J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... 349–356 EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS PARAMETERS TO OBTAIN THE MINIMUM SURFACE ROUGHNESS OF THE Al 7075 ALUMINIUM ALLOY EMPLOYED WITH A ZINC-COATED WIRE USING RSM AND GA EKSPERIMENTALNA RAZISKAVA OPTIMIZACIJE PROCESNIH PARAMETROV @I^NE EROZIJE S CINKOM OPLA[^ENE Cu @ICE ZA ZAGOTOVITEV MINIMALNE POVR[INSKE HRAPAVOSTI Al ZLITINE 7075 Z UPORABO POSTOPKOV RSM IN GA Shanthi Jayachandran 1* , Mohan Raman 2 , Thangavelu Ramasamy 3 1 Renovation and Modernisation Division, Mettur Thermal Power Station-I, Mettur -636406, Tamilnadu, India 2 Department of Mechanical Engineering, Sona College of Technology, Salem-636005, Tamilnadu, India 3 Renovation and Modernisation Division, Mettur Thermal Power Station-I, Mettur-636406, Tamilnadu, India Prejem rokopisa – received: 2018-07-28; sprejem za objavo – accepted for publication: 2018-12-17 doi:10.17222/mit.2018.166 Wire Electrical Discharge Machining (WEDM) is widely used for machining conductive materials of intricate, complex and challenging shapes in the field of aerospace, die and mould making, automobile industries and the medical field. Proper selection of the WEDM process parameters can give good responses. Out of the various process responses, to achieve the minimum surface roughness is very difficult, due to arcing by the electrical discharge. The present investigation has been made to optimize the process parameters of WEDM during machining the Al 7075 aluminium alloy with zinc-coated copper wire using the Response Surface Methodology (RSM). Four input process parameters of WEDM, i.e., Pulse On Time, Pulse Off Time, Wire Feed and Wire Tension, were chosen as the process variables to study the process performance and to obtain the minimum surface roughness. An analysis of variance (ANOVA) was carried out to study the effect of the process parameters on the surface roughness and a mathematical model was developed. The model has been verified and checked for adequacy. The best fit surface roughness (Ra) value predicted is 1.048 μm for a Pulse On (TON) value of 120 μsec, a Pulse Off (TOFF) value of 58 μsec, a Wire Feed (WF) of 3 m/min and a Wire Tension (WT) value of 9 gm. Furthermore, it is observed that with an increase in the pulse-on time the Surface Roughness also increases, and an increase in the pulse-off time and the wire tension, the Surface Roughness decreases. Wire Feed does not influence much on the Surface Roughness. Keywords:WEDM (Wire Electrical Discharge Machining), optimisation, surface roughness, RSM, GA, Al 7075 @i~na erozija (WEDM; angl.: Wire Electrical Discharge Machining) se pogosto uporablja za obdelavo in rezanje kompleksno oblikovanih izdelkov, modelov in orodij iz prevodnih materialov v letalski, orodjarski, modelarski in avtomobilski industriji ter v zdravstvu. Pri tem postopku je zelo pomembna izbira ustreznih procesnih parametrov WEDM. Doseganje minimalne povr{inske hrapavosti reza je zelo zahtevno zaradi nastajajo~ega talilnega obloka med razelektrevanjem. Avtorji so optimizirali procesne parametre WEDM, ki uporablja s cinkom opla{~eno bakreno `ico med mehansko obdelavo Al zlitine 7075 z uporabo metodologije odgovora povr{ine (RSM, angl.: Response Surface Methodology). Izbrali so {tiri vhodne procesne parametre WEDM, in sicer: ~as vklopa (TON) in izklopa (TOFF) elektri~nega impulza, hitrost dovajanja `ice WF in napetost `ice WT kot spremenljivke za {tudij vpliva procesa na zagotovitev minimalne hrapavosti. Z analizo variance (ANOVA) so raziskovali vpliv procesnih parametrov na povr{insko hrapavost in na njeni osnovi razvili matemati~ni model. Model so verificirali in preizkusili njegovo ustreznost. Najbolj{e ujemanje vrednosti za povr{insko hrapavost (Ra) je bilo 1,048 μm pri TON vrednosti 120 μsec, TOFF vrednosti 58 μsec, hitrosti dovajanja `ice WF 3 m/min ter napetosti `ice WT 9 mN/m. Avtorji ugotavljajo, da se je z nadaljnjim podalj{evanjem ~asa TON pove~evala povr{inska hrapavost. S podalj{evanjem ~asa TOFF in pove~evanjem napetosti `ice pa se je povr{inska hrapavost zmanj{evala. Hitrost dovajanja `ice ni pomembno vplivala na povr{insko hrapavost. Klju~ne besede: WEDM – `i~na erozija, optimizacija, povr{inska hrapavost, RSM, GA, Al zlitina 7075 1 INTRODUCTION Several researchers investigated the different aspects of WEDM, but no comprehensive research work has been reported so far in the field of wire electrical discharge machining of this Al 7075 alloy using zinc-coated copper wire. Hence, an attempt was made to explore the influences of selected variable process para- meters. G. E. Totten and D. S. Mackenzie 1 reported the ma- chinability ratings of aluminium alloys span into five groups, with ratings of A, B, C, D and E, which are ordered in increasing order of chip length and decreasing order of surface quality. The Al 5083 aluminium alloy ranked D is an indicator for poor machinability. WEDM is one of the latest machining techniques to process the Al 5083 aluminium alloy to any complex intricate shapes with high accuracy and precision when comparing with diamond-based cutting tools. J. Prohaszka et al. 2 inves- tigated the effect of electrode material coating with zinc, tin and magnesium on machinability in the WEDM pro- Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 349 UDK 620.1:669.715:620.191.35 ISSN 1580-2949 Original scientific article/Izvirni znanstveni ~lanek MTAEC9, 53(3)349(2019) *Corresponding author e-mail: shanthi_jc@yahoo.com (Shanthi Jayachandran) cess. These coating materials are required for improving the cutting efficiency because the existing wires do not fulfill all the requirements. R. Chalisgaonkar and J. Kumar 3 explored the characteristics of pure titanium dur- ing rough cut operation, and after the finish cut oper- ation, they revealed the microstructure analysis of zinc- coated and in the uncoated wires the erosion during the rough cut operation was found to be more than the finish cut. B. Sivaraman et al. 4 stated that in the WEDM process the Taguchi method is most ideal and suitable, it sim- plifies the optimisation of multiple performance charac- teristics by avoiding complicated mathematical compu- tations. G. Selvakumar et al. 5 presented an optimum input-parameter combination for the minimum Ra and the maximum MRR was obtained by an analysis of the signal-to-noise (S/N) ratio and the process was opti- mized by a Pareto-optimality approach by machining the Al 5083 aluminium alloy. D. Siva Prasad et al. 6 inves- tigated the effect of different WEDM process parameters on the damping behavior of the A 356.2 aluminum alloy. The damping capacity of this alloy increases with an increase in the frequency and increasing Pulse On. A. Dey et al. 7 examined the machinability of the cenosphere fly-ash reinforced Al 6061 aluminium alloys for various combinations of the input process para- meters. The optimal combination of process parameters was arrived at for the maximum MRR, the minimum Tool Wear Rate and the minimum R a .K.H.Hoetal. 8 carried out the WEDM process by understanding the interrelationship between the various factors affecting the process and identified the optimal machining con- dition from the infinite number of combinations. The adaptive monitoring and control systems were imple- mented to tame the transient WEDM behaviour without the risk of wire breakages. S. Kuriakose and M. S. Shunmugam 9 investigated the optimal parameters of the WEDM process for improving the cutting performance. There is no single optimal combination of cutting parameters, as their influences on the cutting velocity and the surface finish are quite the opposite. In the present work, a multiple regression model is used to represent the relationship between the input and output variables and a multi-objective optimization method based on a Non-Dominated Sorting Genetic Algorithm (NSGA) is used to optimize the WEDM process. A. Sharma et al. 10 made an attempt to machine an Al 6063 / ZrSiO4(p) (5 %) metal-matrix composite using WEDM. The objective was to investigate the influence of the process parameters, i.e., T ON , T OFF , Peak Current and SV on the Cutting Rate and found experimentally that increasing the T ON and Peak current, the cutting rate increases, whereas increasing the T OFF and SV decreases the cutting rate. The higher discharge energy associated with the increased T ON , Peak Current and lesser TOFF and SV leads to more powerful explosions, which in- crease the cutting rate. H. C. Tsai et al. 11 investigated the electrode performance and revealed that wires generally used are of brass or copper with a diameter of about 0.3–0.5 mm, but in recent times coated wires are widely used, usually zinc coated over brass wire. The impacts of coated wires were found to have a significant effect. The productivity and surface roughness were found to be better than uncoated wires. Several authors 12–14 also suggested that the concentration of electrical discharges at a certain point of the wire, which causes an increase in the localized temperature, resulting in the breakage of the wire. V. Chengal Reddy et al. 15 discussed the effects of the input control parameters, such as T ON , T OFF , Cur- rent, WT, upper flush and lower flush on the R a , MRR and Kerf Width, while machining the aluminum HE 30 material and suggested the selection of the right com- bination of input parameters by Grey Relational Analysis (GRA). Dain Thomas et al. 16 , developed a second-order regression model using RSM and found that T ON and WT play a major role in the surface roughness. V. R. Surya et al. 17 predicted the machining characteristics of an Al 7075-TiB2 composite using ANN for the maximum MRR, minimum Dimensional Error (DE) and better surface finish. In this study the control factors considered were T ON , T OFF , Current and Bed Speed based on Taguchi’s L 27 orthogonal array. S. Prashantha et al. 18 investigated the Al 6061 aluminium alloy reinforced with SiC particles by varying the percentage of SiC from 3 %, 6%and9%byweight. T ON , T OFF , Current (I) and Bed speed (BS) are varied to find their effects on the MRR. From the analysis, the average MRR for an unreinforced Al 6061 aluminium alloy is 9.2 mm 3 /min and the average MRR is 9.15 mm 3 /min, 9.13 mm 3 /min and 9 mm 3 /min, respectively for Al 6061 aluminium alloy MMCs with 3 %, 6 % and 9 % SiC, i.e., the MRR decreases with an increase of the silicon carbide particles. S. Prasad Ari- katla et al. 19 executed a study on a titanium alloy using RSM in WEDM and registered the quality of the machined surface by T ON & Input Power and WT&SV . In the I case Ra increases while in the II case Ra de- creases. G. Amitesh and K. Jatinder 20 investigated the influence of machining parameters on the material removal rate and the cutting speed for the machining of Nimonic 80 A with Brass wire as the electrode in wire electrical discharge machining. From the observation, the cutting speed (CS) and MRR both increase with an increase in T ON and the Peak Current (IP). Furthermore, it decreases with an increase in T OFF and the spark gap set voltage. M. T. Antar et al. 21 explored the role of coated wire in the production and surface integrity, while machining aerospace alloys in WEDM. Coated wires are stated to protect the core from thermal shock and also from wire rupture. Its other effects were found on vibra- tion, damping effect, heat transfer and resistance, which ultimately increased the machining speed. N. Kinoshita et al. 22 observed that wire breaks due to a rapid rise in the pulse frequency of the gap voltage. They developed a monitoring and control system that switches off the pulse generator and the servo system, preventing the wire from breaking, but it affects the machining efficiency. The above literature review indicates that most of the researchers have considered the influence of a limited J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... 350 Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 number of control parameters on the performance measures of Wire Electric Discharge Machined parts. Furthermore, from the literature review it is understand- able that the impact of coated wires was found to improve the productivity and surface finish, better than uncoated wires. Hence, it is intended to investigate the effect of the selected variable process parameters on the surface roughness, while machining with zinc-coated copper wire of diameter 0.25 mm. So far, no such inves- tigation was carried out on the Al 7075 aluminium alloy. In this study an attempt has been made to optimize the various WEDM process parameters such as T ON , T OFF , WF and WT to find out the best fit to obtain minimum R a . 2 EXPERIMENTAL PART 2.1 Work material As the Al 7075 Aluminium alloy is a lightweight ma- terial, zinc-based alloy and possesses excellent corrosion resistant, it is widely used in marine, aerospace applica- tions and in the medical field. Aluminium alloys have very good mechanical properties such as a high tensile strength, a very high yield strength, good fatigue strength, and superior corrosion resistance, and average machinability. However, these alloys were very difficult to fabricate as they are not ductile and have a low frac- ture toughness at room temperature. An unconventional machining process like WEDM is used intensively for a better process The response is to machine an aluminium alloy, due to its exceptional strength properties, whereas it is very difficult to machine in a conventional method. The analysis of the consequence of different process parameters is essential. 2.2 Machine tool WEDM requires thin, single-strand conducting metal wire that is used as the electrode. There are several elec- trode materials available, but brass wire is commercially used. The wire can either be coated wire (zinc, brass, tin, magnesium etc.) or uncoated wire (copper, brass, molyb- denum). This conducting wire is passed through the pre-drilled hole in the metal piece to be machined. The wire is fed from a spool and held between upper and lower guides tha are made of diamond, and in turn it is finally controlled by CNC and moved in the X-Y plane. This allows the wire-cut EDM to be programmed to cut very intricate, delicate and complex shapes. By using a pump, dielectric fluid (Deionised Water) is continuously passed over the work piece to remove, clear and flush out the debris that is cut from the work piece. When a D.C. supply is attached to the circuit, thousands of spark dis- charges occur across the gap between the wire and the work piece, which increases the temperature and causes the melting of material, erosion and even vaporizing and thus removing the metal from the work piece. The removed fine material particles are carried away by the dielectric fluid circulating around it. J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 351 Table 1: Al 7075 alloy composition in percentage by weight Al Cr Cu Fe Mg Mn Si Ti Zn others 87.1–91.4 0.18–0.28 1.2–2.0 Max 0.5 2.1–2.9 Max 0.3 Max 0.4 Max 0.2 5.1–6.1 Max 0.15 Figure 1: WEDM machine set up Table 2: Properties of Al 7075 Aluminium Alloy Sl. No. Property Value 1 Density 2.81 g/cc 2 Ultimate Tensile strength 572 MPa 3 Tensile Yield strength 503 Mpa 4 Elongation at break 11 % 5 Modulus of Elasticity 71.7 GPa 6 Poisson Ratio 0.33 7 Hardness Brinell 150 8 Fatigue strength 159 MPa 9 Shear Modulus 26.9 GPa 10 Machinability 70 % 11 Thermal Conductivity 130 W/m k 12 Melting Point 477–635 °C 13 Electrical Resistivity 5.15 e –006 cm 2.3 Specimen An Al 7075 aluminum alloy rectangular block of length 200 mm, width 16 mm and thickness 10 mm was taken as the work material. The experiment was per- formed on a WEDM machine with zinc-coated copper wire (tool) of 0.25 mm diameter and deionized water is used as the dielectric fluid. 2.4 Parameters considered in this experiment Table 3: Fixed parameters Sl. No. Parameter Unit value 1 Input Power V 230 2 Dielectric fluid pressure kg/cm 2 1 machine unit (low) 3 Pulse Peak Voltage V 2 machine unit 4 Servo Voltage V 20 5 Servo Frequency cycles/s 2100 Table 4: Variable parameters and range Sl. No. Parameter Unit From To 1 Pulse On (T ON ) μs 120 128 2 Pulse Off (T OFF )μ s5 05 8 3 Wire Feed (WF) m/min 1 3 4 Wire Tension (WT)N59 2.5 Experimental values Table 5: Experimental results of R a using L27 orthogonal array matrix Variable Process Parameters Response R a Error Re- marks Sl. no. Pulse on Pulse off Wire Feed Wire Ten- sion Exper- imen- tal RSM pre- dicted μs μs m/min N μm μm % 1 128 54 2 5 1.84 2.08 11.62 2 120 54 1 7 1.80 1.92 6.44 3 124 58 2 9 1.36 1.39 1.88 WB 4 124 58 1 7 1.91 1.95 1.95 5 124 50 2 5 1.79 2.19 18.12 l6 124 54 2 7 1.94 2.15 9.94 7 120 58 2 7 1.62 1.48 9.31 8 128 54 3 7 1.91 2.22 13.96 9 128 54 1 7 1.93 2.23 13.38 10 124 54 3 5 1.87 2.02 7.61 11 124 54 3 9 1.74 1.94 10.12 12 120 54 2 5 1.73 1.69 2.37 13 120 54 2 9 1.35 1.55 13.13 14 124 54 2 7 1.93 2.15 10.40 15 128 54 2 9 1.39 1.88 26.14 WB 16 128 50 2 7 1.98 2.47 19.97 17 124 50 1 7 1.86 2.27 17.99 18 124 50 3 7 2.11 2.52 16.14 19 120 54 3 7 1.67 1.80 7.43 20 128 58 2 7 1.62 1.62 0.12 21 124 54 2 7 1.98 2.15 8.08 22 124 54 1 5 2.02 2.17 6.83 23 120 50 2 7 1.55 1.89 17.99 24 124 54 1 9 1.73 1.92 9.90 25 124 50 2 9 1.65 2.11 21.95 26 124 58 2 5 1.70 1.65 3.03 WB 27 124 58 3 7 1.54 1.57 2.04 2.6 Surface roughness Roughness is a measure of the texture (quality) of the surface. It is quantified by the vertical deviations of the actual surface from its ideal form. If these deviations are large, the surface is rough; if they are small, the surface is smooth. The surface roughness R a was measured with a Mitutoyo Surftest 211 Surface Roughness tester and the values are tabulated in Table 5. 2.7 Response Surface Methodology (RSM) This is a collection of statistical and mathematical techniques useful for developing, improving and opti- mizing processes. RSM consists of an experimental approach to investigate the independent variables in the process, the experimental statistical model developed for an appropriate similar relationship between the yield and the process variables. Optimization methods for finding values of the process variables that produce desirable values of the responses. In order to investigate the effects of the WEDM parameters on the above-mentioned ma- chining criteria, second-order polynomial response sur- face mathematical models can be developed. In the gene- ral case, the response surface is described by an equation of the form: Y = 0 + j x j + jj x 2 j + ij x i x j (1) where Y is the response, in current research surface roughness, whereas the terms 0 , j , ij are second-order regression coefficients. The second term under the sum- mation sign of this polynomial equation is attributable to a linear effect, whereas the third term corresponds to the higher-order effects and the fourth term of the equation includes the interactive effects of the process parameters. The above equation can be rewritten as: Y = 0 + 1 X 1 + 2 X 2 + 3 X 3 + 4 X 4 + 11 X 12 + 22 X 22 + 33 X 32 + 44 X 42 +….. (2) J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... 352 Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 Figure 2: a) Work piece before machining and b) after machining The value of , the regression coefficient, will be determined by the least-squares method. 2.8 Wire breakage A wide variety of the control strategies preventing the wire from breaking are based on a knowledge of the characteristics of the wire. The breaking of the wire can be due to the excessive thermal load producing unwar- ranted heat on the wire. Most of the thermal energy generated during the WEDM process is transferred to the wire, while the rest is lost to the flushing fluid. However, when the instantaneous energy rate exceeds a certain limit depending on the thermal properties of the wire material, the wire will break. The WB in the Table 5 indicates the occurrence of wire breakage while conduct- ing the experiment, hence the corresponding set of parameters to be avoided for better performance. 3 RESULTS 3.1 Response Surface Methodology (RSM) The relationship between the selected variable pro- cess parameters and the response R a was obtained by a quadratic regression equation using RSM in Minitab. This regression equation is useful in predicting the response surface roughness with respect to the variable process parameters Pulse on Time (A), Pulse off Time (B), Wire Feed (C) and Wire Tension (D). R a = –231.114 + 2.903 A + 1.773 B + 0.866 C + 1.162 D – 0.01 A 2 – 0.008 B 2 + 0.05 C 2 – 0.048 D 2 – 0.007 A·B + 0.007 A·C – 0.002 A·D – 0.039 B·C – 0.006 B·D – 0.02 C·D Figure 3 shows the difference between the experi- mental and predicted R a . The error percentage was cal- culated based on the input variable process parameters and the predicted value, and tabulated in Table 5, and found to be reasonable. 3.2 Analysis of variance for R a Table 6: ANOVA result for R a Source DF Seq SS Adj MS F % Contri- bution Regression 14 1.02098 0.072927 15.96 Linear 4 0.45663 0.057484 12.58 Pulse on 1 0.07521 0.175001 38.31 6.99 Pulse off 1 0.11801 0.132032 28.90 10.97 Wire Feed 1 0.01401 0.002568 0.56 1.30 Wire Tension 1 0.24941 0.018231 3.99 23.18 Square 4 0.40138 0.100344 21.97 Pulse on* Pulse on 1 0.07993 0.140833 30.83 7.43 Pulse off* Pulse off 1 0.05184 0.083333 18.24 4.82 Wire Feed* Wire Feed 1 0.07707 0.133333 2.92 7.16 Wire Tension* Wire Tension 1 0.19253 0.192533 42.15 17.90 Interaction 6 0.16297 0.027162 5.95 Pulse on* Pulse off 1 0.04623 0.027162 10.12 4.30 Pulse on* Wire Feed 1 0.00302 0.046225 0.66 0.28 Pulse on* Wire Tension 1 0.00122 0.003025 0.27 0.11 Pulse off* Wire Feed 1 0.09610 0.001225 21.04 8.93 Pulse off* Wire Tension 1 0.01000 0.096100 2.19 0.93 Wire Feed* Wire Tension 1 0.00640 0.010000 1.40 0.59 Residual Error 12 0.05482 0.006400 Lack-of-Fit 10 0.05342 0.004568 7.63 Pure Error 2 0.00140 0.005342 Total 26 1.07580 0.000700 3.3 Contribution of the process variable parameter during machining Table 6 shows the results of the ANOVA for a 95 % confidence level of R a . It is observed from the table that foremost variable that affects R a is linear WT with a con- tribution of 23.18 %. The second important factor is squared WT with a contribution of 17.90 %, then linear T OFF with 10.97 % , interaction of T OFF × WF, squared T ON , squared WF, linear T ON, squared T OFF , interaction of T ON × T OF F and linear WF, with a contribution of (8.93, 7.43, 7.16, 6.99, 4.82, 4.30 and 1.30) % respectively. In addi- tion to the above, it is found that interaction of T OFF × WT, WF × WT, T ON × WF, T ON × WT contribution values are less than 1 %, which states that these interactions do not affect R a . Further, from Table 5, it is observed that the predicted values from RSM are close to the experi- mental values of R a . The higher correlation coefficient (R 2 ) of more than 90 % confirms the fitness of the model. Figure 4a shows the fitness of the experimental R a obtained to the predicted R a . It is observed that there is not much deviation found between the experimental value and the predicted value obtained from RSM. Fig- J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 353 Figure 3: Experimental vs. predicted values of R a ure 4b shows the effect plot for the SN ratios of the data mean of R a , R a is the minimum for the minimum T ON , maximum T OFF , moderate WF & maximum WT. R a is the maximum for mid-value T ON , minimum T OFF , minimum WF and WT. 3.4 Contour and surface plots of RSM 4 DISCUSSION 4.1 Discussion of contour plot and surface plot ob- tained from RSM Figure 5a depicts the effect of T ON and T OFF on R a when WF and WT are held constant, for the T ON value ranging from 123.5 μs to 128 μs and T OFF rate from 50 μs J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... 354 Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 Figure 5: Contour plot and surface plot of surface roughness: a) R a versus T OFF , T ON ,b)R a versus WF, T ON ,c)R a versus WT, T ON ,d)R a versus WF, T OFF ,e)R a versus WT, T OFF ,f)R a versus WT, WF Figure 4: a) Fitness of the experiment, b) effect of SN ratios to 54.5 μs, the R a value is a maximum (>1.90 μm). There is a gradual increase in the R a for the intermediate T OFF value and lower for higher and lower T OFF value, as the T ON value decreases the R a value also decreases. And for the T ON value ranging from 120 μs and T OFF value 50 μs, the R a value is a minimum (<1.60 μm). Figure 5b depicts the effect of T ON and WF on R a when T OFF and WT are held constant, for the T ON value ranging from 122.5 μs to 126.5 μs and for the WF value ranging between 1 m/min and 1.25 m/min, the R a value is a maximum (>2.00 μm), hence this condition should be avoided. As the T ON value decreases and WF increases simultaneously the R a value decreases. For the T ON value of 120 μs and the WF range from 2.5 m/min to 3.0 m/min, the R a value is a minimum (<1.7 μm). This is the ideal condition. Figure 5c depicts the effect of T ON and WT on R a when T OFF and WF are held constant, for the value of T ON ranging from 122.5 μs to 128 μs and for WTvalue5Nto 7N,theR a value is a maximum (>1.9 μm), for the T ON rate 120 μs to 121.5 μs and WT values from 8.5 N to 9 N, the R a value is a minimum (<1.4 μm). As the T ON value decreases and WT value increases simultaneously, the R a values decreases further for selected low T ON value and high WT value the R a value is found to be a minimum. Figure 5d depicts the effect of T OFF and WF on R a when T ON and WT are held constant, the R a value is a maximum (>2.0 μm ) for a T OFF value of 50 μs to 53 μs and WF value above 2.5 m/min, i.e., in general it is clear that for minimum T OFF value and maximum WF value the R a is a maximum. For a T OFF of more than 58 μs and WF value of 3.0 m/min, the R a is minimum (<1.6 μm) and for the other values of T OFF &WF, the R a value is medium. Figure 5e depicts the effect of T OFF and WT on R a when T ON and WF are held constant, it is observed that for the T OFF value ranging from 50 μs to 56 μs and WT value ranging from 5.5 N to 7.5 N, the R a value is a maximum (>1.9 μm), the Surface Roughness will be in the extreme condition, and for T OFF value exceeding 57.5 μs and WT value exceeding 8.7 N, the R a value is a minimum (<1.4 μm). As the T OFF and WT increases simultaneously the R a value decreases. Figure 5f depicts the effect of WF and WT on R a when T ON and T OFF are held constant. When the WF ranges from 1 m/min to 1.75 m/min and WT values ranges from5Nto7.3N,theR a value is a maximum (>2.0 μm) the Surface Roughness will be in the ex- cessive, which is an adverse condition. For the all values of WF and WT the value exceeding 8.8 N R a is a mini- mum (<1.7 μm), as WT increases R a decreases. 4.2 Simulation results obtained from the genetic algo- rithm The equation obtained from RSM, i.e., Equation (3), is used for the minimization of R a by using GA in MATLAB software to find the optimal selected variable process parameters for the best fit R a values. Where T ON , T OFF , WF and WT are 4 variables, the population size selected for this simulation is 100, the Rank is set as the Fitness Scaling Function, Stochastic uniform is set as the Selection Function, the Reproduction elite count is 2, the Cross over probability is 0.8, the Cross over function is scattered, the Mutation probability is 0.05, the Initial pe- nalty is 10, the Iteration is 100, the Number of genera- tions is 100, and the Stopping criteria is Best Fitness. The optimization function is formulated as Minimize R a (T ON , T OFF , WF, WT) Subject to the following condition: 120 μs < T ON > 128 μs 50 μs < T OFF >58 μs 1 m/min < WF > 3 m/min 5N9N Figure 6 depicts the best optimal solution for the Surface Roughness obtained in the simulation, for the input value of T ON – 120 μs, T OFF -58 μs, WF-3 m/min, WT-9 N the best fit Predicted R a Value is 1.048 μm. 4.3 Confirmation experiment Confirmatory experiments carried out for the input value of T ON 120 μs, T OFF 58 μs, WF 3 m/min, WT9N and the experimental R a value obtained is 1.08 μm and the error percentage between the predicted and experi- mental value is calculated as 3.05, which is less than 5 %. It confirms the excellent reproducibility of the results. Table 7 indicates the error obtained. Table 7: Comparison of the Optimized Process Parameter and its best fit R a value Sl. no. Parameter Values 1 Pulse On (TON ) 120 μs 2 Pulse Off (TOFF )5 8 μ s 3 Wire Feed (WF) 3 m/min 4 Wire Tension (WT)9 N Best Fit R a Value (Predicted) μm 1.048 Actual R a Value (Experimental) μm 1.08 Error % 3.05 J. SHANTHI et al.: EXPERIMENTAL INVESTIGATION FOR THE OPTIMIZATION OF THE WEDM PROCESS ... Materiali in tehnologije / Materials and technology 53 (2019) 3, 349–356 355 Figure 6: Predicted optimal solution of R a using GA 5 CONCLUSIONS The present work elucidates the effect of variable WEDM process parameters while machining an Al 7075 alloy is investigated by using zinc-coated copper wire, a quadratic model for the Surface Roughness was deve- loped, using RSM, to correlate the effects of the process parameters and the same is used in GA to establish the best fit R a . Based on the results obtained the following conclusions were furnished for machining of an Al 7075 alloy using zinc-coated copper wire. The best fit Surface Roughness value predicted is 1.048 μm for Pulse On (T ON ) value 120 μs, Pulse Off (T OFF ) value 58 μs, Wire Feed (WF) 3 m/min and for Wire Tension (WT) value 9 gm. It is observed that for the increase in the Pulse On time, the Surface Roughness also increases. The Surface Roughness decreases as the Pulse Off time increases. The increase in the Wire Tension leads to a decrease of the Surface Roughness. Wire Feed does not influence much on the Surface Roughness. For the maximum value of Pulse Off (T OFF ), Wire Feed (WF), the Wire Tension (WT) and minimum Pulse On (T ON ) the Surface Roughness predicted is a minimum, which is the ideal condition for improving the quality of machined parts. Furthermore, WEDM can be employed for ma- chining an Al 7075 alloy with other coated and uncoated wires in order to compare the machined surfaces. 6 REFERENCES 1 G. E. Totten, D. S. 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