) × 60   t
where W b m and W a m are the weight of the components in grams, and t represents the time in seconds.
The Mitutoyo Surftest SJ-410 model was used to measure the SR by selecting the cut-off length of 0.8 mm. SR values were measured at three locations and the average value was taken for analysis.
RLT and surface morphology of the machined surface were measured by using a FE-SEM. Initially, the machined samples were mechanically polished using different grades of emery paper, and then chemically etched (14 mL HNO3, 4 mL HF, 82 mL H2O) to avoid burrs. Specimens were then explored for the measurement of RLT through the SEM technique.

3.2. Optimization Using TLBO Algorithm

For the current study, Teaching–Learning-Based Optimization (TLBO) algorithm is used to obtain the optimum values of the machining parameters. Multi-objective optimization is applied to such problems when there is a trade-off between conflicting objectives. TLBO overcomes the complexity of tuning control parameters and offers ease in the computational time compared to other multi-objective optimization algorithms [40]. It is an easy and efficient algorithm wherein the significance of a teacher on the outcome of the learner is taken into consideration. It adapts the teaching–learning process in a traditional classroom where students learn from teachers to improve their knowledge. Furtherly, students can also interact among themselves to share their knowledge, hence, TLBO involves the following two-phase learning: (a) teacher phase—wherein students learn from teacher; (b) learner phase—wherein students interact among learners [41]. Figure 1 represents the flowchart of the processes involved in the TLBO algorithm.
With this analogy, the TLBO algorithm is developed to obtain good results (objective function) for the given class of students (population) by teaching different subjects (design variables). The result of the student after undergoing the teaching–learning process is as good as the fitness value of an objective function. The best result (solution) from the class is considered as a teacher. A good teacher strives to bring the level of learners to his or her knowledge and eventually increases the mean of the results. However, in practice, not each learner can reach up to a level of the teacher, as it depends on the individual’s capability [42]. If Mi is the mean of the class, then for each ith iteration, the solution in the teacher phase will be updated for the existing and new mean which is given as follows:
Difference_Meani = ri (MnewTF Mi)
where ri represents a random number generated between 0 and 1, Mnew represents the values of design variables corresponding to the teacher, and Mi represents the mean value of design variables considering all students.
TF = round (1) + rand (0, 1)
Xnew,i = Xold,i + Difference_Meani
where TF is the teaching factor which decides the mean value, either 1 or 2.
In the learner’s phase, learners improve their knowledge through interaction between themselves. If a learner interacts through group discussion and presentations, with the learner having more knowledge, the former ones learn something new. Upon selecting two learners randomly, modification is presented, as per Equations (5) and (6):
If f(Xj) < f(Xk),
Xnew,j = Xold,j + rj (XjXk)
Else
Xnew,j = Xold,j + rj (XkXj)
where, rj represents a random number generated between 0 and 1, and the subscript i represents iterations, while j and k represent the population, where jk.

4. Results and Discussions

4.1. Morphological and Structural Analysis

The morphology and structure of as-synthesized Al2O3 nanopowder were examined under a field emission scanning electron microscope (FE-SEM), as shown in Figure 2a. It was observed that the nanopowder was in the range of about 100 nm. Further, energy-dispersive X-ray spectroscopy was carried out to determine the elements present in the as-synthesized Al2O3 nanopowder, shown in Figure 2b. The results confirmed the presence of aluminum and oxygen in the synthesized material and no extra elements were observed other than carbon, which can be attributed to the presence of carbon in carbon tape. In addition, the structural properties of the prepared Al2O3 were analyzed under X-ray diffraction and Raman Spectroscopy (Renishaw in via Raman Microscope, Pune, India), as shown in Figure 2c,d. The diffraction profile shows peaks at 2θ~68.2°, 66.3°, 57.6°, 52.4°, 43.7°, 37.8°, 35.2°, and 25.3° can be attributed to 300, 214, 116, 024, 113, 110, 104, and 012 planes (JCPDS No 46-1212), confirming the formation of α-Al2O3 with hexagonal structure [43]. The average crystallite size obtained from peaks was 27 nm using the Debye–Scherrer formula, as shown in Equation (7):
D = 0.9 λ β C o s θ
where ‘β’ represents full width at half maximum (FWHM), ‘D’ represents the crystalline size, ’λ’ represents the wavelength of CuKα radiation, and ‘θ’ represents the angle of diffraction. Further, the Raman profile (Figure 2d) showed characteristic peaks at 378 cm−1 and 416 cm−1, which were found in agreement with the reported work of Cava et al. [44]. The sharp peaks of the α-phase indicate the well-defined long-range order in corundum and large grain sizes. The powders do not present any impurities, as no extra peaks were observed. The Raman spectra also confirm the formation of α-phase Al2O3 and were found in agreement with XRD results.

4.2. Experimental Results as per Taguchi’s L9 OA

The Al2O3 nanopowder-mixed WEDM process variables, as per the L9 Taguchi OA, are shown in Table 2. Experimentally obtained results of the process variables (MRR, SR, and RLT) are also presented in Table 2.

4.3. Parametric Effect on MRR

ANOVA can be effectively used to check the relative significance of input parameters on output variables. A 95% confidence level was selected to determine the significance of WEDM parameters, such as Ton, Toff, and Al2O3 nanopowder, on MRR. Lower P-/higher F-value indicates the larger influence of the machining variable on the selected response [45]. To have a significance of an input variable on the output variable, it is desired to have a p-value of less than 0.05 [46,47]. Table 3 illustrates the ANOVA for MRR. All the input variables, such as Ton, Toff, and Al2O3 nanopowder, were having a significant effect on the MRR, as their p-value was less than 0.05. The Al2O3 nanopowder has the highest contribution of 76.13%, followed by Toff (17.47%) and Ton (7.14%). A small deviation among the R-sq. and Adj. R-sq. signifies the adequacy and fitness of the model [48]. A negligible difference in R-Sq. values of the existing model suggests that it is adequate and fit for estimation of future outcomes of MRR. The regression model for the prediction of MRR is shown in Equation (8), as follows:
MRR   = 0.0730 + 0.0471 · Current + 0.0111 · T on 0.0143 · T off   + 0.1299 · Powder   Conc .
The significance of the WEDM variables on MRR is illustrated in Figure 3. The MRR value was enhanced with an increase in the concentration of Al2O3 nanopowder. The MRR has improved substantially with the increase in Al2O3 nanopowder, as the sparking frequency and thermal conductivity of the dielectric fluid increases [27]. This further increases the rate of erosion of the work material and gives the increase in MRR. From Figure 3, upon increasing Ton, the value of MRR was improved. As Ton increases, discharge energy and spark intensity also increase [49]. Discharge energy gets converted into thermal energy. Thermal energy melts and vaporizes the material from the work surface [50]. Thus, higher thermal energy erodes more material from work, and thereby, increases the MRR. Toff was found to have a reverse on MRR, in comparison to Ton. An increase in Toff reduces the intensity of the spark [51,52]. This further reduces the discharge energy, and subsequently, the MRR value also decreases with an increase in Toff.

4.4. Analysis of SR

ANOVA was employed to evaluate the regression coefficients of the model. Table 4 illustrates the ANOVA of SR. A 95% confidence level was selected to determine the significant impact of machining parameters such as Ton, Toff, and Al2O3 nanopowder on SR. Ton, Toff, and Al2O3 nanopowder were observed as significant contributing factors for SR response as p-value of these input factors was found to be less than 0.05. Ton was found to be the highest contributing factor (91.88%), trailed by Toff (6.36%) and Al2O3 nanopowder (1.17%). A negligible error of 0.58% was found for SR. A small deviation among the R-sq. and Adj. R-sq. signifies the adequacy and fitness of the model [53,54]. A negligible difference in R-Sq. values of the existing model suggest that it is adequate and fit for estimation of future outcomes of SR. The regression model for the prediction of SR is shown in Equation (9), as follows:
SR   = 3.195 + 0.2522   · Current + 0.0565 · T on 0.0588 · T off 0.3550 · Powder   Conc
Figure 4 describes the significance of the WEDM variables on the SR response. SR of the machined components was found to follow an increasing trend with a rise in the value of Ton. The rise in the Ton value increases the discharge energy, which in turn increases the thermal energy [55,56]. Due to higher discharge energy and thermal energy, plasma channel pressure increases, impulsive forces are created, and this produces rough and irregular surfaces [56]. Thus, due to the higher thermal energy, SR value increases with an increase in Ton value. The declined trend was noticed in SR with an increase in Toff. An increase in Toff decreases the discharge energy and small craters are created [57,58]. This increases the quality of the surface by decreasing the SR value. Another reason for the decreasing SR is that with an increase in the Toff value, the flushing of debris gains more time and it removes the unwanted eroded particles from the machined zone [59,60]. From Figure 4, by increasing the Al2O3 amount, a decrease in the SR was identified. The addition of nanopowder concentration expands the interelectrode gap and also increases the heat dissipation in the dielectric fluid by forming small craters and reducing the plasma heat flux [31,61]. The addition of Al2O3 nanopowder enhances the flushing of debris from the machining zone. Improved flushing of debris forms small ridges resulting in improved surface quality [27].

4.5. Analysis of RLT

Investigation on the effect of the input process parameters of Ton, Toff, and Al2O3 nanopowder on RLT was carried out by using ANOVA. Specimens were explored for the measurement of RLT through the SEM technique at 1000× magnification. Table 5 illustrates the ANOVA for RLT. All the input variables, such as Ton, Toff, and Al2O3 nanopowder, were having a significant effect on the RLT as their P-value was observed to be less than 0.05. Ton was found to be the highest contributing factor (88.3%), trailed by Toff (7.85%) and Al2O3 nanopowder (3.38%). A negligible error contribution of 0.47% was observed for SR. A small deviation among the R-sq. and Adj. R-sq. signifies the adequacy and fitness of the model. A negligible difference in R-Sq. values of the existing model suggest that it is adequate and fit for the estimation of future outcomes of RLT. The regression model for the prediction of RLT is shown in Equation (10), as follows:
RLT   = 3.195 + 0.2522   · Current + 0.0565 · T on 0.0588 · T off 0.3550 · Powder   Conc
Figure 5 describes the influence of the WEDM process parameters on RLT. The RLT of the machined components was found to follow the increasing trend with a rise in the value of Ton. An increase in the Ton value creates larger dispersive energy, which in turn melts more work material. With the increased value of Ton, the dielectric is unable to flush the molten metal, due to which it gets deposited on the machined surface [62]. This unflushed molten metal then quenches and re-solidifies by forming a thick RLT [63]. However, with an increase in the value of Toff, RLT decreases as the melting of the material reduces with the increased value of Toff. Additionally, debris of work material gain enough time to flush away from the machining zone [64]. This reduces the RLT of the machined zone. From Figure 5, by increasing the Al2O3 amount, a decrease in RLT was noticed. The addition of nanopowder increases the interelectrode gap and reduces the insulation strength of the dielectric by reducing the energy density [27,64]. This in turn produces a thin RLT, as it largely eliminates the redeposition of debris in the machined zone. Additionally, with the addition of Al2O3 nanopowder, the spark gap increases. This reduces the discharge energy in the machined zone, and Al2O3 nanopowder removes the dissipated heat from the zone. It creates shallow craters and forms a thin RLT [34,65].

4.6. Optimization Using TLBO Algorithm

TLBO algorithm was executed by considering all responses as positive integers. Following machining, limits were used for the WEDM process parameters during the execution of the algorithms.
(Ton): 30 µs ≤ Ton ≥ 90 µs
(Aoff): 5 µs ≤ Toff ≥ 25 µs
(Al2O3 Conc.): 0 g/L ≤ Al2O3 Conc. ≥ 2 g/L
Single-objective optimization was carried out for the response parameters to maximize MRR and minimize SR and RLT using the TLBO algorithm. The effect of machining variables Ton, Toff, and Al2O3 nanopowder was studied on the aforementioned response parameters. Results of the optimization are presented in Table 6. Within the selected range of machining variables, single-objective optimization results showed that maximum MRR of 0.3228 g/min, minimum SR of 5.94 µm, and minimum RLT of 20.59 µm was obtained. It is evident from the results that with an increase in Ton, MRR increases, but at the same time SR and RLT also reach a maximum value, which is not desirable. Similarly, minimum SR and RLT were obtained with minimum Ton time, but by doing so, MRR is compromised as it gives the least MRR of 0.1988 g/min. Hence, it can be concluded that the response parameters are conflicting and results of the single-objective optimization allow a user to select the machining variables in such a way that either of the response parameters can be maximized or minimized. It is important to solve the trade-off between these variables so that the optimum combination of parametric settings for the WEDM process can be adapted. Such complexity can be resolved by solving the problem using a multi-objective optimization approach. Equal weights of 0.33 have been assigned to the output responses to perform the simultaneous optimization by using the MOTLBO algorithm. Equation (11) shows the objective function for simultaneous optimization, as follows:
Obj   = w 1 · ( MRR ) + w 2 · ( SR ) + w 3 · ( RLT )
The simultaneous optimization result has yielded response values for MRR, SR, and RLT of 0.2539 g/min, 3.65 µm, and 12.28, respectively, at Ton of 31 µs, Toff of 12 µs, and Al2O3 conc. of 2 g/L.
In the basic TLBO algorithm, learners learn from a single teacher and through interaction among themselves, and subsequently, there are two possibilities that either the learner learns completely or nothing at all. The modified algorithm addresses the problems by dividing the learners into small groups and each group of learners is assigned a teacher, thus, having more than one teacher in a class. Now, the teacher has to improve the skills of the respective assigned group of learners and once the desired results are attained, they are allotted to the next best teacher. Another modification in terms of the adaptive teaching factor is incorporated in the basic algorithm. The learners may learn in any proportion from the teacher and not just two or one as in basic algorithm. Such modifications help in a faster convergence rate and speed up exploration and exploitation in the search space.
Table 7 shows the 48 Pareto points of multi-objective optimization, where each point represents a unique optimal combination of machining variables between the bounds. The optimal Pareto curve for the three response parameters was plotted in 3D with X, Y, and Z-axis representing MRR, RLT, and SR, respectively, as shown in Figure 6. Each combination of the machining variables selected from the Pareto front will yield optimum machining results, with the intended objective of maximizing MRR and minimizing RLT & SR. The input parameters Ton, Toff, and Al2O3 nanopowder influence the response parameters concerning the magnitude of variables and the selection of the optimum combination of machining variables is left to the user for attaining the desired outcome.
To validate the results of the optimization algorithm, five optimal points are selected from the Pareto front, and machining is carried out to measure the response parameters. Table 8 shows the comparison of predicted values of MRR, SR, and RLT obtained from the MOTLBO algorithm and experimentally measured response values. It was observed that the experimental results are in good agreement with the optimization results and the measured responses are well within 5% variation, which is regarded as a negligible variance.
To understand the effect of the variables on the response parameters, simplified 2D graphs were plotted considering the effect of the third variable. Figure 7a shows the effect of the machining variables on MRR and SR. It was observed that with an increase in machining MRR, SR increases, resulting in poor machining surface. A maximum MRR (marked with red dot) of 0.322 g/min was obtained with a maximum SR of 5.94 µm, whereas a minimum SR of 3.13 µm was obtained when the MRR was 0.198 g/min. Users can work with the conflicting nature of the parameters and select the combination with the intended objective. Similarly, Figure 7b,c represents the effect of the variables on MRR & RLT and SR & RLT, respectively. Higher MRR results in higher RLT, which is again not a desirable outcome, however, for a user, it is easy to proceed with the combination that can be aimed for either maximum MRR or minimum RLT. However, a linear relationship between SR and RLT is observed indicating that with an increase in SR, RLT increases linearly, and hence, it is always desired to have their minimum. From Figure 7c, it is obvious that minimum SR and RLT (marked with red dot) were obtained as 3.13 µm and 10.24 µm, respectively.

4.7. Surface Morphological Study

Investigation of the machined surfaces was carried out using FE-SEM. Specimens were explored for a surface morphological study through the SEM technique at 500× magnification. The optimal parameter settings obtained through simultaneous optimization of responses (Equation (5)) were used to study the surface morphology of the obtained machined surfaces at different nanopowder concentrations. The simultaneous optimal parameter settings have a Ton of 31 µs, Toff of 12 µs, and Al2O3 conc. of 2 g/L. Surface morphology analysis was carried out to find the effect of Al2O3 conc. According to this, Al2O3 conc. was varied at 0 g/L, 1 g/L, and 2 g/L, while keeping Ton and Toff at their optimal values of 31 µs and 12 µs, respectively. Figure 8, Figure 9 and Figure 10 illustrate the SEM micrographs at Al2O3 conc. Of 0 g/L, 1 g/L, and 2 g/L, respectively. A large number of surface defects can be observed in Figure 8. A large amount of melted material deposition, micro-cracks, globules of debris, and micro-pores was found on the machined surface. Figure 9 (Al2O3 amount of 1 g/L) shows improved surface in terms of reduction in surface defects in comparison with Figure 8 (Al2O3 amount of 0 g/L). A substantial improvement can be observed in the surface morphology of Figure 10 (Al2O3 amount of 2 g/L), which clearly shows a major reduction in surface defects. A large reduction in melted material deposition, micro-cracks, globules of debris, and micro-pores can be seen in Figure 10. This clearly shows that the addition of Al2O3 amount has reduced the surface defects to a larger extent. The addition of nanopowder creates uniform sparking among the work–tool interface [40,66]. This uniform sparking between work and tool has reduced the micro-crack substantially [67]. The addition of nanopowder concentration expands the interelectrode gap and also increases the heat dissipation in the dielectric fluid by forming small craters and reducing the plasma heat flux [27,31]. In turn, this reduces the surface defects of the melted material deposition, formation of globules, and micro-pores. The addition of Al2O3 nanopowder enhances the flushing of debris from the machining zone [31]. The improved flushing of debris forms small ridges resulting in improved surface quality.

5. Conclusions

In the current study, pulse-on time (Ton), pulse-off time (Toff), and Al2O3 nanopowder concentration were used for achieving higher MRR and lower SR and RLT for the WEDM machining of Nitinol. TLBO algorithm was used to achieve the desired responses simultaneously. The below mentioned useful remarks can be made based on the present study:
  • Statistical analysis from ANOVA showed that all WEDM variables (Ton, Toff, and Al2O3 nanopowder) were observed to have a significant effect on all the response variables (MRR, SR, and RLT).
  • For MRR, Al2O3 nanopowder has the highest contributing effect of 76.13%, followed by Toff (17.47%) and Ton (7.14%). For SR, Ton was found to be the highest contributing factor (91.88%), trailed by Toff (6.36%) and Al2O3 nanopowder (1.17%). For RLT, Ton was found to be the highest contributing factor (88.3%), trailed by Toff (7.85%) and Al2O3 nanopowder (3.38%). Negligible error contribution was observed for all responses.
  • The proposed model can be treated as adequate and the best fit as close relation between R-sq. and Adj. R-sq. was obtained and their values were near to 1. This also signifies that the model is appropriate for predicting the future outcomes of MRR.
  • The main effect plots for MRR, SR, and RLT illustrated that the addition of Al2O3 nanopowder improved the performance of all response variables.
  • With the addition of Al2O3 nanopowder, the rate of erosion of the work material increased and gave an increased MRR. With the addition of Al2O3 nanopowder, the formation of small craters and uniform flushing of debris resulted in lower SR. With the addition of Al2O3 nanopowder, redeposition of debris was removed from the machined zone resulting in thin RLT.
  • The single-objective optimization result from TLBO yielded maximum MRR of 0.3228 g/min (at Ton of 90 µs, Toff of 5 µs, and amount of Al2O3 of 2 g/L), minimum SR of 3.13 µm, and minimum RLT of 10.24 µm (both responses at Ton of 30 µs, Toff of 25 µs, and amount of Al2O3 of 2 g/L).
  • The simultaneous optimization result yielded response values of MRR, SR, and RLT of 0.2539 g/min, 3.65 µm, and 12.28, respectively, at Ton of 31 µs, Toff of 12 µs, and Al2O3 conc. of 2 g/L.
  • A multi-objective TLBO algorithm was used to generate Pareto optimal points highlighting the non-dominant feasible solutions.
  • It was observed that the experimental results were in good agreement with the optimization results and the measured responses were well within 5% variation. The least error between predicted and actual values suggests the effectiveness of both the regression model and TLBO algorithm.
  • A considerable reduction in surface defects (melted material deposition, micro-cracks, globules of debris, and micro-pores) owing to the addition of Al2O3 nanopowder (from 0 g/L to 2 g/L) was observed in the surface morphology analysis.

Author Contributions

Conceptualization, R.C., P.P., J.V., K.G., V.K.P. and D.Y.P.; methodology, R.C. and P.P.; software, V.K.P. and S.K.; validation, R.C., J.V., P.P. and S.K.; formal analysis, J.V. and R.C.; investigation, R.C., K.G. and D.Y.P.; resources, V.K.P. and S.K.; data curation, R.C.; writing—original draft preparation, P.P. and R.C.; writing—review and editing, J.V., R.C., V.K.P. and K.G.; visualization, R.C. and S.K.; supervision, J.V., K.G., R.C. and D.Y.P. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not Applicable.

Informed Consent Statement

Not Applicable.

Data Availability Statement

Data presented in this study are available in this article.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Jani, J.M.; Leary, M.; Subic, A.; Gibson, M.A. A review of shape memory alloy research, applications and opportunities. Mater. Des. 2014, 56, 1078–1113. [Google Scholar] [CrossRef]
  2. Chaudhari, R.; Vora, J.J.; Patel, V.; López de Lacalle, L.; Parikh, D. Surface analysis of wire-electrical-discharge-machining-processed shape-memory alloys. Materials 2020, 13, 530. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  3. Khanna, S.; Marathey, P.; Patel, R.; Paneliya, S.; Chaudhari, R.; Vora, J.; Ray, A.; Banerjee, R.; Mukhopadhyay, I. Unravelling camphor mediated synthesis of TiO2 nanorods over shape memory alloy for efficient energy harvesting. Appl. Surf. Sci. 2021, 541, 148489. [Google Scholar] [CrossRef]
  4. Khanna, S.; Marathey, P.; Paneliya, S.; Vinchhi, P.; Chaudhari, R.; Vora, J. Fabrication of graphene/Titania nanograss composite on shape memory alloy as photoanodes for photoelectrochemical studies: Role of the graphene. Int. J. Hydrogen Energy, 2022; in press. [Google Scholar]
  5. Vora, J.; Jain, A.; Sheth, M.; Gajjar, K.; Abhishek, K.; Chaudhari, R. A Review on Machining Aspects of Shape Memory Alloys. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2022; pp. 449–458. [Google Scholar]
  6. Rathi, P.; Ghiya, R.; Shah, H.; Srivastava, P.; Patel, S.; Chaudhari, R.; Vora, J. Multi-response Optimization of Ni55. 8Ti Shape Memory Alloy Using Taguchi–Grey Relational Analysis Approach. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2020; pp. 13–23. [Google Scholar]
  7. Kaya, E.; Kaya, İ. A review on machining of NiTi shape memory alloys: The process and post process perspective. Int. J. Adv. Manuf. Technol. 2019, 100, 2045–2087. [Google Scholar] [CrossRef]
  8. Manjaiah, M.; Narendranath, S.; Basavarajappa, S. Review on non-conventional machining of shape memory alloys. Trans. Nonferrous Met. Soc. China 2014, 24, 12–21. [Google Scholar] [CrossRef]
  9. Chaudhari, R.; Vora, J.J.; Parikh, D. A review on applications of nitinol shape memory alloy. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2021; pp. 123–132. [Google Scholar]
  10. Khanna, S.; Marathey, P.; Paneliya, S.; Chaudhari, R.; Vora, J. Fabrication of rutile–TiO2 nanowire on shape memory alloy: A potential material for energy storage application. Mater. Today Proc. 2021, 50, 11–16. [Google Scholar] [CrossRef]
  11. Khanna, S.; Patel, R.; Marathey, P.; Chaudari, R.; Vora, J.; Banerjee, R.; Ray, A.; Mukhopadhyay, I. Growth of titanium dioxide nanorod over shape memory material using chemical vapor deposition for energy conversion application. Mater. Today Proc. 2020, 28, 475–479. [Google Scholar] [CrossRef]
  12. Hassan, M.; Mehrpouya, M.; Dawood, S. Review of the machining difficulties of nickel-titanium based shape memory alloys. Appl. Mech. Mater. 2014, 564, 533–537. [Google Scholar] [CrossRef]
  13. Chaudhari, R.; Sheth, M.; Patel, H.; Fuse, K.; Ayesta, I.; Lacalle, L.; Vora, J. Multi-response Optimization of Alumina Powder-Mixed WEDM Process Using Taguchi-TOPSIS Approach of Nitinol SMA. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2022; pp. 359–367. [Google Scholar]
  14. Velmurugan, C.; Senthilkumar, V.; Dinesh, S.; Arulkirubakaran, D. Machining of NiTi-shape memory alloys—A review. Mach. Sci. Technol. 2018, 22, 355–401. [Google Scholar] [CrossRef]
  15. Chaudhari, R.; Vora, J.J.; Patel, V.; Lacalle, L.; Parikh, D. Effect of WEDM process parameters on surface morphology of nitinol shape memory alloy. Materials 2020, 13, 4943. [Google Scholar] [CrossRef]
  16. Sheth, M.; Gajjar, K.; Jain, A.; Shah, V.; Patel, H.; Chaudhari, R.; Vora, J. Multi-objective optimization of inconel 718 using Combined approach of taguchi—Grey relational analysis. In Advances in Mechanical Engineering; Springer: Berlin/Heidelberg, Germany, 2021; pp. 229–235. [Google Scholar]
  17. Chaudhari, R.; Vora, J.; Parikh, D.; Wankhede, V.; Khanna, S. Multi-response Optimization of WEDM Parameters Using an Integrated Approach of RSM–GRA Analysis for Pure Titanium. J. Inst. Eng. Ser. D 2020, 101, 117–126. [Google Scholar] [CrossRef]
  18. Gupta, N.K.; Somani, N.; Prakash, C.; Singh, R.; Walia, A.S.; Singh, S.; Pruncu, C.I. Revealing the WEDM Process Parameters for the Machining of Pure and Heat-Treated Titanium (Ti-6Al-4V) Alloy. Materials 2021, 14, 2292. [Google Scholar] [CrossRef] [PubMed]
  19. Aggarwal, V.; Pruncu, C.I.; Singh, J.; Sharma, S.; Pimenov, D.Y. Empirical investigations during WEDM of Ni-27Cu-3.15 Al-2Fe-1.5 Mn based superalloy for high temperature corrosion resistance applications. Materials 2020, 13, 3470. [Google Scholar] [CrossRef]
  20. Mukhopadhyay, A.; Barman, T.K.; Sahoo, P.; Davim, J.P. Modeling and optimization of fractal dimension in wire electrical discharge machining of EN 31 steel using the ANN-GA approach. Materials 2019, 12, 454. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  21. Chaudhari, R.; Vora, J.J.; Pramanik, A.; Parikh, D. Optimization of Parameters of Spark Erosion Based Processes. In Spark Erosion Machining; CRC Press: Boca Raton, FL, USA, 2020; pp. 190–216. [Google Scholar]
  22. Chaudhari, R.; Patel, H.; Sheth, M.; Prajapati, N.; Fuse, K.; Abhishek, K.; Vora, J. Effect of Different Tool Electrodes (Wire) of WEDM Process of Inconel 718. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2022; pp. 317–327. [Google Scholar]
  23. Sen, B.; Hussain, S.A.I.; Gupta, A.D.; Gupta, M.K.; Pimenov, D.Y.; Mikołajczyk, T. Application of type-2 fuzzy AHP-ARAS for selecting optimal WEDM parameters. Metals 2021, 11, 42. [Google Scholar] [CrossRef]
  24. Chaudhari, R.; Vora, J.J.; Prabu, S.; Palani, I.; Patel, V.K.; Parikh, D. Pareto optimization of WEDM process parameters for machining a NiTi shape memory alloy using a combined approach of RSM and heat transfer search algorithm. Adv. Manuf. 2021, 9, 64–80. [Google Scholar] [CrossRef]
  25. Talla, G.; Gangopadhayay, S.; Biswas, C. State of the art in powder-mixed electric discharge machining: A review. Proc. Inst. Mech. Eng. Part B J. Eng. Manuf. 2017, 231, 2511–2526. [Google Scholar] [CrossRef]
  26. Vora, J.; Prajapati, N.; Patel, S.; Sheth, S.; Patel, A.; Khanna, S.; Ayesta, I.; Lacalle, L.; Chaudhari, R. Multi-response Optimization and Effect of Alumina Mixed with Dielectric Fluid on WEDM Process of Ti6Al4V. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2022; pp. 277–287. [Google Scholar]
  27. Joshi, A.Y.; Joshi, A.Y. A systematic review on powder mixed electrical discharge machining. Heliyon 2019, 5, e02963. [Google Scholar] [CrossRef] [Green Version]
  28. Abdudeen, A.; Abu Qudeiri, J.E.; Kareem, A.; Ahammed, T.; Ziout, A. Recent advances and perceptive insights into powder-mixed dielectric fluid of EDM. Micromachines 2020, 11, 754. [Google Scholar] [CrossRef]
  29. Kumar, A.; Maheshwari, S.; Sharma, C.; Beri, N. A study of multiobjective parametric optimization of silicon abrasive mixed electrical discharge machining of tool steel. Mater. Manuf. Processes 2010, 25, 1041–1047. [Google Scholar] [CrossRef]
  30. Prakash, C.; Kansal, H.; Pabla, B.; Puri, S. Experimental investigations in powder mixed electric discharge machining of Ti–35Nb–7Ta–5Zrβ-titanium alloy. Mater. Manuf. Processes 2017, 32, 274–285. [Google Scholar] [CrossRef]
  31. Kumar, A.; Mandal, A.; Dixit, A.R.; Das, A.K.; Kumar, S.; Ranjan, R. Comparison in the performance of EDM and NPMEDM using Al 2 O 3 nanopowder as an impurity in DI water dielectric. Int. J. Adv. Manuf. Technol. 2019, 100, 1327–1339. [Google Scholar] [CrossRef]
  32. Sahu, D.R.; Mandal, A. Critical analysis of surface integrity parameters and dimensional accuracy in powder-mixed EDM. Mater. Manuf. Processes 2020, 35, 430–441. [Google Scholar] [CrossRef]
  33. Kumar, A.; Mandal, A.; Dixit, A.R.; Das, A.K. Performance evaluation of Al2O3 nano powder mixed dielectric for electric discharge machining of Inconel 825. Mater. Manuf. Processes 2018, 33, 986–995. [Google Scholar] [CrossRef]
  34. Tan, P.; Yeo, S. Investigation of recast layers generated by a powder-mixed dielectric micro electrical discharge machining process. Proc. Inst. Mech. Eng. Part B J. Eng. Manuf. 2011, 225, 1051–1062. [Google Scholar] [CrossRef]
  35. Alhodaib, A.; Shandilya, P.; Rouniyar, A.K.; Bisaria, H. Experimental Investigation on Silicon Powder Mixed-EDM of Nimonic-90 Superalloy. Metals 2021, 11, 1673. [Google Scholar] [CrossRef]
  36. Kumar, V.; Kumar, A.; Kumar, S.; Singh, N. Comparative study of powder mixed EDM and conventional EDM using response surface methodology. Mater. Today Proc. 2018, 5, 18089–18094. [Google Scholar] [CrossRef]
  37. Patel, S.; Thesiya, D.; Rajurkar, A. Aluminium powder mixed rotary electric discharge machining (PMEDM) on Inconel 718. Aust. J. Mech. Eng. 2018, 16, 21–30. [Google Scholar] [CrossRef]
  38. Bhattacharya, A.; Batish, A.; Singh, G. Optimization of powder mixed electric discharge machining using dummy treated experimental design with analytic hierarchy process. Proc. Inst. Mech. Eng. Part B J. Eng. Manuf. 2012, 226, 103–116. [Google Scholar] [CrossRef]
  39. Chaudhari, R.; Shah, H.; Ayesta, I.; Lacalle, L.; Vora, J. Experimental Investigations and Optimization of WEDM Parameters Using Taguchi Analysis of Pure Titanium. In Recent Advances in Mechanical Infrastructure; Springer: Berlin/Heidelberg, Germany, 2022; pp. 349–358. [Google Scholar]
  40. Chaudhari, R.; Khanna, S.; Vora, J.; Patel, V.K.; Paneliya, S.; Pimenov, D.Y.; Giasin, K.; Wojciechowski, S. Experimental investigations and optimization of MWCNTs-mixed WEDM process parameters of nitinol shape memory alloy. J. Mater. Res. Technol. 2021, 15, 2152–2169. [Google Scholar] [CrossRef]
  41. Sharma, P.; Chakradhar, D.; Narendranath, S. Measurement of WEDM performance characteristics of aero-engine alloy using RSM-based TLBO algorithm. Measurement 2021, 179, 109483. [Google Scholar] [CrossRef]
  42. Sibalija, T.V.; Kumar, S.; Patel, G.M. A soft computing-based study on WEDM optimization in processing Inconel 625. Neural Comput. Appl. 2021, 33, 11985–12006. [Google Scholar] [CrossRef]
  43. Mohammed, A.A.; Khodair, Z.T.; Khadom, A.A. Preparation and investigation of the structural properties of α-Al2O3 nanoparticles using the sol-gel method. Chem. Data Collect. 2020, 29, 100531. [Google Scholar] [CrossRef]
  44. Cava, S.; Tebcherani, S.M.; Souza, I.A.; Pianaro, S.A.; Paskocimas, C.A.; Longo, E.; Varela, J.A. Structural characterization of phase transition of Al2O3 nanopowders obtained by polymeric precursor method. Mater. Chem. Phys. 2007, 103, 394–399. [Google Scholar] [CrossRef]
  45. Wankhede, V.; Jagetiya, D.; Joshi, A.; Chaudhari, R. Experimental investigation of FDM process parameters using Taguchi analysis. Mater. Today Proc. 2020, 27, 2117–2120. [Google Scholar] [CrossRef]
  46. Chaurasia, A.; Wankhede, V.; Chaudhari, R. Experimental investigation of high-speed turning of INCONEL 718 using PVD-coated carbide tool under wet condition. In Innovations in Infrastructure; Springer: Berlin/Heidelberg, Germany, 2019; pp. 367–374. [Google Scholar]
  47. Vora, J.; Chaudhari, R.; Patel, C.; Pimenov, D.Y.; Patel, V.K.; Giasin, K.; Sharma, S. Experimental Investigations and Pareto Optimization of Fiber Laser Cutting Process of Ti6Al4V. Metals 2021, 11, 1461. [Google Scholar] [CrossRef]
  48. Fuse, K.; Chaudhari, R.; Vora, J.; Patel, V.K.; de Lacalle, L.N.L. Multi-Response Optimization of Abrasive Waterjet Machining of Ti6Al4V Using Integrated Approach of Utilized Heat Transfer Search Algorithm and RSM. Materials 2021, 14, 7746. [Google Scholar] [CrossRef]
  49. Selvakumar, G.; Chandrasekhara, S.C. Experimental Investigation of Wire-EDM Machining of Low Conductive Al-SiC-TiC Metal Matrix Composite. Metals 2020, 10, 1188. [Google Scholar]
  50. Fuse, K.; Dalsaniya, A.; Modi, D.; Vora, J.; Pimenov, D.Y.; Giasin, K.; Prajapati, P.; Chaudhari, R.; Wojciechowski, S. Integration of Fuzzy AHP and Fuzzy TOPSIS Methods for Wire Electric Discharge Machining of Titanium (Ti6Al4V) Alloy Using RSM. Materials 2021, 14, 7408. [Google Scholar] [CrossRef]
  51. Dzionk, S.; Siemiątkowski, M.S. Studying the effect of working conditions on WEDM machining performance of super alloy Inconel 617. Machines 2020, 8, 54. [Google Scholar] [CrossRef]
  52. Lalwani, V.; Sharma, P.; Pruncu, C.I.; Unune, D.R. Response surface methodology and artificial neural network-based models for predicting performance of wire electrical discharge machining of inconel 718 alloy. J. Manuf. Mater. Processing 2020, 4, 44. [Google Scholar] [CrossRef]
  53. Chaudhari, R.; Vora, J.J.; Mani Prabu, S.; Palani, I.; Patel, V.K.; Parikh, D.; de Lacalle, L.N.L. Multi-response optimization of WEDM process parameters for machining of superelastic nitinol shape-memory alloy using a heat-transfer search algorithm. Materials 2019, 12, 1277. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  54. Vora, J.; Patel, V.K.; Srinivasan, S.; Chaudhari, R.; Pimenov, D.Y.; Giasin, K.; Sharma, S. Optimization of Activated Tungsten Inert Gas Welding Process Parameters Using Heat Transfer Search Algorithm: With Experimental Validation Using Case Studies. Metals 2021, 11, 981. [Google Scholar] [CrossRef]
  55. Batish, A.; Bhattacharya, A.; Singla, V.; Singh, G. Study of material transfer mechanism in die steels using powder mixed electric discharge machining. Mater. Manuf. Processes 2012, 27, 449–456. [Google Scholar] [CrossRef]
  56. Ramesh, S.; Jenarthanan, M. Investigating the performance of powder mixed electric discharge machining of Nimonic 75 by using different tool materials. World J. Eng. 2018, 15, 205–215. [Google Scholar]
  57. Shard, A.; Shikha, D.; Gupta, V.; Garg, M. Effect of B 4 C abrasive mixed into dielectric fluid on electrical discharge machining. J. Braz. Soc. Mech. Sci. Eng. 2018, 40, 1–11. [Google Scholar] [CrossRef]
  58. Sahu, S.K.; Datta, S. Experimental studies on graphite powder-mixed electro-discharge machining of Inconel 718 super alloys: Comparison with conventional electro-discharge machining. Proc. Inst. Mech. Eng. Part E J. Process Mech. Eng. 2019, 233, 384–402. [Google Scholar] [CrossRef]
  59. Lenin, N.; Sivakumar, M.; Selvakumar, G.; Rajamani, D.; Sivalingam, V.; Gupta, M.K.; Mikolajczyk, T.; Pimenov, D.Y. Optimization of Process Control Parameters for WEDM of Al-LM25/Fly Ash/B4C Hybrid Composites Using Evolutionary Algorithms: A Comparative Study. Metals 2021, 11, 1105. [Google Scholar] [CrossRef]
  60. Vakharia, V.; Vora, J.; Khanna, S.; Chaudhari, R.; Shah, M.; Pimenov, D.Y.; Giasin, K.; Prajapati, P.; Wojciechowski, S. Experimental investigations and prediction of WEDMed surface of Nitinol SMA using SinGAN and DenseNet deep learning model. J. Mater. Res. Technol. 2022; in press. [Google Scholar] [CrossRef]
  61. Abed, F.N.; Shather, S.K. Influence of Additive Alumina Nanopowder on Surface Roughness during WEDM Process. In Proceedings of the IOP Conference Series: Materials Science and Engineering, Baghdad, Iraq, 15–16 December 2020; p. 012139. [Google Scholar]
  62. Goyal, K.K.; Sharma, N.; Dev Gupta, R.; Singh, G.; Rani, D.; Banga, H.K.; Kumar, R.; Pimenov, D.Y.; Giasin, K. A Soft Computing-Based Analysis of Cutting Rate and Recast Layer Thickness for AZ31 Alloy on WEDM Using RSM-MOPSO. Materials 2022, 15, 635. [Google Scholar] [CrossRef]
  63. Govindan, P.; Joshi, S.S. Analysis of micro-cracks on machined surfaces in dry electrical discharge machining. J. Manuf. Processes 2012, 14, 277–288. [Google Scholar] [CrossRef]
  64. Rouniyar, A.K.; Shandilya, P. Experimental investigation on recast layer and surface roughness on Aluminum 6061 alloy during magnetic field assisted powder mixed electrical discharge machining. J. Mater. Eng. Perform. 2020, 29, 7981–7992. [Google Scholar] [CrossRef]
  65. Wu, K.L.; Yan, B.H.; Huang, F.Y.; Chen, S.C. Improvement of surface finish on SKD steel using electro-discharge machining with aluminum and surfactant added dielectric. Int. J. Mach. Tools Manuf. 2005, 45, 1195–1201. [Google Scholar] [CrossRef]
  66. Chaudhari, R.; Vora, J.; Lacalle, L.; Khanna, S.; Patel, V.K.; Ayesta, I. Parametric Optimization and Effect of Nano-Graphene Mixed Dielectric Fluid on Performance of Wire Electrical Discharge Machining Process of Ni55. 8Ti Shape Memory Alloy. Materials 2021, 14, 2533. [Google Scholar] [CrossRef]
  67. Khan, A.A.; Ndaliman, M.B.; Zain, Z.M.; Jamaludin, M.F.; Patthi, U. Surface modification using electric discharge machining (EDM) with powder addition. Appl. Mech. Mater. 2012, 110–116, 725–733. [Google Scholar] [CrossRef]
Figure 1. Flowchart of the TLBO algorithm.
Figure 1. Flowchart of the TLBO algorithm.
Materials 15 02018 g001
Figure 2. Morphological and structural analysis of as prepared α-phase Al2O3: (a) FE-SEM, (b) EDX, (c) X-ray diffraction spectra, and (d) Raman Profile.
Figure 2. Morphological and structural analysis of as prepared α-phase Al2O3: (a) FE-SEM, (b) EDX, (c) X-ray diffraction spectra, and (d) Raman Profile.
Materials 15 02018 g002
Figure 3. Influence of WEDM variables on MRR.
Figure 3. Influence of WEDM variables on MRR.
Materials 15 02018 g003
Figure 4. Influence of WEDM variables on SR.
Figure 4. Influence of WEDM variables on SR.
Materials 15 02018 g004
Figure 5. Effect of input process parameters on RLT.
Figure 5. Effect of input process parameters on RLT.
Materials 15 02018 g005
Figure 6. 3D Pareto graph of MRR vs. SR vs. Kerf taper angle.
Figure 6. 3D Pareto graph of MRR vs. SR vs. Kerf taper angle.
Materials 15 02018 g006
Figure 7. 2D Pareto graph (a) MRR vs. SR, (b) MRR vs. RLT, and (c) SR vs. RLT.
Figure 7. 2D Pareto graph (a) MRR vs. SR, (b) MRR vs. RLT, and (c) SR vs. RLT.
Materials 15 02018 g007
Figure 8. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 0 g/L.
Figure 8. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 0 g/L.
Materials 15 02018 g008
Figure 9. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 1 g/L.
Figure 9. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 1 g/L.
Materials 15 02018 g009
Figure 10. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 2 g/L.
Figure 10. Surface morphology at Ton = 31 µs, Toff = 12 µs, and Al2O3 amount = 2 g/L.
Materials 15 02018 g010
Table 1. Experimental conditions of PMWEDM operation.
Table 1. Experimental conditions of PMWEDM operation.
Working ConditionDescription
Pulse-on time (µs)30, 60, 90
Pulse-off time (µs)5, 10, 15
Al2O3 concentration (g/L)0, 1, 2
Discharge current (A)3
Graphene nanopowder-size (nm)100
Powder Al2O3
Wire Molybdenum
Table 2. Taguchi’s L9 OA and the measured values of MRR, SR, and RLT.
Table 2. Taguchi’s L9 OA and the measured values of MRR, SR, and RLT.
RunTon (µs)Toff (µs)Al2O3 Conc. (g/L)MRR (g/min)SR (µm)RLT (µm)
130500.0840734.05614.160
2301510.1146453.74413.120
3302520.1272663.46411.728
460510.1558654.60816.240
5601520.1712594.33614.576
6602500.0704164.29615.000
790520.2010435.22418.328
8901500.0877975.13617.904
9902510.1175595.04017.584
Table 3. ANOVA for MRR.
Table 3. ANOVA for MRR.
SourceDFSSMSFp% Contr.
Regression30.0147450.00491573.710.000
Ton10.0010780.00107816.160.0107.14
Toff10.0026350.00263539.520.00117.47
Al2O3 Conc.10.0110320.011032165.440.00073.16
Error50.0003330.000067 2.23
Total80.015079
R-Sq. = 97.79%, R-Sq. (Adj.) = 96.82%, R-Sq. (pred.) = 91.78%.
Table 4. ANOVA for SR.
Table 4. ANOVA for SR.
SourceDFSSMSFp% Contr.
Regression33.084261.02809275.010.000
Ton12.851082.85108762.670.00091.88
Toff10.197290.1972952.780.0016.36
Al2O3 Conc.10.035880.035889.600.0271.17
Error50.018690.00374 0.58
Total83.10295
R-Sq. = 99.40%, R-Sq. (Adj.) = 99.04%, R-Sq. (pred.) = 97.71%.
Table 5. ANOVA for RLT.
Table 5. ANOVA for RLT.
SourceDFSSMSFp% Contr.
Regression340.782113.590114.250.000
Ton136.546136.5461307.140.00088.3
Toff13.25023.250227.310.0037.85
Al2O3 Conc.10.98580.98588.280.0353.38
Error50.59490.1190 0.47
Total841.3770
R-Sq. = 98.56%, R-Sq. (Adj.) = 97.70%, R-Sq. (pred.) = 95.83%.
Table 6. Single-objective optimization results.
Table 6. Single-objective optimization results.
Objective FunctionTon (µs)Toff (µs)Powder Conc. (g/L)MRR (g/min)SR (µm)RLT (µm)
Maximum MRR90520.32285.9420.59
Minimum SR302520.19883.1310.24
Minimum RLT302520.19883.1310.24
Table 7. Pareto optimal points obtained from HTS algorithm.
Table 7. Pareto optimal points obtained from HTS algorithm.
Sr. No.Pulse on Time (µs)Pulse off Time (µs)Powder Conc. (g/L)MRR (g/min)SR (µm)RLT (µm)
190520.32285.9420.59
2302520.19883.1310.24
382520.31755.6619.60
485520.31955.7619.97
532620.27983.9013.29
634520.28534.0113.68
778520.31485.5219.11
889520.32215.9020.47
945520.29274.3915.04
10301720.23233.4311.42
11302320.20723.2110.54
12302420.20303.1710.39
13301320.24913.5712.01
1430820.27003.7612.75
15311920.22463.3911.25
1630720.27423.7912.89
1730620.27843.8313.04
1872520.31085.3218.37
1965520.30615.0717.51
2070520.30945.2518.12
2151520.29674.5915.78
2276520.31345.4518.86
2374520.31215.3818.62
2448520.29474.4915.41
2536520.28664.0713.93
2642520.29074.2814.67
2738520.28804.1414.17
2842520.29074.2814.67
29301020.26173.6812.45
3054520.29874.7016.15
3157520.30074.8016.52
3267520.30745.1417.75
3368520.30815.1817.88
34302020.21983.3210.98
3538520.28804.1414.17
36302020.21983.3210.98
37311220.25393.6512.28
38302120.21563.2810.83
3930920.26593.7212.60
40301420.24493.5411.86
41311120.25813.6812.43
42302120.21563.2810.83
43302220.21143.2410.68
44302220.21143.2410.68
45301420.24493.5411.86
4630920.26593.7212.60
47311620.23723.5011.69
4859520.30204.8716.77
Table 8. Confirmatory trials.
Table 8. Confirmatory trials.
Sr. No.Ton (µs)Toff (µs)Powder (g/L)Prediction from TLBOActual Experimental Values% Error
MRRSRRLTMRRSRRLTMRRSRRLT
190520.32285.9420.590.33815.7320.884.523.661.38
2302520.19883.1310.240.20733.1110.114.100.641.28
3054520.29874.7016.150.28924.9216.673.284.473.11
37311220.25393.6512.280.24993.7811.981.603.432.5
47311620.23723.5011.690.24323.4112.012.462.632.66
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Chaudhari, R.; Prajapati, P.; Khanna, S.; Vora, J.; Patel, V.K.; Pimenov, D.Y.; Giasin, K. Multi-Response Optimization of Al2O3 Nanopowder-Mixed Wire Electrical Discharge Machining Process Parameters of Nitinol Shape Memory Alloy. Materials 2022, 15, 2018. https://doi.org/10.3390/ma15062018

AMA Style

Chaudhari R, Prajapati P, Khanna S, Vora J, Patel VK, Pimenov DY, Giasin K. Multi-Response Optimization of Al2O3 Nanopowder-Mixed Wire Electrical Discharge Machining Process Parameters of Nitinol Shape Memory Alloy. Materials. 2022; 15(6):2018. https://doi.org/10.3390/ma15062018

Chicago/Turabian Style

Chaudhari, Rakesh, Parth Prajapati, Sakshum Khanna, Jay Vora, Vivek K. Patel, Danil Yurievich Pimenov, and Khaled Giasin. 2022. "Multi-Response Optimization of Al2O3 Nanopowder-Mixed Wire Electrical Discharge Machining Process Parameters of Nitinol Shape Memory Alloy" Materials 15, no. 6: 2018. https://doi.org/10.3390/ma15062018

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop