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1. Introduction
Growing demand for lightweight structural materials in the aerospace and transport industries has resulted in a major interest in magnesium and its alloys. Compared with aluminium and steel, magnesium is one of the engineering materials that weighs the least, which helps with boosted fuel economy and a reduction in pollutants [1, 2]. Likewise, it exhibits a better strength-to-weight ratio, toughness, high damping capacity, and easier machinability. However, these materials have some major limitations, such as low creep, stiffness, low resistance to wear, and increased reactivity towards chemicals that frequently limit their industrial applications. It also has poor ductility, characterized by a brittle-like performance at ambient temperature owing to its HCP crystal structure and a limited slip system [3–5]. Composite development is considered one of the key ways to enhance the desired strength of Mg matrix material by the addition of selected reinforcements. The inclusion of carbide and carbon-based reinforcement such as SiC, TiC, CNT, graphene, etc. in the magnesium matrix enhances the mechanical characteristics and functional properties [6, 7]. In several industrial applications, material life is mainly dependent on surface mechanical qualities, and hence the development of surface composites has been adopted by several researchers.
Friction stir processing is a surface modification technique used to develop surface composites at a temperature below the substrate’s melting point, and there is little literature available based on Mg FSP [8]. Qiao et al. adopted FSP with different passes to develop a ZrO2-reinforced magnesium surface composite [9]. Investigation over mechanical behaviour depicts improved tensile strength (∼15.9%) while compared with base material. Likewise, increases in FSP pass decrease its grain size. An SiC-reinforced Mg surface composite was developed by Lu et al. through the FSP approach, and optimization was done for the FSP parameters to attain better mechanical properties [10]. Results revealed that FSP of three passes showcases better tensile and hardness properties. A graphene-reinforced Mg surface composite was developed by Zang et al. and its effects on mechanical properties were analyzed [11]. Observed results show that higher rotation speed and three passes increase the tensile and microhardness of the Mg matrix and also found that the addition of graphene up to 6.43 volume % showcased improved strength compared to the base material. Because composite materials are harder, tougher, and more resistant to wear and fatigue, they are more difficult to machine. Though these composites have better properties, the existence of reinforcement particles in the matrix phase harms the cutting tool life during traditional machining, which results in a deprived surface quality of machined engineering parts. Additionally, the inclusion of reinforcement reduces the tool life of traditional tungsten carbide and high-speed steel tools due to abrasion. As a result of their high hardness, composite materials are challenging to process using traditional techniques, particularly where complex geometry and dimensional accuracy are needed.
These composites are easily processed using nontraditional techniques like abrasive water jet machining. However, they can only be cut in one direction with these techniques. Consequently, WEDM has become a good method for shaping complicated materials made of composites. Herein, material removal takes place by erosion formed by sparks in-between the work samples and wire. Conversely, the formation of an immediate rise in temperature due to sparks and variation in melting point among the matrix and reinforcement will affect the surface of machined components. Another fact is that the presence of reinforcement phase in composite forms limits electrical conductivity, which results in damage due to anisotropic thermal distribution. Furthermore, wire breaking owing to the limited build-up current and variation in hardness of the composite is also a limiting factor to reducing the production rate in WEDM. Hence, there is a need for an hour to optimize the control factors to improve the quality of machined surfaces by maintaining higher material removal. It was found that only minimal studies discussed the WEDM of Mg surface composites. Kavimani et al. examined the consequences of WEDM parameters on graphene magnesium composite, and the results revealed that a surge in pulse on time increases MRR [12]. Further, observation revealed that pulse off time and pulse on time have more domination in influencing control parameters over output response. Vijayabhaskar and Rajmohan et al. developed a nano SiC-reinforced Mg composite and discussed the consequences of WEDM control factors on the developed composite [13]. Reinforcement percentage, pulse off time, voltage, pulse on time, and wire feed rate are chosen as input parameters. The results reveal that an increase in reinforcement percentage decreases the surface finish. Progress in newer soft computing techniques results in the development of different optimization approaches to attain solutions for complex objectives and uncertain situations. For predicting and attaining optimal machining parameters, researchers adopted various mathematical and statistical techniques such as Taguchi, ANN, GA, PSO, etc. [14, 15]. Additionally, a multiresponse optimization strategy was utilized to address the competing natural responses brought on by material removal rate, surface roughness, kerf taper, etc., which prevented the individually optimized settings from accomplishing their goals [16, 17]. From an industrial viewpoint, the ideal combination is necessary to ensure that the defined reactions are obtained in the best possible balance.
This fact made the researchers adopt hybrid optimization techniques, and a little literature on these techniques is discussed in detail. An analytical hierarchy process coupled genetic algorithm approach was adopted by Kumar et al. to optimize WEDM parameters. Input parameters such as wire tension, spark gap-set voltage, pulse on time, pulse peak current, pulse off time, wire feed rate, and other input parameters are selected and optimized for MRR and roughness [18]. At the optimal combination, 13.79% and 19.16% improvements have been attained while compared with discrete optimal solutions. A PCA-coupled ANN approach was adopted by Phate et al. to understand the WEDM behaviour of the developed composite. The results reveal that integrated form optimization techniques deliver an effective optimal solution. Based on available literature, it can be noted that wire feed rate, pulse off time, and pulse on time are the major influencing parameters in WEDM [19]. Machinability analysis of graphene-based surface composites has rarely been reported. Multiobjective optimization techniques deliver better results when compared with traditional techniques. Utilization of Entropy-coupled CORPUS for WEDM analysis is not yet reported. On the basis of the obtained evidence, an attempt has been made to understand the machinability characteristics of graphene-reinforced surface composite. The Entropy-coupled CORPUS methodology is adopted to understand and optimize the machining parameters to improve the quality of the machined surface and production rate in a single unique solution.
2. Materials and Methods
AZ31 Mg alloy substrate with dimensions of 150 × 100 × 8 mm is selected as the base material. Graphene and boron nitride particles are selected as reinforcements to improve the basic and functional properties of the AZ31 Mg alloy. Herein, graphene and boron nitride particles are mixed in equal proportion by the assistance of an ultrasonic assisted stirring process. Herein, the calculated amount of graphene and BN particles are ultrasonicated separately with organic solvent for 1 h, and then the samples are further sonicated for 3 h. After that, the samples are stirred using a magnetic stir coupled with a hot plate for 3 h at 1000 rpm. Then the attained mixtures are vacuum dried for 24 h and the resultant samples are used as reinforcement. The profile of the FSP tool used and the step-by-step procedure for FSP are illustrated in Figures 1(a) and 1(b). As a first step in FSP, a groove has been made at the center of the Mg plate parallel to its longest side, as shown in Figure 1(b) using the WEDM process. The groove depth is fixed at 5 mm and its width is varied based on volume % of reinforcement (1, 3, and 5). A double-tempered H13 steel tool with a 5 mm pin length (L), a 20 mm diameter shoulder (D), and a 6 mm diameter pin (d) was utilized for FSP. Friction stir processing was conducted in a modified vertical milling machine with an optimized rotation speed and traverse feed of 1200 rpm and 20 mm/min (Figure 1(c)). Initially, the reinforcement mixture is filled in the groove gap and the pin-less tool is allowed to pass for compacting, followed by the passing of the pin-headed tool [20]. The developed surface composite is shown in Figure 1(d).
[figure(s) omitted; refer to PDF]
3. Experimental Design
The Taguchi approach was adopted for the experimental plan with three levels and four factors with the L27 orthogonal array. Based on available literature, pulse off time, pulse on time, and wire feed rate are found to be the most important control factors in WEDM and hence they are chosen as input parameters (Table 1). Similarly, the production rate of a material and the surface quality of mechanical components are mainly based on MRR, surface roughness, and kerf width, respectively, and so these parameters are chosen as output responses (Table 2). Herein, procedures for MRR, surface roughness, and kerf width measurement are already shown in our previous reports [20, 21]. While larger is better condition, it is designated for MRR and smaller is better condition, it is designated for kerf width (KW) and surface roughness during SN ratio analysis, since higher surface roughness (Ra) decreases the surface quality.
Table 1
Machining parameters and respective levels.
Parameters | Notation | Unit | Level 1 | Level 2 | Level 3 |
Reinforcement % | A | Wt. % | 1 | 3 | 5 |
Pulse off time | B | Μs | 4 | 8 | 12 |
Pulse on time | C | Μs | 10 | 15 | 20 |
Wire feed rate | D | m/min | 4 | 6 | 8 |
Table 2
Experimental trails along with output response.
Reinforcement (%) | Pulse off time (μs) | Pulse on time (μs) | Wire feed rate (m/min) | MRR (mm3/min) | Ra (μm) | KW (μm) |
1 | 4 | 10 | 4 | 12.0765 | 3.6730 | 0.2877 |
1 | 4 | 15 | 6 | 14.8180 | 3.7540 | 0.2905 |
1 | 4 | 20 | 8 | 16.2010 | 3.8610 | 0.2967 |
1 | 8 | 10 | 6 | 12.3505 | 3.6830 | 0.2972 |
1 | 8 | 15 | 8 | 14.6605 | 3.7270 | 0.3027 |
1 | 8 | 20 | 4 | 13.4580 | 3.7630 | 0.3010 |
1 | 12 | 10 | 8 | 11.8400 | 3.6540 | 0.3049 |
1 | 12 | 15 | 4 | 11.5170 | 3.6980 | 0.3053 |
1 | 12 | 20 | 6 | 13.3415 | 3.7670 | 0.3093 |
3 | 4 | 10 | 4 | 10.0170 | 3.7280 | 0.2870 |
3 | 4 | 15 | 6 | 13.7505 | 3.8130 | 0.2948 |
3 | 4 | 20 | 8 | 14.8505 | 3.8960 | 0.2963 |
3 | 8 | 10 | 6 | 10.9015 | 3.6820 | 0.2967 |
3 | 8 | 15 | 8 | 12.8680 | 3.7680 | 0.3014 |
3 | 8 | 20 | 4 | 12.2725 | 3.7750 | 0.3004 |
3 | 12 | 10 | 8 | 11.3505 | 3.7280 | 0.3023 |
3 | 12 | 15 | 4 | 11.1015 | 3.7220 | 0.3032 |
3 | 12 | 20 | 6 | 13.1340 | 3.7960 | 0.3079 |
5 | 4 | 10 | 4 | 9.2265 | 3.7260 | 0.2873 |
5 | 4 | 15 | 6 | 12.6765 | 3.8290 | 0.2897 |
5 | 4 | 20 | 8 | 13.9850 | 3.8820 | 0.2916 |
5 | 8 | 10 | 6 | 9.9400 | 3.7430 | 0.2930 |
5 | 8 | 15 | 8 | 13.2080 | 3.8110 | 0.2947 |
5 | 8 | 20 | 4 | 11.3830 | 3.8230 | 0.2969 |
5 | 12 | 10 | 8 | 10.0180 | 3.7480 | 0.2972 |
5 | 12 | 15 | 4 | 9.6890 | 3.7590 | 0.3002 |
5 | 12 | 20 | 6 | 10.9415 | 3.8250 | 0.3010 |
4. Results and Discussion
To determine the correlation among the set of variable pairings, a scatter-plot matrix is utilized (Figure 2). It is possible to arrange these pairwise correlations into a matrix. In general, the diagonal arrangement of the current matrix pair shows a stronger correlation between the matrix pairs and a lack of outliers in the obtained output data. Further relations between the various control factors and their respective output responses can also be understood with the help of a matrix plot. It can also be used to observe the clustering of data by control factors in the dataset for a specific response variable. Herein, the correlation set of variables can be identified based on the mirror images. For example, the eighth row fifth column and the ninth row sixth column of the scatter plot resemble the mirror image of the fifth row eighth column and the sixth row ninth column of the scatter plot, which denotes the correlation among data sets. Likewise, the influence of each control factor over other output responses can also be examined using a scatter plot. For example, the fifth column in the first row implies the relation between surface roughness and reinforcement percentage. In this, the x-axis denotes the surface roughness, and the y-axis denotes the reinforcement percentage. The movement of variables from left to right indicates that surface roughness increases with respect to reinforcement increment.
[figure(s) omitted; refer to PDF]
An algorithmic analysis known as a “hierarchical cluster” groups the related data into clusters. Each cluster, in this case, differs from the others, and the values are very close to one another. Figure 3 shows that the output parameter values are clustered into four groups using the expressive colours of blue and brown (dark and lighter). According to the input parameter, these are ranked from −1 to 1. The output parameter values are presented in lighter and darker shades of blue and brown in a top-to-bottom arrangement.
[figure(s) omitted; refer to PDF]
4.1. Effect of Control Factors on Surface Roughness
In Figure 4 depicts the influence of control factors on surface quality. It can be noted that increases in reinforcement decrease the surface roughness as the presence of reinforcement particles promotes the hardness values of the developed composite that results in breakage of wires during the WEDM process, thus decreasing the surface finish. The thermal mismatch between the matrix and reinforcement also plays a vital role in surface roughness. During pulse on time, the creation of sparks results in the melting of base material due to its low melting point. Compared with reinforcement (Graphene: BN), further gets flushed out by the dielectric medium at pulse off time. These reinforcement particles do not melt and stick to the matrix, increasing its surface roughness [12].
[figure(s) omitted; refer to PDF]
Another reason is the presence of BN, which is a well-known wide band gap semiconductor that decreases the chance for the production of sparks and results in improper cuts during machining. It can also be shown that increases in pulse off time increase the surface quality of developed samples. This upsurge in pulse off time results in the absence of spark generation and splashing of dielectric fluid. This fact removes the burs and debris formed over the machined surface. Thus, surface quality increases. Likewise, an increase in the pulse on time upsurges surface roughness that might be owing to the effect of spark generation that creates harder heat affected zones near the machined surface, thus increasing the surface roughness [22]. A rise in wire feed rate decreases the surface quality since the surge in wire feed rate results in newer wire recovery at a faster phase during the machining process. This fact increases the quality and efficiency of generated sparks that form deeper craters over the machined surface, thus reducing the surface finish. Among the available control factors, pulse on time acts as the key parameter in governing the surface quality of the developed composite, followed by reinforcement percentage in second position (Table 3). Wire feed rate has low significance on surface finish [23].
Table 3
Response table for surface roughness.
Level | Reinforcement % | Pulse off time | Pulse on time | Wire feed rate |
1 | −11.44 | −11.58 | −11.38 | −11.46 |
2 | −11.52 | −11.49 | −11.51 | −11.52 |
3 | −11.58 | −11.47 | −11.64 | −11.56 |
Delta | 0.15 | 0.12 | 0.26 | 0.1 |
Rank | 2 | 3 | 1 | 4 |
Further, the contribution percentage of individual parameters and their significance can be confirmed by the ANOVA results shown in Table 4. In general,
Table 4
ANOVA table for surface roughness.
Source | DF | Seq. SS | Adj. SS | MS | F | Contribution (%) | |
Reinforcement vol.% | 2 | 0.017996 | 0.017996 | 0.008998 | 33.1 | 0 | 17.32 |
Pulse off time | 2 | 0.013792 | 0.013792 | 0.006896 | 25.37 | 0 | 13.28 |
Pulse on time | 2 | 0.057949 | 0.057949 | 0.028974 | 106.59 | 0 | 55.78 |
Wire feed rate | 2 | 0.009264 | 0.009264 | 0.004632 | 17.04 | 0 | 8.92 |
Error | 18 | 0.004893 | 0.004893 | 0.000272 | |||
Total | 26 | 0.103893 | |||||
R-square–93.20% |
It can be observed from Table 4 that all the
[figure(s) omitted; refer to PDF]
The optimal parameters can be attained from the response table. It states that lower values of wire feed rate, pulse on time, and reinforcement volume % with a higher value of pulse off time are optimal solutions for higher surface quality.
4.2. Influence of Control Factors on Kerf Width
Figure 6 infers the impact of control factors on kerf width in the WEDM slot on the developed composite. It can be observed that increases in reinforcement percentage decrease the kerf width of the samples. The addition of reinforcement improves the hardness, which decreases the chances of widening of the sample during the machining process. Further, graphene and BN have better thermal stability that decreases the intensity and heat dissipation over the composite at spark generation, thus decreasing the kerf width. Increment in pulse on time increases the kerf width as more pulse on time maximises the discharge current or energy over the electrode that results in more dielectric supply which causes material evaporation. Likewise, higher pulse on time improves the transfer dissipation inside near the workpiece and dielectric fluid, thus increasing the kerf width. This fact initiates confined heat over the material that erodes a large portion of the material and causes widening of the kerf and profounder craters. During machining, an increase in pulse off time increases flushing time that results in debris and burs over the machined surface that results in a higher kerf width. Lower pulse off time causes inadequate flushing time, which results in the creation of a recast layer over the surface of the machined component that decreases the kerf width. Herein, lower kerf width can be obtained during minimal energy discharge that improvises exactness in dimension [13]. Likewise, an increase in wire feed rate increases kerf width; this might be due to an increase in the intensity of generated sparks. Another reason is increment in wire feed rate increases wire tension and vibration of the wire that causes irregular cuttings on the machined surface [24].
[figure(s) omitted; refer to PDF]
The response table revealed that pulse off time acts as more dominating parameter in governing kerf width (Table 5), followed by pulse on time. Herein, wire feed rate depicts lower influence over kerf width. From the response table, it can be noted that an increasing percentage of reinforcement and minimal values of control factors is the optimal parameter combination. 10 μs of pulse on time with a pulse off time of 4 μs and a 4 m/mm of wire feed rate is the optimal solution for obtaining a lower kerf width. From Table 6, it can be inferred that
Table 5
Response table for kerf width.
Levels | Reinforcement % | Pulse off time | Pulse on time | Wire feed rate |
1 | 10.47 | 10.71 | 10.61 | 10.56 |
2 | 10.49 | 10.51 | 10.52 | 10.52 |
3 | 10.62 | 10.36 | 10.46 | 10.5 |
Delta | 0.14 | 0.36 | 0.16 | 0.06 |
Rank | 3 | 1 | 2 | 4 |
Table 6
ANOVA table for kerf width.
Source | DF | Seq. SS | Adj. SS | MS | F | Contribution (%) | |
Reinforcement | 2 | 0.0001264 | 0.0001264 | 6.32E−05 | 24.81 | 0 | 12.72 |
Pulse off time | 2 | 0.0006728 | 0.0006728 | 0.000336 | 132.06 | 0 | 67.69 |
Pulse on time | 2 | 0.000129 | 0.000129 | 6.45E−05 | 25.32 | 0 | 12.98 |
Wire feed rate | 2 | 0.0000198 | 0.0000198 | 9.9E−06 | 3.9 | 0.039 | 1.99 |
Error | 18 | 0.0000459 | 0.0000459 | 0.0000025 | |||
Total | 26 | 0.0009939 | |||||
R2 = 95.39% |
[figure(s) omitted; refer to PDF]
4.3. Effect of Control Factors on MRR
Figure 8 shows the consequence of control factors on the rate of material removal. It can be observed from the figure that an increase in volume % of reinforcement decreases MRR values. This might be due to the presence of graphene and BN particles that decrease the intensity of spark generation, so the machining rate decreases. Further, these particles have varying electrical conductivity when compared with the base matrix material, which thus decreases the generation of sparks. The hybrid reinforcement has higher thermal stability. This fact decreases the chances of melting of composite material, which increases the machining time. Similarly, an increment in pulse off time decreases MRR values. During pulse off time, the machining process will be in idle condition and no spark generation will happen, which decreases the production rate. An increase in pulse on time increases the MRR value since an increase in the pulse on time promotes the spark cohort time that increases the MRR. It could be shown that increases in wire feed rate increase MRR [12, 23]. During machining conditions, increases in the wire feed rate increase the chance of changeover on new wires that increase the intensity of the spark generated near the work piece, which results in higher MRR. The response table shows that pulse on time is the key dominant parameter for governing the MRR, and pulse off time attains the last position in influencing the MRR. From the response table, the optimal solution for MRR can be attained. Herein, higher values of pulse on time and wire feed followed by lower addition of reinforcement and pulse off time is the optimal condition for a better production rate (Table 7).
[figure(s) omitted; refer to PDF]
Table 7
Response table for MRR.
Levels | Reinforcement (%) | Pulse off time | Pulse on time | Wire feed rate |
1 | 22.46 | 22.19 | 20.67 | 20.92 |
2 | 21.7 | 21.77 | 22 | 21.83 |
3 | 20.92 | 21.12 | 22.41 | 22.34 |
Delta | 1.54 | 1.07 | 1.73 | 1.42 |
Rank | 2 | 4 | 1 | 3 |
The significance of machining parameters and their respective contributions are inferred from ANOVA (Table 8). Based on ANOVA results,
Table 8
ANOVA for MRR.
Source | DF | Seq. SS | Adj. SS | MS | F | Contribution (%) | |
Reinforcement % | 2 | 20.483 | 20.483 | 10.242 | 62.41 | 0 | 24.65 |
Pulse off time | 2 | 11.998 | 11.998 | 5.999 | 36.56 | 0 | 14.44 |
Pulse on time | 2 | 28.876 | 28.876 | 14.438 | 87.98 | 0 | 34.75 |
Wire feed rate | 2 | 18.778 | 18.778 | 9.389 | 57.22 | 0 | 22.60 |
Error | 18 | 2.954 | 2.954 | 0.164 | |||
Total | 26 | 83.089 | |||||
R 2 = 96.45% |
[figure(s) omitted; refer to PDF]
4.4. Multiresponse Optimization of Control Factors
Mutual optimal parameter combinations for two or more output parameters can be obtained with the assistance of multiobjective optimization. The determination of an accurate weight for the output response is the foremost difficulty in multiresponse optimization. Researchers determined the weightage for the response based on their familiarity with and trial and error method related to the control factors’ significance [25]. Hence, there is a need to develop a new approach for computing the weightage for the output response. In this proposed research, the entropy method was adopted for allotting individual weightage on output response, which was earlier used for several multicriteria decision making problems. Most of the time, the decision maker expresses their ideas by taking into account choice variables in order to determine the weights for their traits and to parallelize comparisons with actual-world circumstances. Since entropy weight is a quantity that represents a criterion’s relevance in terms of the relative weights of criteria, the entropy method does not require such a choice. When more factors are taken into account, the entropy idea might be used to reduce the human errors involved in assigning weights. The steps involved in the entropy approach are illustrated as follows [26]:
Step 1: normalization of decision matrix EI:
Herein, (4) is used for maximization function, and (5) is used for normalizing the minimization function (refer to Table 9)
Step 2: calculation of entropy index:
Entropy index of the normalized values can be obtained from equation (6). The calculated values are illustrated in Table 10.
Step 3: determination of weightage:
Table 9
Entropy modelling for output variables.
Maximize function | Minimization function | Normalization | Entropy index (EI) | |||||
MRR | Ra | KW | MRR | Ra | KW | EIMRR | EIRa | EiKW |
12.0765 | 3.673 | 0.2877 | 0.0364 | 0.0027 | 0.0383 | −0.1206 | −0.0159 | −0.1250 |
14.818 | 3.754 | 0.2905 | 0.0447 | 0.0026 | 0.0379 | −0.1389 | −0.0156 | −0.1241 |
16.201 | 3.861 | 0.2967 | 0.0489 | 0.0025 | 0.0371 | −0.1475 | −0.0152 | −0.1223 |
12.3505 | 3.683 | 0.2972 | 0.0372 | 0.0027 | 0.0371 | −0.1226 | −0.0158 | −0.1222 |
14.6605 | 3.727 | 0.3027 | 0.0442 | 0.0026 | 0.0364 | −0.1379 | −0.0157 | −0.1206 |
13.458 | 3.763 | 0.3010 | 0.0406 | 0.0026 | 0.0366 | −0.1301 | −0.0155 | −0.1211 |
11.84 | 3.654 | 0.3049 | 0.0357 | 0.0027 | 0.0361 | −0.1190 | −0.0159 | −0.1200 |
11.517 | 3.698 | 0.3053 | 0.0347 | 0.0027 | 0.0361 | −0.1167 | −0.0158 | −0.1199 |
13.3415 | 3.767 | 0.3093 | 0.0402 | 0.0026 | 0.0356 | −0.1293 | −0.0155 | −0.1188 |
10.017 | 3.728 | 0.2870 | 0.0302 | 0.0026 | 0.0384 | −0.1057 | −0.0157 | −0.1252 |
13.7505 | 3.813 | 0.2948 | 0.0415 | 0.0026 | 0.0374 | −0.1320 | −0.0154 | −0.1229 |
14.8505 | 3.896 | 0.2963 | 0.0448 | 0.0025 | 0.0372 | −0.1391 | −0.0151 | −0.1224 |
10.9015 | 3.682 | 0.2967 | 0.0329 | 0.0027 | 0.0371 | −0.1123 | −0.0158 | −0.1223 |
12.868 | 3.768 | 0.3014 | 0.0388 | 0.0026 | 0.0366 | −0.1261 | −0.0155 | −0.1210 |
12.2725 | 3.775 | 0.3004 | 0.0370 | 0.0026 | 0.0367 | −0.1220 | −0.0155 | −0.1213 |
11.3505 | 3.728 | 0.3023 | 0.0342 | 0.0026 | 0.0365 | −0.1155 | −0.0157 | −0.1207 |
11.1015 | 3.722 | 0.3032 | 0.0335 | 0.0026 | 0.0363 | −0.1137 | −0.0157 | −0.1205 |
13.134 | 3.796 | 0.3079 | 0.0396 | 0.0026 | 0.0358 | −0.1279 | −0.0154 | −0.1192 |
9.2265 | 3.726 | 0.2873 | 0.0278 | 0.0026 | 0.0384 | −0.0997 | −0.0157 | −0.1251 |
12.6765 | 3.829 | 0.2897 | 0.0382 | 0.0026 | 0.0380 | −0.1248 | −0.0153 | −0.1244 |
13.985 | 3.882 | 0.2916 | 0.0422 | 0.0025 | 0.0378 | −0.1335 | −0.0152 | −0.1238 |
9.94 | 3.743 | 0.293 | 0.0300 | 0.0026 | 0.0376 | −0.1051 | −0.0156 | −0.1234 |
13.208 | 3.811 | 0.2947 | 0.0398 | 0.0026 | 0.0374 | −0.1284 | −0.0154 | −0.1229 |
11.383 | 3.823 | 0.2969 | 0.0343 | 0.0026 | 0.0371 | −0.1158 | −0.0153 | −0.1223 |
10.018 | 3.748 | 0.2972 | 0.0302 | 0.0026 | 0.0371 | −0.1057 | −0.0156 | −0.1222 |
9.689 | 3.759 | 0.3002 | 0.0292 | 0.0026 | 0.0367 | −0.1032 | −0.0156 | −0.1213 |
10.9415 | 3.825 | 0.301 | 0.0330 | 0.0026 | 0.0366 | −0.1126 | −0.0153 | −0.1211 |
Table 10
Calculated weighted entropy values.
Degree of divergence | Entropy weights | ||||
MRR | Ra | Kw | MRR | Ra | Kw |
0.0031 | 0.8726 | 0.0001 | 0.00352832 | 0.99639944 | 0.00007224 |
The values attained for individual parameters from (7) can be used as weightage for the hybrid optimization approaches as shown in Table 10. In this research, entropy-coupled Complex Proportional Assessment (COPRAS) was adopted to attain an optimal solution for better MRR with better surface quality.
4.5. Multiobjective Optimization by the Entropy-Coupled Complex Proportional Assessment Approach
The COPRAS approach involves proportional and direct confidence in the significance and effectiveness of substitutions available in the existence of equally conflicting parameters [27]. COPRAS incorporates the success of alternatives in relation to several control factors and connects the weights by ranking and suggesting the optimal parameters. The following steps are involved in the COPRAS approach as follows [28]:
Step 1: The initial step involves formation of decision matrix followed by normalization of output parameter.
Step 2: This involves multiplication of calculated individual weight to create a normalized decision matrix. Herein, weightage calculated from the entropy approach will be multiplied with a normalized matrix (equation (9)) to form a weighted matrix as shown in Table 9.
Step 3: calculation of Pi
In this, Pi is maximization function calculated by
Here, n is number of maximizing response.
Step 4: calculation of Ri.
In this Ri, denote the minimization function calculated by
The calculated values are summarized, and the calculated values are illustrated in Table 11.
Step 5: Observing the diminutive value of R.
Step 6: Determination of weight for attained individual response Qi
The Qi values are calculated by using equation (13), and the maximum value in Qi is termed as Qmax.
Step 7: Determination of the utility degree Ni %.
Table 11
Computed attributes values.
Weighted normalized matrix | Pi | Ri | ||
MRR | Ra | KW | MRR | Ri |
0.00012851 | 0.03600936 | 0.00000259 | 0.00012851 | 0.03601194 |
0.00015768 | 0.03680347 | 0.00000261 | 0.00015768 | 0.03680608 |
0.00017240 | 0.03785247 | 0.00000267 | 0.00017240 | 0.03785514 |
0.00013142 | 0.03610740 | 0.00000267 | 0.00013142 | 0.03611007 |
0.00015600 | 0.03653876 | 0.00000272 | 0.00015600 | 0.03654148 |
0.00014321 | 0.03689170 | 0.00000271 | 0.00014321 | 0.03689441 |
0.00012599 | 0.03582309 | 0.00000274 | 0.00012599 | 0.03582583 |
0.00012255 | 0.03625445 | 0.00000274 | 0.00012255 | 0.03625720 |
0.00014197 | 0.03693092 | 0.00000278 | 0.00014197 | 0.03693370 |
0.00010659 | 0.03654857 | 0.00000258 | 0.00010659 | 0.03655115 |
0.00014632 | 0.03738189 | 0.00000265 | 0.00014632 | 0.03738454 |
0.00015802 | 0.03819561 | 0.00000266 | 0.00015802 | 0.03819827 |
0.00011600 | 0.03609759 | 0.00000267 | 0.00011600 | 0.03610026 |
0.00013693 | 0.03694072 | 0.00000271 | 0.00013693 | 0.03694343 |
0.00013059 | 0.03700935 | 0.00000270 | 0.00013059 | 0.03701205 |
0.00012078 | 0.03654857 | 0.00000272 | 0.00012078 | 0.03655128 |
0.00011813 | 0.03648974 | 0.00000273 | 0.00011813 | 0.03649247 |
0.00013976 | 0.03721523 | 0.00000277 | 0.00013976 | 0.03721799 |
0.00009818 | 0.03652896 | 0.00000258 | 0.00009818 | 0.03653154 |
0.00013489 | 0.03753875 | 0.00000260 | 0.00013489 | 0.03754136 |
0.00014882 | 0.03805835 | 0.00000262 | 0.00014882 | 0.03806097 |
0.00010577 | 0.03669562 | 0.00000263 | 0.00010577 | 0.03669826 |
0.00014055 | 0.03736228 | 0.00000265 | 0.00014055 | 0.03736493 |
0.00012113 | 0.03747993 | 0.00000267 | 0.00012113 | 0.03748260 |
0.00010660 | 0.03674464 | 0.00000267 | 0.00010660 | 0.03674731 |
0.00010310 | 0.03685249 | 0.00000270 | 0.00010310 | 0.03685518 |
0.00011643 | 0.03749954 | 0.00000271 | 0.00011643 | 0.03750224 |
Based on the utility degree, the maximum value is ranked as the optimal parameter and the calculated values are shown in Table 12.
Table 12
Optimal criteria and ranking.
Rimin/Ri | Qi | Ni (%) | Ranking |
0.994832 | 0.001497 | 92.92797 | 23 |
0.973367 | 0.001557 | 96.61189 | 7 |
0.946393 | 0.001611 | 100 | 1 |
0.992128 | 0.001504 | 93.3404 | 19 |
0.980415 | 0.001545 | 95.8837 | 12 |
0.971037 | 0.001546 | 95.92208 | 11 |
1 | 0.001488 | 92.33272 | 26 |
0.988102 | 0.001501 | 93.13701 | 21 |
0.970004 | 0.001546 | 95.93782 | 10 |
0.980156 | 0.001496 | 92.8398 | 24 |
0.958306 | 0.001567 | 97.27148 | 4 |
0.937891 | 0.00161 | 99.91754 | 2 |
0.992398 | 0.001488 | 92.3603 | 25 |
0.969748 | 0.001541 | 95.64807 | 14 |
0.96795 | 0.001537 | 95.41665 | 15 |
0.980152 | 0.00151 | 93.7208 | 16 |
0.981732 | 0.001505 | 93.41761 | 17 |
0.962594 | 0.001554 | 96.47144 | 8 |
0.980682 | 0.001487 | 92.27149 | 27 |
0.954303 | 0.001562 | 96.93211 | 5 |
0.941275 | 0.001595 | 99.02206 | 3 |
0.976227 | 0.001501 | 93.13598 | 22 |
0.958809 | 0.001561 | 96.86694 | 6 |
0.955799 | 0.001546 | 95.93924 | 9 |
0.974924 | 0.001503 | 93.30322 | 20 |
0.97207 | 0.001504 | 93.3404 | 18 |
0.955298 | 0.001542 | 95.694 | 13 |
Based on the entropy-coupled corpus method, optimal control factors to attain better MRR along with minimal Ra and kerf width are attained. Herein, lower pulse off time and volume percentage of reinforcement with higher values of wire feed rate and pulse on time are the optimal machining parameters for attaining a good quality machined surface and production rate for the developed composite. The optimal parameter attained based on the hybrid approach (highlighted in bold font) yields the outcome values of 16.20 mm3/min of MRR with 0.29 μm of kerf width and minimal surface roughness of 3.86 μm.
5. Conclusion
A magnesium surface composite with varying volume percentages of hybrid reinforcement was developed by the friction stir processing route. The WEDM process was used to understand the machinability of magnesium surface composites. The Taguchi approach was utilized for planning the experiment. The obtained results are as follows:
(i) Pulse on time and reinforcement volume percentage act as the dominating factors to influence MRR, kerf width, and surface roughness.
(ii) Lower values of pulse on time and reinforcement volume %; higher values of wire feed rate and pulse off time are the optimal machining control factors for attaining better surface integrity
(iii) Wire feed rate has the least significance over output responses.
(iv) Entropy-coupled COPRAS was adopted to attain an optimal solution, viz. a wire feed rate of 8 m/min, 1 volume % of reinforcement, 20 μs of pulse on time, and 4 μs of pulse off time.
(v) mathematical model has been developed based on the correlation between the output and input parameters with better predictability.
(vi) In the future, artificial neural networks can be used to develop models for composite machining and to predict the output response without wasting the work sample with various experimental trials.
(viii) The developed composite can be used in potential industrial applications where lightweight structures with high hardness and wear-resisting surfaces are needed.
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Abstract
In this research, friction stir processing (FSP) is utilized to develop the graphene-boron nitride-reinforced hybrid magnesium surface composite with varying volume percentages of reinforcements. A Taguchi-coupled Entropy-COPRAS approach is adopted to understand the influence of control factors of wire electrical discharge machining on the developed magnesium surface composite. An optimal combination of machining factors to attain maximum material removal rate (MRR) along with minimal kerf width and surface roughness is to be finalized. The Taguchi method is utilized for planning the experiments with three levels and four factors, namely, reinforcement volume %, pulse off time, wire feed rate, and pulse on time. ANOVA results show that pulse on time and reinforcement volume % act as the most significant factors for output responses. Using the Entropy-COPRAS approach, an optimal combination for output response was found for a maximum MRR of 16.20 mm3/min; minimal surface roughness of 3.86 μm; and 0.29 μm of kerf width.
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1 Centre for Material Science, Department of Mechanical Engineering, Karpagam Academy of Higher Education, Coimbatore 641021, India
2 Department of Mechanical Engineering, Audisankara College of Engineering and Technology (Autonomous), Gudur, India
3 Department of Production Engineering, National Institute of Technology, Tiruchirappalli 620015, India