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Effect of process parameters on the electrical discharge machining of aluminum metal matrix composites through a response surface methodology approach

  • V. Balasubramaniam , N. Baskar and Chinnaiyan Sathiya Narayanan EMAIL logo
Published/Copyright: September 26, 2014

Abstract

This work presents the multiobjective optimization of machining parameters during the electrical discharge machining (EDM) of aluminum (Al)-silicon carbide (SiC) metal matrix composites (MMC). The process parameters considered were current, pulse on-time, dielectric flushing pressure, and SiC particles. A copper rod was used as an electrode. An Al-SiC MMC with Al 6061 as matrix and SiC particles having three different sizes (i.e., 15, 25, and 40 μm) were used as workpieces. The experiments were planned using design of experiments through response surface methodology (RSM). The mathematical models were developed to predict the better performance measures such as the material removal rate (MRR), electrode wear rate (EWR), surface roughness (SR), and cylindricity (CY). The desirability approach in RSM was performed for optimization. It was found that the MRR increases with increasing peak current, pulse on-time, flushing pressure, and particle size. The EDM parameters are to be analyzed for the MRR, EWR, SR, and CY. The best one is proposed for validation.

1 Introduction

Electrical discharge machining (EDM), an unconventional machining process, is used to machine any complex shapes in any conductive workpieces irrespective of their hardness. In the EDM process, the material is removed from the workpiece by means of repetitive sparks struck between the tool and the workpiece material [1–3]. The EDM technology is increasingly being used in the tool, die, and mold-making industries for machining heat-treated tool steels and advanced materials such as super alloys, ceramics, and hard composite materials [4]. Among the composite materials, aluminum (Al)-based metal matrix composites (MMC) are finding very wide applications [5, 6]. In the present scenario of the research, optimization plays a vital role since it gives suitable parameters and yields optimal performance. The mathematical model is used in optimization and it plays a crucial role for the selection of machining parameters. For the development of Al MMC, many researchers [7, 8] have carried out quite a large number of experimental works, which include techniques to improve the material removal rate (MRR), to reduce the electrode wear rate (EWR), to improve the surface roughness (SR), and to reduce the thickness of the recast layer formed. On the contrary, some researchers worked in optimizing the process parameters such as current, pulse on-time, pulse off-time, intensity, and flushing pressure for an optimal output [8, 9].

Among the Al MMCs, Al-silicon carbide (SiC) composites are being widely used in industrial applications [8–11]. Few researchers have determined the mathematical models for the MRR, EWR, and SR with the volume fraction of SiC [12–14]. Teimouri and Baseri [15] worked with a SPK cold work steel. In this work, the effects of rotary magnetic field and also the ultrasonic vibration of workpiece were studied on dry EDM process performance. The results showed a positive effect on the MRR and SR. By the application of ultrasonic vibration, the maximum MRR is possible; also, they developed a mathematical model to correlate the relation between the EDM input and output parameters. Bai et al. [16] worked on a powder mixed EDM process to improve the MRR. They reported that the MRR increased initially then decreased with the powder concentration. The empirical formula for the MRR was established based on the experimental results. In this work, the AISIH13 material was used for investigation. They reported that increasing current, voltage, and duty cycle values increased the MRR, but increasing pulse on-time value initially increased the MRR until a maximum value and then started to decrease. Hosseini Kalajahi et al. [17] formulated the thermal model and finite element simulation of EDM considering several factors such as the temperature-dependent material properties, shape and size of the heated zone, energy distribution factor, plasma flushing efficiency, and phase change to predict the thermal behavior and material removal mechanism.

In these models, the common parameters such as current, pulse on-time, intensity, and duty cycle were discussed. However, the size of the SiC is believed to have its influence on the responses. In this work, the mathematical models for the MRR, EWR, SR and cylindricity (CY) were developed, which are the function of current (A), pulse on-time (Pon), flushing pressure (Pr), and particle size (Ps). The mathematical models for the MRR, EWR, SR, and CY were used to find the effect of process parameters on the performance measures. The main objective was to optimize the process parameters using the desirability approach through response surface methodology (RSM).

2 Materials and methods

In this study, the experiments were planned with four factors and three levels. The preferred levels and the factors selected for the machining parameter are shown in Table 1.

Table 1

Machining parameters and their levels.

ParametersUnitsLevel 1Level 2Level 3
Current (A)amps4.008.0012.00
Flushing pressure (Pr)kgf/cm20.250.500.75
Particle size (Ps)μm15.0025.0040.00
Pulse on-time (Pon)μs200.00400.00600.00

The Sparkonix EDM machine shown in Figure 1 is used to perform the machining operations. The flushing of the dielectric fluid was carried out by a jet flushing system in which the dielectric fluid was pumped through the nozzle with the aid of a circulation system. Kerosene was used as the dielectric fluid. The Al 6061-15% SiC composite material was taken as a workpiece. The composite samples with different particle size (i.e., 15, 25, and 40 μm) were prepared by a stir casting process. A fine-machined copper rod of ∅12 mm was used as the electrode.

Figure 1 Electrical discharge machine setup.
Figure 1

Electrical discharge machine setup.

Many factors are influencing the EDM process. In this experimental work, the factors such as peak current, pulse on-time, flushing pressure, and particle size were taken into account as the design factor. Twenty-seven experiments were conducted on Al 6061-SiC with three different particle sizes. Two trials of machining were performed for each set of parameters, and blind holes of ∅12 mm diameter and 5 mm depth were made. The machining time of each trial was measured. The tool and the workpiece were weighed before and after machining. Based on the wear weight, the MRR and EWR are calculated using Equations (1) and (2). Figures 2 and 3 show the SR tester electronic weight balance machine used in this work.

Figure 2 SR tester.
Figure 2

SR tester.

Figure 3 Electronic weight balance.
Figure 3

Electronic weight balance.

(1)MRR(g/min)=MaterialRemoved from the Work Piece Machiningtime  (1)
(2)EWR(g/min)= MaterialRemovedfromtheElectrode Machiningtime (2)

Using the above equations, the relationship between the process variables and the performance measures are established using the Design Expert 7.0.0 software. The MRR, EWR, SR, and CY are the performance measures, which are important in the aspect of increasing the productivity and improving the quality. The Mitutoyo Shimadzu electronic weight balance model BL 220H (L) of capacity 220 g and with the readability of 0.001 g was used to weigh the workpiece and electrodes. A Mitutoyo SR tester was used to measure the SR of the workpieces measured on the sides of the machined hole for three places and the average value is observed. The CY value was measured using the coordinate measuring machine (CMM) Checkmaster with the least count of 0.001 μm as shown in Figure 4. The CY is an actual volumetric assessment measured through the sides of the machined hole on three different regions. The specifications of EDM and CMM are shown in Table 2. The design matrix and measured outputs are shown in Table 3.

Figure 4 Coordinate measuring machine.
Figure 4

Coordinate measuring machine.

Table 2

Specifications of EDM and CMM.

Specifications
EDMCMM
Current: 1–15 ampsAccuracy: 4.5+L/150 μm
Pulse on-time: 100–1000 μsT-Stylus
Pulse off-time: 10–100 μs2.00 mm T-Stylus
Flushing pressure: 0.1–2 kfg/cm24.00 mm T-Stylus
Tank size: 500×300×200 mm6.00 mm T-Stylus
Table size: 300×200 mmStar stylus (each 2 mm) set
Maximum weight of workpiece: 100 kg
Maximum weight of electrode: 25 kg
Table 3

Design matrix by experiment.

RunA (amps)Pr (kgf/cm2)Ps (μm)Pon (μs)MRR (g/min)EWR (g/min)SR (μm)CY (mm)
140.25152000.03180.00261.740.003
240.25254000.03220.00282.010.004
340.25406000.03390.00292.050.006
440.5154000.03310.00271.930.008
540.5256000.03440.00311.920.009
640.5402000.03420.00321.980.012
740.75156000.03410.00331.990.013
840.75252000.03440.00312.010.014
940.75404000.03470.00352.130.017
1080.25154000.03490.00362.040.019
1180.25256000.03530.00392.050.021
1280.25402000.03510.00382.070.024
1380.5156000.03520.00412.090.021
1480.5252000.03540.00422.080.032
1580.5404000.03710.00452.110.035
1680.75152000.03640.00432.220.037
1780.75254000.03720.00492.230.038
1880.75406000.03770.00512.130.039
19120.25156000.03860.00532.120.042
20120.25252000.03880.00522.340.045
21120.25404000.03920.00542.430.049
22120.5152000.03890.00522.390.052
23120.5254000.03950.00562.360.052
24120.5406000.04020.00592.370.053
25120.75154000.04010.00562.410.056
26120.75256000.04050.00572.360.058
27120.75402000.04060.00622.450.057

3 Response surface methodology

From the set of process parameters and the output responses measured, the mathematical model for the MRR, EWR, SR, and CY was developed and analyzed using RSM. The RSM is a collection of the mathematical and statistical technique that is useful for the modeling and analysis of the problem in which a response of interest is influenced by several variables and the objective is to optimize the parameters. It is an empirical modeling approach for determining the relationship between the process parameters and performance measures with various desired criteria and searching the significance of the parameters on the performance measures. RSM is utilized to accurately describe and identify the influence of the interaction of different independent variables on the response when they are varied simultaneously [18, 19]. RSM is also an empirical technique devoted to the evolution of the relationship between the groups of controlled experimental factors and the observed results of one or more selected criteria.

The effect of process parameters of the machining process on the response variables in the MRR, EWR, and SR is summarized and the empirical relations are formulated. The Design Expert 7.0.0 software has constructed a nonlinear regression expression using the experimental data. The nonlinear estimation is a general fitting procedure that will estimate the kind of relationship between a dependent (response) variable and a list of independent variables. The regression model is expressed as

(3)Y=f(C,Pr,Ps,Pon). (3)

Here, Y is the desired response and f is the response function. In the procedure of the analysis, the approximation of Y was proposed using the fitted second-order polynomial regression model, which is called as the quadratic model. The quadratic model was studied for the interactive effects of combinative factors on the performance evaluations [11]. The quadratic model of Y can be written as follows:

(4)y =β0 +i=1kβixi+i=1kβiixi2+i<jβijxixj+ (4)

where β0 is constant and β1, β2, and βij are the coefficients of the linear, quadratic, and cross-product terms, respectively. xi is a coded variable corresponding to the machining parameters.

The optimization for the multiple response work was carried out through the desirability approach in the Design Expert 7.0.0 software, which is a mathematical method to find the optimum. The desirability of each performance measure is calculated as follows:

(5)D=(d1×d2×....dn)=(i=1ndi) (5)

The desirability converts the performance measures into a dimensionless value between 0 and 1, where 0 means the performance measures are unacceptable and 1 means it is acceptable.

If any of the parameters or performance measure falls outside their desirability range, the overall function becomes zero. For simultaneous optimization, each parameter must have a low and high value assigned to each goal. The parameters should be in the range of lower and upper limits. The performance measure will always be included in the optimization, at their design range by default, or as a maximum, minimum of target goal. The meanings of the goal parameters are as follows: If the goal is to be maximum, di=0 if response<low value, di=1 if response>high value, and 0≤di≤1 as response varies from low to high; if the goal is to be minimum, di=1 if response<low value, di=0 if response>high value, and 1≥di≥0 as response varies from low to high; if the goal is target, di=0 if response<low value, di=0 if response>high value, 0≤di≤1 as response varies from low to target, and 1≥di≥0 as response varies from target to high; the range is di=0 if response<low value, di=0 if response>high value, and di=1 as response varies from low to high, where D is the objective function, d is the desired range, n is the number of response, and i is the machining parameters.

4 Proposed mathematical models

The mathematical models for the responses viz. MRR, EWR, and SR are discussed. The models proved that the effect of particle size has a significance on the responses compared with the other responses.

4.1 Material removal rate

From the empirical model, it is clear that the peak current has a significant effect on the MRR. The MRR increases with increasing peak current, pulse on-time, flushing pressure, and particle size. When peak current increases, the pulse discharge energy channel diameter also increases. This will increase the crater diameter and depth. This makes the increase in the MRR. The increase in pulse on-time produces heating flux for a longer time and it leads to the expansion of plasma channel, which results in a higher MRR. Therefore, as the pulse on-time increases, the MRR decreases. Although the MRR increases with increasing particle size, the combined effect of particle size and flushing pressure also impacts on the MRR. The MRR decreases with increasing flushing pressure and particle size.

(6)MRR=+0.026403+8.05263E-004× A +3.95439E-003× Pr+6.83626E-005×Ps+1.19444E-006×Pon-2.28070E-006× A× Ps-1.57895E-005× Pr× PsR2=97.68 (6)

4.2 Electrode wear rate

From the EWR model, it is observed that the peak current has some notable effect on the EWR. The EWR decreases with decreasing peak current, decreasing pulse on-time, and decreasing particle size. When the peak current increases, a higher heat energy is subjected to both workpiece and electrode. This causes the increase in the volume of molten metal and ejected metal from the workpiece. This will increase the EWR. When pulse on-time is high, a higher number of positively charged particles strike the negatively charged tool. This leads to the melting of electrode material and leads to a higher EWR. The EWR increases with increasing flushing pressure. The increase in the cooling rate of the electrode by the higher flushing pressure leads to a less EWR. This is due to the reason that the cooling rate of the tool decreases with the increase in flushing pressure. This leads to an increase in the EWR. The combined effect is that the EWR increases with increasing peak current and particle size. The EWR also increases with increasing flushing pressure and particle size.

(7)EWR=+8.08772E-004+3.18056E-004×A+6.38596E-004×Pr+2.86550E-006×Ps+4.16667E-007×Pon+7.017E-007×A×Ps+2.77193E-005×Pr×PsR2=98.73 (7)

4.3 Surface roughness

The mathematical model for the SR given in Equation (8) implies that flushing pressure has a significant effect on the SR. The SR increases with increasing peak current, flushing pressure, and particle size. When peak current increases, it leads to an increase in the discharge heat energy at the point of discharge. At this point, a pool of molten metal is formed and overheated. Gas bubbles formed and explode due to the evaporation of molten metal and it was carried away by the dielectric fluid. During higher pulse on-time, a higher energy is produced. Due to the above reasons, the SR is increased. The combined effect of peak current and particle size yields to a decrease in the SR, whereas the SR decreases with increasing flushing pressure and particle size.

(8)SR=+1.33099+0.055329×A+0.61053×Pr+0.012532 ×Ps-5.55556E-005×Pon-2.67544E-004×A×Ps-0.013895×Pr×PsR2=89.22 (8)

4.4 Cylindricity

When improving the performance measures such as the MRR, EWR, and SR, there is an impact in the form tolerance such as circularity, CY, and perpendicularity. The CY is one of the important form tolerances of a cylindrical object. Therefore, it is important to measure the geometric feature such as CY, and the effect of machining parameters in the CY is vital. From the empirical model of the CY, it is clear that the peak current has significant effect on the CY. The CY increases with increasing peak current, flushing pressure, and particle size. Although the CY increases with increasing peak current and particle size, the combined effect of peak current and particle size and flushing pressure with particle size reduces the CY. The CY decreases with increasing particle size and flushing pressure.

(9)CY=-0.031626+5.35526E-003×A+0.031579×Pr+3.19298E-004×Ps-3.88889E-006×Pon-3.94737E-006×A×Ps-2.17544E-004×Pr×PsR2=98.80 (9)

From the mathematical models developed for the MRR, EWR, SR, and CY to establish the effect of parameters on the performance measures, the influences of parameters are ranked based on the coefficients of each parameter in the mathematical model. The second-order mathematical model of the above equations was tested through analysis of variance (ANOVA), and the results are tabulated in Table 4.

Table 4

ANOVA for MRR, EWR, SR, and CY.

SourceSSDFMSF-valuep-Value
MRR
 Model0.0001863E-05140.0735<0.0001
 A-Current0.00015810.000158736.7925<0.0001
 B-Flushing pressure1.38E-0511.38E-0564.68292<0.0001
 C-Particle size5.08E-0615.08E-0623.72922<0.0001
 D-Pulse on-time1.03E-0611.03E-064.7975640.0405
 AC1.58E-0711.58E-070.7385280.4003
 BC2.96E-0812.96E-080.1382690.7139
 Residual4.28E-06202.14E-07
 Cor total0.00018426
EWR
 Model3.23E-0565.38E-06258.6826<0.0001
 A-Current2.91E-0512.91E-051396.017<0.0001
 B-Flushing pressure2.19E-0612.19E-06105.4021<0.0001
 C-Particle size7.97E-0717.97E-0738.3115<0.0001
 D-Pulse on-time1.25E-0711.25E-076.0069550.0236
 AC1.5E-0811.5E-080.719430.4064
 BC9.12E-0819.12E-084.3847260.0492
 Residual4.16E-07202.08E-08
 Cor total3.27E-0526
SR
 Model0.79487660.13247927.58139<0.0001
 A-Current0.65843210.658432137.0815<0.0001
 B-Flushing pressure0.05831510.05831512.140730.0023
 C-Particle size0.03381310.0338137.039650.0153
 D-Pulse on-time0.00222210.0022220.4626530.5042
 AC0.00217610.0021760.4530350.5086
 BC0.02292610.0229264.7731170.0410
 Residual0.096064200.004803
 Cor total0.89094126
CY
 Model0.00879460.001466274.295<0.0001
 A-Current0.00787610.0078761474.047<0.0001
 B-Flushing pressure0.00073210.000732137.0434<0.0001
 C-Particle size9.13E-0519.13E-0517.080.0005
 D-Pulse on-time1.09E-0511.09E-052.0378680.1689
 AC4.74E-0714.74E-070.0886510.7690
 BC5.62E-0615.62E-061.0517680.3173
 Residual0.000107205.34E-06
 Cor total0.00890126

DF, degrees of freedom; MS, mean squares; SS, sum of squares.

The quadratic mathematical models were proposed for the performance measures viz. MRR, EWR, SR, and CY. The fit summary reveals that the quadratic model is statistically significant to analyze the performances. The values “Prob>F” in tables for the term of models are <0.05, which indicates that the obtained model is statistically significant. The other important coefficient is R2, which is the ratio of the explained variation to the total variation in the measure of degree of fit.

5 Effect of process parameters

The effect of parameters such as peak current, pulse on-time, flushing pressure, and different particle size on the output responses (i.e., MRR, EWR, SR, and CY) is discussed using graphs generated by the Design Expert 7.0.0 software for the experimental data.

5.1 Material removal rate

Figure 5 shows the interactive effect of current and particle size on the MRR. When the particle size is low, the MRR increases as the current is increased. This is also true for the larger value of particle size, but the rate of increase is less compared to that for the lower value of particle size. This can be visualized by this slope of the curve for different particle sizes. This may be because the binding area between the matrix and this requires a large energy for the removal. This may occur due to the large binding area between the matrix and reinforcement of large particle size.

Figure 5 Interactive effect of current and particle size on MRR.
Figure 5

Interactive effect of current and particle size on MRR.

From Figure 6, it is clear that the effect of flushing pressure on the MRR is the same for both lower particle size and larger particle size. It is clear that the MRR increases with the increase in flushing pressure. It is also noted that, for any flushing pressure, the effect of flushing pressure on the MRR is the same. It is observed that the MRR decreases with an increase in particle size. The larger particle size leads to a larger binding area and also a larger energy is required for the removal.

Figure 6 Interactive effect of flushing pressure and particle size on MRR.
Figure 6

Interactive effect of flushing pressure and particle size on MRR.

5.2 Electrode wear rate

Figure 7 shows the interactive effect of current and particle size on the EWR. It is observed that the EWR increases with both current and particle size. At a lower particle size, the EWR is less compared to that in a larger particle size. Thus, the larger particle size is increased as an erosion effect. When both particle size and flushing pressure become larger, the EWR increases largely as shown in Figure 8. SiC particles are removed from the workpiece, which flows in the dielectric fluid around the soft electrode and erode the electrode. This is the reason for the larger EWR in the process.

Figure 7 Interactive effect of current and particle size on EWR.
Figure 7

Interactive effect of current and particle size on EWR.

Figure 8 Interactive effect of flushing pressure and particle size on EWR.
Figure 8

Interactive effect of flushing pressure and particle size on EWR.

5.3 Surface roughness

It is obvious that the increase in the particle size and peak current leads to the increase in the SR value. This interactive effect is shown in Figure 9. From Figure 10, it is clear that the effect of flushing pressure has less significant on the SR. When the flushing pressure increases, there is slight decrease in the SR. The effect of particle size has larger impact on the SR. When the particle size increases, the SR is decreases largely.

Figure 9 Interactive effect of current and particle size on SR.
Figure 9

Interactive effect of current and particle size on SR.

Figure 10 Interactive effect of flushing pressure and particle size on SR.
Figure 10

Interactive effect of flushing pressure and particle size on SR.

5.4 Cylindricity

Figure 11 shows the interactive effect of current and particle size on the CY. It is observed that the CY increases in a larger manner for increasing current and particle size. At a lower particle size, the CY is less compared to that in larger particle size. The larger particle size required a maximum erosion effect, which leads to an increase in the CY. The larger particle size and flushing pressure increased the CY as shown in Figure 12. The larger particles are removed from the workpiece, which is carried by the dielectric flow, and it affects the machined hole. This is the reason for the larger CY in the process.

Figure 11 Interactive effect of current and particle size on CY.
Figure 11

Interactive effect of current and particle size on CY.

Figure 12 Interactive effect of flushing pressure and particle size on CY.
Figure 12

Interactive effect of flushing pressure and particle size on CY.

6 Confirmation experiment

After the selection of the optimal design parameters, the next step is to predict and verify the improvements of the quality characteristics for the machining of Al-SiC MMC by the EDM. The predicted optimum values are obtained from the Design Expert 7.0.0 software with a desirability value of 0.513.

Based on the experimental results for the maximum MRR, minimum EWR, minimum SR, and minimum CY, the Design Expert 7.0.0 software provides the predicted machining parameters for the optimum performance measures. A confirmation experiment was carried out through the predicted parameters and the performance measures are observed in Table 5.

Table 5

Predicted vs. observed values.

Current (amps)Flushing pressure (kgf/cm2)Pulse on-time (μs)Particle size (μm)MRR (g/min)EWR (g/min)SR (μm)CY (mm)
Predicted values50.25600150.03310.00301.8560.0057
Observed values50.25600150.04530.00562.3400.007

7 Conclusions

In this work, EDM was conducted on a Al-SiC MMC with different SiC particle sizes using a copper electrode of ∅12 mm. The experiment was designed using the Design Expert 7.0.0 software. Using the experimental data, the mathematical models for the MRR, EWR, SR, and CY were developed. The peak current is found to be the most significant parameters in the models for the MRR and EWR. The optimization was carried out by the desirability approach. The 3D plots were generated for analyzing the effect of particle size using the Design Expert 7.0.0 software. Based on the analysis, the following conclusions were derived.

When the particle size is high, the MRR increases with current. It is due to the larger binding area between the matrix and reinforcement particles. The MRR is less for the MMC having larger particles. The MRR is slightly decreased when both particle size and current increased. For any particle size, the effect of flushing pressure is same. That is, when the flushing pressure increases, the MRR also increases. However, the MRR is not maximum at the larger level of particle size and flushing pressure.

The EWR largely increases with the increase in current. Meanwhile, it is slightly increased when the size of the particle is increased. The EWR is largely affected with the increasing current and particle size. The EWR is significantly increased with the increase in the particle size. For higher particle size and flushing pressure values, the EWR is maximum. It is due to the low hardness of the electrode. It is noted that the EWR is minimum at a lower particle size compared to that in a larger particle size.

The effect of particle size has a larger impact on SR. When the particle size increases, the SR decreases largely.

It is observed that the CY increased in a larger manner with the increased current and particle size.


Corresponding author: Chinnaiyan Sathiya Narayanan, National Institute of Technology, Department of Production Engineering, Triuchirappalli, Tamil Nadu 620 015, India, e-mail:

References

[1] Luis CJ, Puertas I, Villa G. J. Mater. Process. Technol. 2005, 164–165, 889–896.Search in Google Scholar

[2] Puertas I, Luis CJ, Alvarez L. J. Mater. Process. Technol. 2004, 153–154, 1026–1032.Search in Google Scholar

[3] Khan AA. Int. J. Adv. Manuf. Technol. 2008, 39, 482–487.Search in Google Scholar

[4] Garg RK, Singh KK, Sachdeva A, Sharma VS, Ojha K, Singh S. Int. J. Adv. Manuf. Technol. 2010, 50, 611–624.Search in Google Scholar

[5] Singh S, Maheshwari S, Pandey PC. J. Mater. Process. Technol. 2004, 149, 272–277.Search in Google Scholar

[6] Rozenek M, Kozak J, Daîbrowski L, Eubkowski K. J. Mater. Process. Technol. 2001, 109, 367–370.Search in Google Scholar

[7] Dhar S, Purohit R, Saini N, Sharma A, Hemath Kumar G. J. Mater. Process. Technol. 2007, 194, 24–29.Search in Google Scholar

[8] Mandal D, Pal SK, Saha P. J. Mater. Process. Technol. 2007, 186, 154–162.Search in Google Scholar

[9] Beri N, Kumar A, Maheshwari S, Sharma C. Int. J. Mach. Mach. Mater. 2011, 9, 103–115.Search in Google Scholar

[10] Narender Singh P, Raghukandan K, Rathinasabapathi M, Pai BC. J. Mater. Process. Technol. 2004, 155–156, 1653–1657.Search in Google Scholar

[11] Chiang K-T. Int. J. Adv. Manuf. Technol. 2008, 37, 523–533.Search in Google Scholar

[12] Dvivedi A, Kumar P, Singh I. Int. J. Mach. Mach. Mater. 2008, 3, 293–308.Search in Google Scholar

[13] Habib SS. Appl. Math. Model. 2009, 33, 4307–4407.Search in Google Scholar

[14] Muller F, Monaghan J. Int. J. Mach. Tool. Manuf. 2000, 40, 1351–1366.Search in Google Scholar

[15] Teimouri R, Baseri H. Int. J. Adv. Manuf. Technol. 2013, 67, 1371–1384.Search in Google Scholar

[16] Bai X, Zhang Q-H, Yang T-Y, Zhang J-H. Int. J. Adv. Manuf. Technol. 2013, 68, 1757–1766.Search in Google Scholar

[17] Hosseini Kalajahi M, Rash Ahmadi S, Nadimi Bavil Oliaei S. Int. J. Adv. Manuf. Technol. 2013, 69, 687–704.Search in Google Scholar

[18] Pradhan MK, Biswas CK. Int. J. Mach. Mach. Mater. 2011, 9, 66–85.Search in Google Scholar

[19] Pandian M, Sivapirakasam SP, Udayakumar M. Appl. Energ. 2011, 88, 2663–2676.Search in Google Scholar

Received: 2013-12-19
Accepted: 2014-7-8
Published Online: 2014-9-26
Published in Print: 2016-3-1

©2016 by De Gruyter

This article is distributed under the terms of the Creative Commons Attribution Non-Commercial License, which permits unrestricted non-commercial use, distribution, and reproduction in any medium, provided the original work is properly cited.

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