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PERFORMANCE STUDY OF TOOL

MATERIALS AND OPTIMIZATION OF

PROCESS PARAMETERS DURING EDM

ON ZrB

2

-SiC COMPOSITE THROUGH

PARTICLE SWARM OPTIMIZATION

ALGORITHM

S.SIVASANKAR

Research Scholar,

Department of Production Engineering, National Institute of Technology,

Thiruchirappalli-620015, Tamilnadu, India

E-mail:[email protected]

R.JEYAPAUL

Associate Professor,

Department of Production Engineering, National Institute of Technology,

Thiruchirappalli-620015, Tamilnadu, India E-mail:[email protected] Abstract:

This paper deals with optimization of EDM of ZrB2-SiC composite using Particle swarm optimization (PSO). In this work ZrB2 with different volume proportions of SiC (15, 20, 25 and 30%) are selected as workpiece. ZrB2– SiC ultra high temperature ceramics exhibited an excellent thermal-oxidative and configurationally stable under supersonic conditions, which suggests they are potential candidates for leading edges. Results indicate that ZrB2–SiC can maintain the high oxidation resistance coupled with configurationally stable at temperatures lower than that point which results in significant softening and degradation of the oxide scale, and that point will be the temperature limit for UHTC.It is a candidate for high temperature aerospace applications such as hypersonic flight or rocket propulsion systems. To expand its area of applications, machining is mandatory. Due to high strength and hardness of ZrB2 mechanical machining is very difficult or even impossible. Electrical discharge machining is promising technology to machine ceramic components of complex shape with high-dimensional accuracy and good surface roughness. In this investigation the influence of SiC over the machinability is carried out. Input parameters are pulse on time, pulse off time and tool materials (graphite, titanium niobium, tantalum and tungsten). Pulse on time and pulse off time are kept at three different levels. Objective is to maximize the material removal rate (MRR) and to minimize the roundness, surface roughness (SR), tool wear rate (TWR), Overcut and taper angle during EDM of hot pressed ZrB2-SiC composite. In general Desirability Functional Analysis (DFA) is used to combine multiple quality characteristics into a single performance statistics. While combining the quality characteristics, weight should be assigned to each response. For this problem, unequal weights are assigned using particle swarm optimization (PSO). Interaction of pulse on time with tool material is investigated using analysis of variance (ANOVA) and it shows that tool material is most significant factor. Keywords: roughness,roundness,taper angle,overcut,ZrB2,SiC,PSO,DFA,Ceramics,Composite.

1. Introduction

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Luigi Scatteia, 2008). The high electrical conductivity of ZrB2 (108 S/m) is sufficient for electrical discharge machining (EDM) allowing for relatively low cost machining of complex components (Cutler R. A, 1992). Since the ceramic materials possess exceptional mechanical and chemical properties such as high compression strength, high hardness, low ductility, high corrosion resistance, low specific weight, and a high strength even at very high temperatures (Klocke F, 1997) they have a wide range of applications. The typical processes of engineering ceramic components are compacting techniques of powder metallurgy and high-temperature sintering. However, ZrB2 is not only hard to sinter [1,2], but also by itself does not meet all the exigent requirements of oxidation resistance and mechanical properties demanded by extreme-environment aerospace engineering [1,2]. For these reasons, ZrB2 is typically combined with other refractory ceramics. One of the most widely used is SiC at relative concentrations between 5 and 30 vol.% [1,2]. Chamberlain et al. (2004) reported the flexural strength increased from 550 MPa for pure ZrB2 to 1100 MPa for ZrB2–30 vol% SiCp. Likewise, fracture toughness ranged from 3.5 to 5.3 MPa m1/2 over the same composition range. Meanwhile, Hwang et al (2007) studied the properties of ZrB2–SiC composites as a function of SiC grain size. Results showed that a reduction in the SiC grain size can improve the processing and oxidation resistance of ZrB2–SiC composites.Monteverde and Bellosi [11,12] also found that ultra-fine SiC particulates could improve the sinterability and mechanical properties of ZrB2 and a mixture of ZrB2 and HfB2.Monteverde F et al (2006) documented that ZrB2 and HfB2 can be strengthened and toughened through the incorporation of SiC particles. Therefore, ZrB2 based and HfB2 based composites reinforced by SiC particles have been investigated by many researchers. Producing complex shapes such as holes, internal cavity in ceramics with high dimensional accuracy is very difficult to achieve through these conventional machining techniques and they are expensive to produce. The use of traditional cutting machinery to machine hard and brittle ceramic materials can cause cracks on the machined surface (Allor RL and Jahanmir S, 1996). Electric discharge machining (EDM) is the best choice for the manufacture of conductive ceramic materials because there is no contact between the tool and workpiece during the EDM process. In the EDM process, the surface layer of a workpiece can be rapidly melted and removed by an arc of 8,000 –12,000°C at each charge point. EDM takes advantage of spark-erosion manufacturing to machine the hard to cut material which efficiently produces the required shapes and sizes, finer surface characteristics, and better dimensional accuracy. Over the past few years, EDM has been widely applied in the modern metal industry for producing intricate and complex shapes required for conductive ceramic materials that are difficult to manufacture by conventional machining (Mc Geough JA, 1988).

Selection of tool material for machining the ceramic is the major area to be analyzed since electrode wear occurs during EDM process leading to a lack of machining accuracy in the geometry of workpiece. To reduce the influence of the electrode wear, it is necessary either to feed electrode larger than the workpiece thickness in the case of making through-holes, or to prepare several electrodes for roughing and finishing in the present state of technology. Very few literatures are available on tool material performance evaluation. Yao-Yang Tsai stated that volumetric wear ratio of the electrode becomes small for the electrode material with high boiling point, high melting point, and high thermal conductivity. This tendency is independent of the workpiece materials. An index is proposed to include the boiling phenomenon for evaluating the erosion property of electrode material in EDM (Yao-Yang Tsai, and Takahisa Masuzawa, 2004) The effects of electrode tool materials and machining input parameters on AISI D3 EDM characteristic, by the use of variance analysis and experiments designing techniques is studied and reported that the graphite electrode, having highest material removal rate and precise dimension and low tool wear ratio, is the most appropriate material for steel machining (Khoshkish, Ashtiani, Goreyshi).

R.A. Mahdavinejad studied about the machining of carbon-based materials such as WC-Co and non-oxide ceramics, which are growingly used and it’s the complexity and non-linear nature of EDM. For getting the instantaneous data from machining condition, the new method of fuzzy analysis of single machining pulses and computing the magnitude of system condition in the form of a real number between 0 and 1 has been used. Some tests with WC-Co material are carried out and finally, the results of implementation of control system on a sinking ED machine and an EDM system that has been set and it has been compared (Mahdavinejad R.A, 2009).

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Particle swarm optimization (PSO) is an evolutionary optimization technique that simulates the social behavior of bird flocking to desired places (Eberhart R.C. and Kennedy J, 1995; Kennedy, J and Eberhart R.C, 1995). PSO starts by initializing a population of random solutions and searches for optima by updating generations. PSO does not use any evolution operators. In PSO, particles fly through the problem space by following its own experience and the best experience attained by the swarm as a whole (Andreas C.Nearchou, 2011). In contrast to analytical or general heuristic methods, PSO is computationally efficient and has great capability of escaping local optima PSO was originally developed by Kennedy and eberhart in 1995, it is a population-based evolutionary algorithm.

PSO is initialized with a population of random solutions (particles) using uniform distribution. Each particle in PSO traces a trajectory in an n-dimensional search space, updating constantly a velocity vector based on best solutions found so far by that particle as well as others in the population (swarm). Each particle keeps track of its coordinates in the problem space, which are associated with the best solution (fitness) it has achieved so far, Pbest. Another ‘‘best” value tracked by the global version of the particle swarm optimizer is the overall best value, Gbest, and its location, obtained so far by any particle in the population. The particle swarm optimization algorithm, at each time step, changes the velocity of each particle moving towards its Pbest and Gbest locations. Velocity is weighted by random terms, with separate random numbers being generated for acceleration toward Pbest and Gbest locations, respectively (Ritchie Mae gamut and armacheska mesa, 2008; Thakshila,Wimalajeewa and Sudharman K. Jayaweera, 2007; Hong Zhang, Heng Li and C.M. Tam, 2006).

The objective of this work is to study the influence of pulse duration during EDM of hot pressed ZrB2-SiC composite and also to identify the best suited tool material for the selected work piece. In this work, roundness, roughness, MRR, TWR, overcut and taper angle are considered as the responses. These multi responses are combined into single response problem using DFA. For this problem, weights are assigned using PSO and interaction of Pulse on time with tool material is investigated using ANOVA.

2. Experimental set-up and method

2.1 Tool material

Graphite (GR), Titanium (Ti), Niobium (Nb), Tantalum (Ta), Tungsten (W), is selected as the tool materials. Cylindrical electrodes of 2 mm diameter from these materials were fabricated through different techniques like wire cut EDM, Diamond grinding and Extrusion process.

2.2 EDM machine specifications

Electronica small sinker machine of series 500 x 300 was used for experimentation. The specification of this machine is Max working current is 35A, Work table size is 500 x 300mm, Power supply is 3 phase, 415VAC, 50Hz. Table 1 gives the details of experimental conditions.

Table.1.Experimental conditions ____________________________________________________ Dielectric medium Kerosene

Polarity Tool: Negative

Workpiece: Positive

Open circuit voltage 100V Discharge current 2A

Pulse on 4µs, 7µs, 10µs Pulse on 1µs, 3µs, 5µs Workpiece dimension 65 x 65 x 4.2 mm Tool diameter 2mm

Dielectric medium Kerosene

2.3.0 Design of Experiments

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2.3.1 Material Removal Rate (MRR)

Material removal rate is the volume of material removed from the workpiece per unit time. It is calculated by measuring weight of workpiece before and after machining, and machining time .MRR is calculated based on the following relation.

M A B

T W W

MRR  

2.3. 2.Tool Wear Rate (TWR)

Tool wear rate is the volume of material removed from the tool per unit time. It is calculated by measuring

weight of tool before and after machining, and machining time.

M A B

T w w

TWR  

2.3.3 Roughness

The surface roughness is assessed by peak-to-valley heights (Rmax) of the craters. the surface roughness were found using video measuring machine (ARCS, Model KIM1510) and image processing using Mat lab. For roughness the hole is cut in half along the axis. Then the image is taken using video measuring machines. Peak to peak height is defined as the height difference between the highest and lowest pixel in the image. Peak to peak height was measured using Ten Point Height, where the difference of the five high local maximums and five low local minimum in a continuous sample length. Ten Point heights were got by selecting a sample length of relative a linear path (C h a n g , H . , L i m , T . V , 1 9 9 3 ) .

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Where ypi are the most important five upper points(y1, y3, y5, y7, y9) and yvi are the most important five lower points of the profile (y2, y4, y6 ,y8 , y10) and shown in Fig.1. Fig.2 shows the display of the matlab output during roughness measurement.

Fig. 1. Ten point roughness measurement Table 2 Design of experiments

Factor/Level 1 2 3 4 5

A. Tool Graphite Titanium Niobium Tantalum Tungsten

B. Pulse on (µs) 4 7 10 - -

C. Pulse off (µs) 1 3 5 - -

D. Work piece(No) 85%ZrB2 -15%SiC (1)

80%ZrB 2 -20%SiC (2)

75%ZrB 2 -25%SiC(3)

70%ZrB 2

-30%SiC (4) -

Where wB =Weight of the tool before machining wA=Weight of the tool after machining

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Fig.2.Mmatlab output during roughness measurement

2.3.4 Roundness

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Fig.3.Image of hole profile

2.3.5 Taper angle

Taper angle is calculated by measuring the top and bottom diameters of the machined hole. Diameters are measured using video measuring machine with matlab.Figure 3 shows the output of the matlab.In this figure the middle circle diameter is the nominal diameter of the hole at the top. Then the procedure is repeated to find the bottom diameter of the hole. Using the following equation the taper angle is calculated.

2.3.6 Overcut

Deviation of hole diameter (middle circle diameter in figure 3) from tool diameter (2mm) is calculated as overcut.

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Table.3.Response value

Ex.No Tool Fraction

of SiC

Pulse on time(µ s)

Pulse off time(μs)

MRR TWR

Roughness(µ m)

Roundness(µ m)

Taper

angle(deg) Overcut(mm)

(mg/min) (mg/min)

1 GR 0.15 4 1 1.1311 1.962 6.4615 83.6246 5.6967 0.4527

2 Ti 0.15 4 1 1.9119 5.005 8.4845 86.2683 5.7978 0.2536

3 Nb 0.15 4 1 0.981 6.6767 9.006 100.964 5.6286 0.6547

4 Ta 0.15 4 1 0.8208 6.006 9.1672 86.6406 5.5496 0.6453

5 W 0.15 4 1 0.961 0.1802 4.5936 81.7868 5.4505 0.6167

6 GR 0.15 4 3 0.6807 1.9019 9.96 69.2553 6.042 0.817

7 Ti 0.15 4 3 0.8108 6.006 10.4214 72.3494 6.3834 0.7182

8 Nb 0.15 4 3 0.7107 7.988 8.0801 80.8388 6.014 0.6498

9 Ta 0.15 4 3 0.6607 3.3333 5.2482 70.2493 5.8248 0.6879

10 W 0.15 4 3 0.6206 7.8078 12.1361 278.4384 5.8058 0.6618

11 GR 0.15 4 5 0.5005 1.7918 7.5726 60.8819 7.008 0.8424

12 Ti 0.15 4 5 0.3704 3.5035 12.1181 63.5355 7.5095 0.8435

13 Nb 0.15 4 5 0.3604 1.3313 10.2673 36.2793 6.6396 0.7849

14 Ta 0.15 4 5 0.5706 6.7868 11.98 68.5425 6.4504 0.7851

15 W 0.15 4 5 0.4104 4.5746 5.995 68.2633 6.4114 0.7569

16 GR 0.15 7 1 2.2723 1.6517 9.7097 137.3834 2.3984 0.3152

17 Ti 0.15 7 1 2.2523 0.4605 11.1922 130.988 2.4595 0.3162

18 Nb 0.15 7 1 2.0621 0.6206 9.1211 131.97 2.2502 0.1672

19 Ta 0.15 7 1 0 0 7.6807 128.6376 1.6206 0.1681

20 W 0.15 7 1 0.961 1.5315 9.3734 137.2272 1.0911 0.1692

21 GR 0.15 7 3 1.3514 1.001 8.2733 121.5626 2.984 0.4103

22 Ti 0.15 7 3 0.8108 1.6717 8.5646 126.6987 3.2052 0.4117

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24 Ta 0.15 7 3 1.2212 0.2903 9.0871 113.007 2.6767 0.185

25 W 0.15 7 3 1.5315 0.7007 6.4554 121.3764 2.6576 0.1806

26 GR 0.15 7 5 0.7307 0.6707 8.8288 103.5395 3.6797 0.237

27 Ti 0.15 7 5 1.1311 0.4004 6.4374 103.4304 3.7808 0.2383

28 Nb 0.15 7 5 0.4004 3.6737 9.6516 111.3293 3.4114 0.2394

29 Ta 0.15 7 5 0.5506 0.9309 10.2733 106.015 3.3523 0.2406

30 W 0.15 7 5 0.5305 0.1201 5.9699 101.0811 3.2132 0.2413

31 GR 0.15 10 1 1.9319 1.4014 10.6356 444.1051 4.1952 0.2627

32 Ti 0.15 10 1 1.3514 0.951 7.994 220.2222 4.2963 0.2633

33 Nb 0.15 10 1 1.0911 1.2813 11.8588 228.1812 3.9669 0.2445

34 Ta 0.15 10 1 1.982 1.3814 12.0901 412.4664 3.9679 0.2453

35 W 0.15 10 1 1.8218 6.5265 5.8648 490.1852 3.7988 0.2476

36 GR 0.15 10 3 0.9109 1.2513 8.8688 189.8058 4.9309 0.367

37 Ti 0.15 10 3 0.3103 0.2202 5.6466 168.6056 4.992 0.3684

38 Nb 0.15 10 3 0.4705 0.4304 8.5305 189.7577 4.8328 0.339

39 Ta 0.15 10 3 0.4805 0.3504 9.4825 171.6106 4.7337 0.3404

40 W 0.15 10 3 0.5405 6.3163 13.047 204.8048 4.4644 0.2713

41 GR 0.15 10 5 0.3504 2.3323 6.2412 165.4564 5.3964 0.4725

42 Ti 0.15 10 5 0.5606 0.1201 5.6016 149.5515 5.4174 0.6537

43 Nb 0.15 10 5 0.8308 0.1201 12.049 159.2422 5.1281 0.4745

44 Ta 0.15 10 5 0.4004 0.1301 10.5485 160.8248 5.0991 0.4155

45 W 0.15 10 5 0.3604 2.6627 11.6006 168.5735 5.0901 0.4165

46 GR 0.2 4 1 1.1512 1.2513 5.2623 45.7478 4.4011 0.1352

47 Ti 0.2 4 1 0.7107 7.1872 7.2853 16.2493 7.285 0.5166

48 Nb 0.2 4 1 0.6406 4.004 7.8068 58.6126 4.5633 0.5677

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50 W 0.2 4 1 0.7007 0.2703 3.3944 40.2262 3.284 0.1893

51 GR 0.2 4 3 0.6907 1.5616 8.7608 107.3443 3.5488 0.2924

52 Ti 0.2 4 3 0.9209 4.3343 9.2222 87.045 1.8781 0.5637

53 Nb 0.2 4 3 1.0811 4.6747 6.8809 91.991 4.5818 0.1943

54 Ta 0.2 4 3 0.8208 3.3333 5.0501 151.3413 5.8541 0.4155

55 W 0.2 4 3 0.6507 6.006 8.9349 108.96 2.1714 0.1963

56 GR 0.2 4 5 0.6907 1.6617 6.3734 152.3143 5.0609 0.5637

57 Ti 0.2 4 5 0.4905 1.0511 10.9189 191.0641 5.7626 0.8999

58 Nb 0.2 4 5 0.6306 3.3333 9.0681 168.3624 5.163 0.862

59 Ta 0.2 4 5 0.3403 4.004 10.7808 98.1331 4.163 0.9137

60 W 0.2 4 5 0.4505 4.8248 4.7958 186.7628 2.2521 0.5837

61 GR 0.2 7 1 1.9319 0.6807 8.5105 72.5796 3.1065 0.0401

62 Ti 0.2 7 1 1.9019 0.5506 6.99 65.964 3.3077 0.1012

63 Nb 0.2 7 1 1.7618 0.3103 7.9219 112.7517 2.0646 0.0226

64 Ta 0.2 7 1 1.001 0.6807 6.4815 127.5475 1.5379 0.0331

65 W 0.2 7 1 2.2322 1.2112 8.1742 180.1211 1.6791 0.0341

66 GR 0.2 7 3 1.1512 1.2513 7.0741 13.4955 5.3573 0.1673

67 Ti 0.2 7 3 0.7107 7.1872 7.3654 38.3313 1.5244 0.1887

68 Nb 0.2 7 3 0.6406 4.004 5.6346 123.3974 4.0079 0.219

69 Ta 0.2 7 3 1.011 5.8358 7.8879 42.8178 1.1961 0.2103

70 W 0.2 7 3 0.7007 0.2703 5.2562 84.6606 2.7186 0.2119

71 GR 0.2 7 5 0.6907 1.5616 7.6296 113.1802 1.9345 0.2646

72 Ti 0.2 7 5 0.9209 4.3343 5.2382 159.7177 5.1387 0.2653

73 Nb 0.2 7 5 1.0811 4.6747 8.4524 74.974 2.6372 0.2462

74 Ta 0.2 7 5 0.8208 3.3333 7.0721 456.1461 5.0806 0.2673

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76 GR 0.2 10 1 0.6907 1.6617 9.4364 79.6516 6.5085 0.2653

77 Ti 0.2 10 1 0.4905 1.0511 11.7998 161.5545 5.8288 0.2563

78 Nb 0.2 10 1 0.6306 3.3333 10.6596 125.3894 5.7597 0.3274

79 Ta 0.2 10 1 0.3403 4.004 6.8869 228.1431 7.6326 0.3584

80 W 0.2 10 1 0.4505 4.8248 4.6656 125.5816 6.4524 0.2994

81 GR 0.2 10 3 1.9319 0.6807 7.6696 28.6656 5.3023 0.4225

82 Ti 0.2 10 3 1.9019 0.5506 4.4474 149.2572 5.1932 0.4235

83 Nb 0.2 10 3 1.7618 0.3103 7.3313 448.1171 1.2102 0.4045

84 Ta 0.2 10 3 1.001 0.6807 8.2833 197.8178 4.5645 0.4055

85 W 0.2 10 3 2.2322 1.2112 11.8478 115.3463 6.6776 0.3764

86 GR 0.2 10 5 1.1512 1.2513 5.042 127.99 6.1882 0.4595

87 Ti 0.2 10 5 0.7107 7.1872 4.4024 180.5836 4.077 0.4705

88 Nb 0.2 10 5 0.6406 4.004 10.8498 107.5615 5.039 0.4415

89 Ta 0.2 10 5 1.011 5.8358 9.3493 176.6216 6.1511 0.4625

90 W 0.2 10 5 0.7007 0.2703 4.3514 174.3464 3.7858 0.88

91 GR 0.25 4 1 0.9409 1.2513 6.0881 82.8559 3.301 0.0762

92 Ti 0.25 4 1 0.6406 2.3323 8.8919 148.1622 1.5002 0.0772

93 Nb 0.25 4 1 1.1111 6.006 7.1311 156.9119 1.5713 0.5286

94 Ta 0.25 4 1 0.6807 5.6757 8.9139 109.3253 3.6744 0.2293

95 W 0.25 4 1 1.2513 1.8519 7.7538 34.7918 3.4251 0.2403

96 GR 0.25 4 3 1.0811 1.3514 8.2553 131.3093 3.2595 0.3034

97 Ti 0.25 4 3 0.6507 4.6747 7.0751 245.4344 4.3015 0.3144

98 Nb 0.25 4 3 0.9209 6.6767 13.1822 261.2212 3.2014 0.4556

99 Ta 0.25 4 3 1.1612 6.006 4.3043 197.5886 3.3025 0.5667

100 W 0.25 4 3 0.6907 7.8178 6.5876 331.8939 3.804 0.1673

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102 Ti 0.25 4 5 0.7207 2.4525 11.2643 96.2803 6.174 0.5516

103 Nb 0.25 4 5 0.5305 1.001 12.6767 288.2432 4.103 0.3524

104 Ta 0.25 4 5 0.3504 3.3333 10.4454 102.2683 5.105 0.1691

105 W 0.25 4 5 0.5305 1.5516 17.5535 128.2052 4.4253 0.5947

106 GR 0.25 7 1 2.1922 0.7307 9.3263 103.3113 4.9694 0.1212

107 Ti 0.25 7 1 2.1922 2.1321 8.7067 165.1341 0.2256 0.2624

108 Nb 0.25 7 1 1.5115 6.006 11.6106 125.0951 0.7672 0.3234

109 Ta 0.25 7 1 1.4515 0.6306 9.5395 140.2713 2.2697 0.1242

110 W 0.25 7 1 2.032 0.5806 14.2552 212.3844 0.2487 0.4155

111 GR 0.25 7 3 1.041 0.1301 6.4785 48.9219 2.4554 0.3384

112 Ti 0.25 7 3 1.2012 0.1702 7.2302 11.2953 2.2061 0.4095

113 Nb 0.25 7 3 1.021 0.1602 12.5766 66.4214 3.9388 0.4605

114 Ta 0.25 7 3 1.2713 0.2302 7.3924 15.1311 2.9388 0.4415

115 W 0.25 7 3 1.1211 5.8358 6.1021 34.7918 2.8097 0.2824

116 GR 0.25 7 5 0.4805 1.5616 4.4815 83.9519 5.8094 0.1552

117 Ti 0.25 7 5 0.4705 0.1602 7.5856 102.061 5.2398 0.1963

118 Nb 0.25 7 5 0.8609 2.6727 12.4514 59.1691 4.1497 0.4675

119 Ta 0.25 7 5 0.5405 1.4214 10.4004 50.2913 5.8224 0.4885

120 W 0.25 7 5 0.2903 3.6737 6.7177 157.4594 3.6712 0.5296

121 GR 0.25 10 1 2.4625 0.1401 6.3683 160.5936 5.1081 0.4963

122 Ti 0.25 10 1 1.4114 1.3413 8.3613 129.1331 4.3483 0.3775

123 Nb 0.25 10 1 2.2923 3.3534 9.6536 165.06 5.07 0.2083

124 Ta 0.25 10 1 2.002 2.022 6.3814 109.4454 4.6807 0.3294

125 W 0.25 10 1 0.5405 3.7437 8.014 91.4885 3.8909 0.3604

126 GR 0.25 10 3 1.8318 3.6737 6.7737 94.072 6.8949 0.4135

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128 Nb 0.25 10 3 1.001 0.8308 12.1611 183.2232 3.8138 0.2353

129 Ta 0.25 10 3 1.8018 0.6907 10.02 152.2032 6.8278 0.3364

130 W 0.25 10 3 1.3313 0.7007 4.6656 83.7257 4.2462 0.4575

131 GR 0.25 10 5 1.1512 1.001 13.3954 111.1541 5.9189 0.05

132 Ti 0.25 10 5 0.3604 0.1401 6.3493 85.0991 6.5105 0.8619

133 Nb 0.25 10 5 0.5105 0.2703 10.7047 164.4794 4.0891 0.3524

134 Ta 0.25 10 5 0.8909 0.2503 8.4294 193.5055 6.0981 0.3595

135 W 0.25 10 5 0.3303 0.2202 6.4585 190.4635 4.7077 0.2604

136 GR 0.3 4 1 0.57 1.21 9.4525 183.7878 6.7908 0.2654

137 Ti 0.3 4 1 0.77 4.33 9.3934 175.3003 5.8509 0.0862

138 Nb 0.3 4 1 1.06 0.11 9.4545 178.5746 5.8418 0.3675

139 Ta 0.3 4 1 1.06 3.33 9.5756 172.6196 5.953 0.1382

140 W 0.3 4 1 0.5 5.67 12.3994 178.3564 6.024 0.1693

141 GR 0.3 4 3 1.1812 2.4124 16.2442 223.1321 4.9239 0.1803

142 Ti 0.3 4 3 0.8408 7.4074 16.4254 229.1992 4.9149 0.3915

143 Nb 0.3 4 3 0.7307 3.6737 16.4865 240.4815 5.0761 0.0622

144 Ta 0.3 4 3 0.6406 2.6727 6.4174 238.7608 5.2272 0.5136

145 W 0.3 4 3 1.1011 2.002 16.4885 490.1431 5.3283 0.0642

146 GR 0.3 4 5 0.6707 1.1011 6.8899 204.1682 5.3694 0.6057

147 Ti 0.3 4 5 1.3113 1.1512 7.5816 214.4895 5.3503 0.1763

148 Nb 0.3 4 5 1.2613 5.1151 7.2322 206.1321 5.5315 0.0972

149 Ta 0.3 4 5 0.6306 1.1712 6.8929 205.4024 5.5325 0.1783

150 W 0.3 4 5 0.9209 5.6757 6.4835 201.049 5.7537 0.1793

151 GR 0.3 7 1 2.5125 0.1001 10.999 66.1551 4.7337 0.0279

152 Ti 0.3 7 1 2.4224 0.1301 11.3704 147.1672 4.6146 0.4816

(13)

154 Ta 0.3 7 1 2.3023 0.1301 11.002 138.7207 4.8969 0.0231

155 W 0.3 7 1 1.952 0.3504 11.5135 254.1071 4.9079 0.3444

156 GR 0.3 7 3 1.992 1.3514 10.5936 83.3573 4.3684 0.4656

157 Ti 0.3 7 3 1.0911 0.1802 10.5946 79.7547 4.3593 0.2263

158 Nb 0.3 7 3 1.1812 0.1401 10.1752 76.2723 4.5105 0.1072

159 Ta 0.3 7 3 0.3904 0.1301 9.8258 74.3013 4.5315 0.2884

160 W 0.3 7 3 2.0821 0.1702 10.1772 76.8448 4.5425 0.3594

161 GR 0.3 7 5 0.7608 1.6917 9.8178 84.3333 4.2332 0.3004

162 Ti 0.3 7 5 0.5105 2.002 9.8188 84.5746 4.1942 0.4015

163 Nb 0.3 7 5 1.1211 2.002 9.8198 86.6676 4.2452 0.0621

164 Ta 0.3 7 5 0.5906 5.6757 9.8308 94.7067 4.2963 0.1632

165 W 0.3 7 5 1.1211 2.1221 9.8318 92.3453 4.3473 0.2143

166 GR 0.3 10 1 2.012 0.1502 15.5886 97.5715 3.6476 0.2854

167 Ti 0.3 10 1 2.002 1.6917 16.2702 99.7447 3.4084 0.0962

168 Nb 0.3 10 1 2.042 2.6727 11.5265 150.4564 1.3273 0.6077

169 Ta 0.3 10 1 0.5005 2.8328 14.5505 168.8358 1.1581 0.7989

170 W 0.3 10 1 0.4505 3.9039 14.5515 170.6086 1.4795 0.7999

171 GR 0.3 10 3 2.002 1.2012 12.6706 153.8628 1.5906 0.7008

172 Ti 0.3 10 3 1.021 0.3804 12.6716 155.9159 1.6917 0.5817

173 Nb 0.3 10 3 1.7217 1.2513 15.3053 136.1571 3.3143 0.5626

174 Ta 0.3 10 3 1.5215 7.8078 15.5966 138.6806 3.3353 0.5236

175 W 0.3 10 3 1.2513 1.3514 15.3073 137.3203 3.3864 0.4846

176 GR 0.3 10 5 2.0721 1.2112 16.4594 107.051 3.6977 0.1853

177 Ti 0.3 10 5 1.0611 3.3333 17.2712 109.8949 3.7487 0.0962

178 Nb 0.3 10 5 1.0711 4.3544 17.2712 118.6336 3.8688 0.4966

179 Ta 0.3 10 5 1.8118 2.1722 14.6286 136.1011 3.2582 0.5967

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2.4 Desirability functional analysis

Desirability functional analysis is used for optimization of machining parameters. Initially the data are normalized to a common scale [0, 1], combine them using the geometric mean and optimize the overall metric. The normalized data are shown in table 4.The objective of MRR is too maximized; therefore equation (1) is employed for normalization.

For maximization of fr(x), the function is

(1)

Can be used, where A, B and s are chosen by investigator. For the responses like TWR, roughness, roundness, taper angle and overcut, therefore equation (2) is employed for normalization.

(2)

Table 4.Normalized value

Ex.No MRR TWR

Roughness Roundness

Taper

angle Overcut 1. 0.450189 0.754382 0.783383 0.848965 0.261361 0.517338

2. 0.760955 0.373435 0.640507 0.843444 0.247712 0.74077

3. 0.390448 0.164159 0.603675 0.812757 0.270555 0.290652

4. 0.326687 0.248122 0.59229 0.842667 0.28122 0.301201

5. 0.382488 0.977441 0.915305 0.852802 0.2946 0.333296

6. 0.270925 0.761905 0.536298 0.87897 0.214743 0.108518

7. 0.322706 0.248122 0.503711 0.872509 0.168651 0.219392

8. 0.282866 0 0.669068 0.854782 0.218523 0.296151

9. 0.262965 0.582712 0.869074 0.876894 0.244066 0.253395

10. 0.247005 0.022559 0.382609 0.442162 0.246632 0.282684

11. 0.199204 0.775689 0.704911 0.896455 0.084326 0.080013

12. 0.147423 0.561405 0.38388 0.890914 0.016619 0.078779

13. 0.143443 0.833338 0.514595 0.947829 0.134062 0.14454

14. 0.227104 0.150376 0.393634 0.880459 0.159606 0.144316

15. 0.163343 0.427316 0.81633 0.881042 0.164871 0.175962

16. 0.904398 0.793227 0.553976 0.736708 0.706656 0.671642

17. 0.896438 0.942351 0.449273 0.750062 0.698407 0.67052

18. 0.820736 0.922308 0.595546 0.748012 0.726664 0.837729

19. 0 1 0.697276 0.75497 0.811665 0.836719

20. 0.382488 0.808275 0.577727 0.737034 0.883151 0.835484

21. 0.537871 0.874687 0.655423 0.769744 0.627596 0.56492

22. 0.322706 0.790724 0.63485 0.759019 0.597732 0.563349

23. 0.378507 0.963658 0.757089 0.78548 0.646254 0.818651

24. 0.48605 0.963658 0.597948 0.787609 0.669083 0.817753

25. 0.609552 0.912281 0.783814 0.770133 0.671662 0.822691

26. 0.290826 0.916037 0.61619 0.807379 0.533671 0.759398

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28. 0.159363 0.540098 0.558079 0.791113 0.569893 0.756705

29. 0.219144 0.883463 0.514171 0.80221 0.577872 0.755359

30. 0.211144 0.984965 0.818103 0.812513 0.596652 0.754573

31. 0.768915 0.824562 0.488583 0.096223 0.464075 0.730558

32. 0.537871 0.880946 0.675149 0.563727 0.450425 0.729884

33. 0.434269 0.839597 0.402194 0.547107 0.494897 0.750982

34. 0.788856 0.827066 0.385858 0.162289 0.494762 0.750084

35. 0.725095 0.182962 0.825526 0 0.517591 0.747503

36. 0.362547 0.843353 0.613365 0.627241 0.36475 0.613511

37. 0.123502 0.972434 0.840936 0.671511 0.356501 0.61194

38. 0.187264 0.946119 0.637258 0.627341 0.377994 0.644933

39. 0.191244 0.956134 0.570022 0.665236 0.391373 0.643362

40. 0.215124 0.209276 0.318276 0.595921 0.427731 0.720907

41. 0.139463 0.708025 0.798942 0.678087 0.301904 0.495118

42. 0.223124 0.984965 0.844114 0.711299 0.299068 0.291774

43. 0.330667 0.984965 0.388761 0.691063 0.338126 0.492874

44. 0.159363 0.983713 0.494735 0.687758 0.342041 0.559084

45. 0.143443 0.666662 0.420429 0.671578 0.343256 0.557962

46. 0.458189 0.843353 0.868078 0.928058 0.436276 0.873639

47. 0.282866 0.10025 0.725201 0.989655 0.046929 0.445629

48. 0.254965 0.498748 0.68837 0.901194 0.414378 0.388284

49. 0.402388 0.269429 0.676985 0.857819 0.218294 0.454607

50. 0.278886 0.966162 1 0.939588 0.587093 0.812928

51. 0.274905 0.804507 0.620993 0.799434 0.551343 0.697228

52. 0.366527 0.457399 0.588406 0.841822 0.7769 0.392773

53. 0.430289 0.414785 0.753763 0.831494 0.411881 0.807317

54. 0.326687 0.582712 0.883065 0.707561 0.240111 0.559084

55. 0.258985 0.248122 0.608697 0.79606 0.737303 0.805072

56. 0.274905 0.791975 0.789605 0.705529 0.347199 0.392773

57. 0.195224 0.868415 0.468575 0.624614 0.252464 0.015486

58. 0.250985 0.582712 0.59929 0.672018 0.333414 0.058018

59. 0.135443 0.498748 0.478328 0.818669 0.468422 0

60. 0.179303 0.395994 0.901025 0.633595 0.726407 0.370329

61. 0.768915 0.914785 0.638671 0.872028 0.611057 0.980361

62. 0.756975 0.931072 0.746057 0.885843 0.583894 0.911794

63. 0.701214 0.961154 0.680241 0.788143 0.751721 1

64. 0.398408 0.914785 0.781971 0.757246 0.82283 0.988217

65. 0.888438 0.848373 0.662422 0.647464 0.803767 0.987095

66. 0.458189 0.843353 0.740118 0.995406 0.307182 0.837616

67. 0.282866 0.10025 0.719544 0.943544 0.824652 0.813601

68. 0.254965 0.498748 0.841784 0.765913 0.489361 0.779598

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70. 0.278886 0.966162 0.868509 0.846801 0.663426 0.787566

71. 0.274905 0.804507 0.700885 0.787248 0.769286 0.728426

72. 0.366527 0.457399 0.86978 0.69007 0.336695 0.72764

73. 0.430289 0.414785 0.642774 0.867029 0.674416 0.749074

74. 0.326687 0.582712 0.740259 0.071079 0.344539 0.725396

75. 0.258985 0.248122 0.902797 0.975843 0.451168 0.791606

76. 0.274905 0.791975 0.573278 0.857261 0.151762 0.72764

77. 0.195224 0.868415 0.406361 0.686234 0.243526 0.73774

78. 0.250985 0.582712 0.486888 0.761753 0.252855 0.657951

79. 0.135443 0.498748 0.753339 0.547187 0 0.623162

80. 0.179303 0.395994 0.91022 0.761352 0.159336 0.689373

81. 0.768915 0.914785 0.69806 0.963728 0.314608 0.551229

82. 0.756975 0.931072 0.925631 0.711913 0.329337 0.550107

83. 0.701214 0.961154 0.721953 0.087845 0.867072 0.571429

84. 0.398408 0.914785 0.654717 0.610511 0.414216 0.570306

85. 0.888438 0.848373 0.402971 0.782725 0.128932 0.602963

86. 0.458189 0.843353 0.883637 0.756322 0.195005 0.509707

87. 0.282866 0.10025 0.928809 0.646498 0.480032 0.497363

88. 0.254965 0.498748 0.473455 0.798981 0.350155 0.529907

89. 0.402388 0.269429 0.579429 0.654772 0.200014 0.50634

90. 0.278886 0.966162 0.932411 0.659523 0.519347 0.037818

91. 0.374488 0.843353 0.809755 0.85057 0.584798 0.93985

92. 0.254965 0.708025 0.611734 0.7142 0.82792 0.938727

93. 0.442229 0.248122 0.736092 0.695929 0.818321 0.432162

94. 0.270925 0.289472 0.61018 0.795297 0.534386 0.76804

95. 0.49803 0.768165 0.692113 0.950935 0.568044 0.755695

96. 0.430289 0.830821 0.656694 0.749391 0.590401 0.684884

97. 0.258985 0.414785 0.740047 0.511079 0.449723 0.67254

98. 0.366527 0.164159 0.308727 0.478114 0.598245 0.514084

99. 0.462169 0.248122 0.935737 0.610989 0.584596 0.389406

100. 0.274905 0.021307 0.774477 0.330538 0.516889 0.837616

101. 0.203184 0.843353 0.006639 0.746329 0.025422 0.497251

102. 0.286846 0.692977 0.444181 0.822537 0.196922 0.406352

103. 0.211144 0.874687 0.344429 0.421688 0.476522 0.629896

104. 0.139463 0.582712 0.502016 0.810034 0.341245 0.835596

105. 0.211144 0.805759 0 0.755873 0.433009 0.357985

106. 0.872517 0.908525 0.581054 0.807856 0.359552 0.88935

107. 0.872517 0.733087 0.624814 0.67876 1 0.730894

108. 0.601592 0.248122 0.419723 0.762368 0.92688 0.66244

109. 0.577711 0.921057 0.565996 0.730677 0.724031 0.885984

110. 0.808756 0.927316 0.232946 0.580093 0.996881 0.559084

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112. 0.47809 0.978693 0.729093 1 0.732618 0.565818

113. 0.406368 0.979945 0.351498 0.884888 0.49869 0.508585

114. 0.50599 0.971182 0.717637 0.99199 0.633698 0.529907

115. 0.446209 0.269429 0.808766 0.950935 0.651127 0.70845

116. 0.191244 0.804507 0.923223 0.848281 0.246146 0.851195

117. 0.187264 0.979945 0.703992 0.810466 0.323046 0.805072

118. 0.342647 0.665411 0.360341 0.900032 0.470217 0.500729

119. 0.215124 0.822058 0.505195 0.91857 0.24439 0.477163

120. 0.115542 0.540098 0.765289 0.694786 0.534818 0.43104

121. 0.9801 0.982461 0.789965 0.688241 0.340826 0.46841

122. 0.561751 0.832086 0.649208 0.753936 0.443405 0.601728

123. 0.912358 0.580195 0.557938 0.678914 0.34597 0.791606

124. 0.796816 0.74687 0.78904 0.795047 0.398528 0.655706

125. 0.215124 0.531335 0.673736 0.832544 0.505157 0.620918

126. 0.729075 0.540098 0.761334 0.827149 0.099595 0.561329

127. 0.258985 0.941099 0.838316 0.793368 0.469758 0.829873

128. 0.398408 0.895994 0.380843 0.640987 0.515566 0.761306

129. 0.717134 0.913533 0.532061 0.705761 0.108654 0.647851

130. 0.529871 0.912281 0.91022 0.848754 0.457189 0.511952

131. 0.458189 0.874687 0.29367 0.791479 0.231362 0.969251

132. 0.143443 0.982461 0.791307 0.845886 0.151492 0.05813

133. 0.203184 0.966162 0.483703 0.680127 0.478399 0.629896

134. 0.354587 0.968665 0.644398 0.619515 0.207169 0.621928

135. 0.131463 0.972434 0.783595 0.625868 0.394883 0.733139

136. 0.226866 0.848523 0.572141 0.639808 0.113649 0.727528

137. 0.306468 0.457937 0.576315 0.657531 0.240543 0.928628

138. 0.421891 0.986229 0.572 0.650694 0.241771 0.61295

139. 0.421891 0.583125 0.563447 0.663129 0.226758 0.870273

140. 0.199005 0.290185 0.364013 0.651149 0.217173 0.835372

141. 0.470129 0.697997 0.092471 0.55765 0.365695 0.823028

142. 0.334647 0.072684 0.079673 0.544981 0.36691 0.586017

143. 0.290826 0.540098 0.075358 0.521422 0.345146 0.955561

144. 0.254965 0.665411 0.786498 0.525015 0.324747 0.448996

145. 0.438249 0.749374 0.075217 8.79E-05 0.311098 0.953316

146. 0.266945 0.862156 0.753127 0.59725 0.305549 0.34564

147. 0.52191 0.855884 0.704275 0.575697 0.308127 0.827517

148. 0.50201 0.359652 0.728952 0.593149 0.283664 0.916283

149. 0.250985 0.85338 0.752915 0.594673 0.283529 0.825272

150. 0.366527 0.289472 0.781829 0.603763 0.253665 0.82415

151. 1 0.987469 0.462918 0.885444 0.391373 0.994052

152. 0.964139 0.983713 0.436687 0.716277 0.407452 0.484906

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154. 0.916338 0.983713 0.462706 0.733915 0.36934 0.999439

155. 0.776915 0.956134 0.426581 0.492969 0.367855 0.638873

156. 0.792836 0.830821 0.49155 0.849523 0.440691 0.502862

157. 0.434269 0.977441 0.491479 0.857046 0.44192 0.771406

158. 0.470129 0.982461 0.5211 0.864317 0.421507 0.905061

159. 0.155383 0.983713 0.545776 0.868433 0.418672 0.701717

160. 0.828697 0.978693 0.520958 0.863122 0.417186 0.62204

161. 0.302806 0.78822 0.546341 0.847485 0.458944 0.68825

162. 0.203184 0.749374 0.546271 0.846981 0.46421 0.574795

163. 0.446209 0.749374 0.5462 0.84261 0.457324 0.955673

164. 0.235065 0.289472 0.545423 0.825823 0.450425 0.842217

165. 0.446209 0.734339 0.545352 0.830754 0.44354 0.784873

166. 0.800796 0.981197 0.138773 0.819841 0.538005 0.705084

167. 0.796816 0.78822 0.090634 0.815303 0.570298 0.917405

168. 0.812736 0.665411 0.425663 0.709409 0.851262 0.343396

169. 0.199204 0.645368 0.21209 0.67103 0.874106 0.12883

170. 0.179303 0.511279 0.212019 0.667328 0.830714 0.127707

171. 0.796816 0.849624 0.344859 0.702296 0.815715 0.238918

172. 0.406368 0.952379 0.344789 0.698009 0.802066 0.372573

173. 0.685254 0.843353 0.158781 0.739268 0.583003 0.394007

174. 0.605572 0.022559 0.138208 0.733999 0.580167 0.437774

175. 0.49803 0.830821 0.15864 0.736839 0.573269 0.48154

176. 0.824716 0.848373 0.077272 0.800047 0.531241 0.817417

177. 0.422328 0.582712 0.019938 0.794108 0.524355 0.917405

178. 0.426308 0.454882 0.019938 0.77586 0.508141 0.468073

179. 0.721114 0.728067 0.206574 0.739385 0.590576 0.35574

180. 0.199204 0.586467 0.206574 0.74783 0.613541 0.479295

2.4.1 Overall desirability (Global desirability)

Overall desirability functional value (D) can be calculated by geometric mean of individual desirability values. If there are “R” number of individual desirability values (d1…… dr) on [0, 1] scale, they can be combined and the

value of D is derived using equation (3). (3) The geometric mean has the property that if any one model is undesirable (dr = 0), the overall desirability is also unacceptable (D = 0).The overall desirability (D) of each experiment is found out and shown in table.5 using weight based approach. MATLAB software is employed to execute the algorithm of PSO for finding the weights of the individual responses.

Table.5Individual and global desirability values

Ex.N MRR TWR Roughness Roundness Taper angle Overcut Global

1. 0.992684 0.903026 0.98505 0.916008 0.988129 0.985346 0.787537

2. 0.99749 0.70014 0.972887 0.912811 0.987657 0.993301 0.608448

3. 0.991385 0.520001 0.969339 0.894864 0.988433 0.972701 0.429938

4. 0.98976 0.603851 0.968201 0.91236 0.988773 0.973479 0.508176

5. 0.991197 0.991776 0.994555 0.918224 0.989182 0.975689 0.86644

6. 0.988057 0.906275 0.962286 0.933214 0.986402 0.95147 0.754705

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8. 0.98845 0 0.97551 0.919365 0.986556 0.97311 0

9. 0.987786 0.822465 0.991379 0.932033 0.987527 0.969717 0.718862

10. 0.987218 0.253551 0.942445 0.645806 0.987619 0.972096 0.146263

11. 0.985266 0.912174 0.978656 0.943115 0.97823 0.944998 0.766828

12. 0.982541 0.811452 0.942638 0.939987 0.964192 0.944669 0.643463

13. 0.982294 0.936149 0.959837 0.9717 0.982275 0.957599 0.806738

14. 0.986455 0.503756 0.944098 0.934061 0.983801 0.957566 0.412825

15. 0.983469 0.735137 0.987557 0.934392 0.984085 0.961828 0.631466

16. 0.999076 0.919585 0.964214 0.848979 0.996915 0.991124 0.743099

17. 0.998995 0.978741 0.951831 0.85719 0.99681 0.991087 0.788119

18. 0.998184 0.971155 0.968528 0.855934 0.997162 0.996042 0.798169

19. 0 1 0.977998 0.860191 0.998145 0.996015 0

20. 0.991197 0.925861 0.966715 0.84918 0.998895 0.995982 0.749506

21. 0.994311 0.952701 0.97427 0.869169 0.995862 0.987289 0.78869

22. 0.989649 0.918534 0.972355 0.862659 0.99543 0.987228 0.749322

23. 0.991102 0.986692 0.982977 0.878645 0.996122 0.995528 0.837573

24. 0.993385 0.986692 0.968769 0.87992 0.99643 0.995503 0.828805

25. 0.995456 0.967321 0.985083 0.869404 0.996464 0.995638 0.818183

26. 0.988702 0.96876 0.970567 0.891686 0.994427 0.993854 0.819246

27. 0.992684 0.981561 0.985182 0.891821 0.994197 0.993811 0.845861

28. 0.983246 0.800169 0.964653 0.882015 0.995008 0.993775 0.66192

29. 0.986131 0.956149 0.959788 0.888623 0.995131 0.993735 0.795251

30. 0.985794 0.994532 0.987689 0.89472 0.995414 0.993712 0.856992

31. 0.997585 0.932569 0.95677 0.28526 0.993191 0.992992 0.250413

32. 0.994311 0.955162 0.976054 0.735568 0.992927 0.992972 0.67228

33. 0.992356 0.938688 0.945352 0.723868 0.993759 0.993606 0.629414

34. 0.99782 0.933593 0.942937 0.377462 0.993757 0.993579 0.327378

35. 0.997047 0.540815 0.98824 0 0.994156 0.993502 0

36. 0.990709 0.940205 0.970292 0.778871 0.991064 0.989116 0.690058

37. 0.980942 0.989935 0.989368 0.807858 0.990862 0.989059 0.760639

38. 0.984706 0.980155 0.972582 0.778938 0.991379 0.990223 0.717799

39. 0.984897 0.983897 0.965914 0.803804 0.991686 0.990169 0.738776

40. 0.985963 0.567765 0.931801 0.757785 0.99247 0.992697 0.389433

41. 0.98204 0.882536 0.986246 0.812087 0.989398 0.984377 0.676054

42. 0.986295 0.994532 0.989598 0.833162 0.989314 0.972785 0.778333

43. 0.989871 0.994532 0.943373 0.820377 0.990396 0.984277 0.742712

44. 0.983246 0.994075 0.957509 0.818273 0.990497 0.98706 0.748719

45. 0.982294 0.863518 0.947942 0.807901 0.990529 0.987015 0.635103

46. 0.992845 0.940205 0.991309 0.960786 0.992645 0.996979 0.879873

47. 0.98845 0.435004 0.980371 0.994444 0.973141 0.982058 0.400618

48. 0.987506 0.777433 0.977223 0.945783 0.99219 0.979032 0.689255

(20)

50. 0.988321 0.987619 1 0.967163 0.995271 0.995371 0.93522

51. 0.98819 0.924296 0.971032 0.886974 0.994715 0.991954 0.776223

52. 0.990809 0.753461 0.967808 0.91187 0.997756 0.979284 0.643733

53. 0.992272 0.727261 0.98271 0.905859 0.992137 0.995217 0.634302

54. 0.98976 0.822465 0.992357 0.830814 0.987383 0.98706 0.654106

55. 0.987648 0.603851 0.969834 0.884966 0.997291 0.995155 0.508006

56. 0.98819 0.91906 0.985531 0.829534 0.990629 0.979284 0.720292

57. 0.985083 0.950223 0.954305 0.777121 0.987824 0.910867 0.624609

58. 0.987363 0.822465 0.968903 0.808185 0.990272 0.938218 0.590805

59. 0.981775 0.777433 0.955519 0.898345 0.993273 0 0

60. 0.984313 0.71516 0.99359 0.783089 0.997159 0.977994 0.53414

61. 0.997585 0.968281 0.972715 0.929258 0.995626 0.999556 0.868913

62. 0.997442 0.974485 0.982087 0.937117 0.995223 0.997934 0.888441

63. 0.99674 0.985764 0.976507 0.880239 0.997463 1 0.842418

64. 0.991569 0.968281 0.98494 0.861579 0.998266 0.999735 0.813131

65. 0.998912 0.942227 0.974909 0.792227 0.998058 0.999709 0.725313

66. 0.992845 0.940205 0.981603 0.997536 0.98955 0.996039 0.900913

67. 0.98845 0.435004 0.979897 0.969343 0.998286 0.99539 0.405839

68. 0.987506 0.777433 0.98943 0.866849 0.99366 0.994438 0.650649

69. 0.99166 0.622125 0.976719 0.964175 0.998751 0.994716 0.577194

70. 0.988321 0.987619 0.991339 0.914756 0.996355 0.994665 0.877215

71. 0.98819 0.924296 0.97831 0.879704 0.997668 0.992927 0.778696

72. 0.990809 0.753461 0.991429 0.819745 0.990358 0.992903 0.59661

73. 0.992272 0.727261 0.973099 0.926399 0.9965 0.993549 0.644085

74. 0.98976 0.822465 0.981615 0.242529 0.990561 0.992835 0.190595

75. 0.987648 0.603851 0.993711 0.986983 0.992941 0.994779 0.577765

76. 0.98819 0.91906 0.966254 0.920793 0.98336 0.992903 0.788963

77. 0.985083 0.950223 0.945954 0.817301 0.987507 0.99321 0.709793

78. 0.987363 0.822465 0.956565 0.864323 0.987838 0.990667 0.657049

79. 0.981775 0.777433 0.982676 0.723924 0 0.989462 0

80. 0.984313 0.71516 0.994213 0.864079 0.983786 0.991702 0.589999

81. 0.997585 0.968281 0.978066 0.980399 0.989761 0.986747 0.904604

82. 0.997442 0.974485 0.995243 0.833548 0.990164 0.986702 0.787798

83. 0.99674 0.985764 0.980099 0.271671 0.998731 0.987543 0.258032

84. 0.991569 0.968281 0.974205 0.76767 0.992187 0.987499 0.703525

85. 0.998912 0.942227 0.945465 0.876992 0.981934 0.988732 0.757678

86. 0.992845 0.940205 0.992396 0.861016 0.985556 0.985018 0.77433

87. 0.98845 0.435004 0.995454 0.791593 0.99349 0.984477 0.33139

88. 0.987506 0.777433 0.954915 0.886704 0.990704 0.985875 0.63491

89. 0.99166 0.622125 0.96689 0.797005 0.985779 0.984871 0.46157

90. 0.988321 0.987619 0.995691 0.800098 0.994186 0.929267 0.718396

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92. 0.987506 0.882536 0.970132 0.834981 0.998321 0.998585 0.703776

93. 0.992522 0.603851 0.981273 0.823467 0.998217 0.981383 0.474426

94. 0.988057 0.638492 0.96998 0.884512 0.994438 0.994106 0.535075

95. 0.993607 0.908962 0.97755 0.973404 0.994979 0.993745 0.849732

96. 0.992272 0.935125 0.974387 0.856779 0.995321 0.991557 0.764507

97. 0.987648 0.727261 0.981597 0.697924 0.992913 0.991153 0.484268

98. 0.990809 0.520001 0.930051 0.673431 0.995438 0.985206 0.316472

99. 0.992924 0.603851 0.99591 0.767992 0.995234 0.979095 0.446861

100. 0.98819 0.248366 0.984355 0.552585 0.994144 0.996039 0.132193

101. 0.985445 0.940205 0.733877 0.854901 0.967846 0.984472 0.553865

102. 0.988577 0.875702 0.951162 0.900618 0.985642 0.98003 0.716341

103. 0.985794 0.952701 0.936352 0.629608 0.993425 0.9897 0.544365

104. 0.98204 0.822465 0.958372 0.893256 0.990477 0.995985 0.682109

105. 0.985794 0.924817 0 0.860742 0.992578 0.977252 0

106. 0.998746 0.965878 0.967057 0.891968 0.990938 0.997377 0.822402

107. 0.998746 0.893717 0.971399 0.812519 1 0.993003 0.699579

108. 0.995336 0.603851 0.947844 0.864696 0.999324 0.990818 0.487753

109. 0.994965 0.970678 0.965492 0.845248 0.99713 0.997292 0.783772

110. 0.998049 0.97306 0.914028 0.746934 0.999972 0.98706 0.654432

111. 0.991927 0.994075 0.984957 0.957103 0.996817 0.990246 0.917558

112. 0.993234 0.992236 0.980694 1 0.997235 0.987325 0.951607

113. 0.99175 0.992695 0.937526 0.936575 0.993827 0.984969 0.846208

114. 0.993752 0.989473 0.979737 0.9957 0.995948 0.985875 0.941844

115. 0.992603 0.622125 0.98699 0.973404 0.996189 0.992309 0.586473

116. 0.984897 0.924296 0.995083 0.915612 0.987601 0.996398 0.816182

117. 0.984706 0.992695 0.978577 0.893512 0.989994 0.995155 0.842056

118. 0.990195 0.862931 0.938965 0.94513 0.993307 0.984626 0.741638

119. 0.985963 0.931544 0.958746 0.955511 0.987538 0.983563 0.817258

120. 0.980341 0.800169 0.983631 0.822742 0.994446 0.981326 0.619511

121. 0.999815 0.993617 0.985559 0.81858 0.990466 0.983155 0.780448

122. 0.994708 0.93564 0.973698 0.859559 0.992788 0.988686 0.764574

123. 0.999157 0.821178 0.964638 0.812618 0.990598 0.994779 0.633791

124. 0.997913 0.899762 0.985487 0.884363 0.991846 0.990591 0.768847

125. 0.985963 0.795446 0.975928 0.906471 0.993941 0.989382 0.682288

126. 0.997097 0.800169 0.983316 0.903319 0.97968 0.987148 0.685363

127. 0.987648 0.97827 0.989178 0.883362 0.993298 0.995832 0.835101

128. 0.991569 0.961035 0.942176 0.78797 0.994121 0.99391 0.699021

129. 0.996946 0.967801 0.961816 0.829681 0.98044 0.990323 0.747581

130. 0.994174 0.967321 0.994213 0.915885 0.993059 0.985115 0.856673

131. 0.992845 0.952701 0.927186 0.882234 0.987057 0.999301 0.76318

132. 0.982294 0.993617 0.985662 0.914226 0.983344 0.938259 0.811465

(22)

134. 0.990507 0.988545 0.973251 0.773716 0.986087 0.989418 0.719375

135. 0.981506 0.989935 0.985066 0.777957 0.991765 0.993071 0.733346

136. 0.986445 0.942287 0.966135 0.787193 0.980832 0.9929 0.688455

137. 0.989179 0.753782 0.966569 0.798803 0.987399 0.998343 0.567499

138. 0.992092 0.994994 0.966121 0.794341 0.987444 0.989096 0.73988

139. 0.992092 0.822676 0.965223 0.802439 0.98688 0.996892 0.621918

140. 0.985257 0.639061 0.939552 0.794639 0.986501 0.995979 0.461881

141. 0.99308 0.877992 0.863381 0.731309 0.991087 0.995647 0.543244

142. 0.989979 0.387217 0.855482 0.722359 0.991116 0.988101 0.231991

143. 0.988702 0.800169 0.852548 0.705456 0.990577 0.998982 0.470849

144. 0.987506 0.862931 0.985291 0.708057 0.99004 0.982223 0.578111

145. 0.992439 0.900852 0.852449 0.006712 0.989662 0.99893 0.005057

146. 0.987923 0.947738 0.982659 0.75869 0.989503 0.976484 0.674468

147. 0.994035 0.945237 0.978601 0.743896 0.989577 0.995768 0.674013

148. 0.99368 0.690675 0.980683 0.755895 0.988849 0.998043 0.502099

149. 0.987363 0.944236 0.982642 0.756934 0.988845 0.995707 0.682764

150. 0.990809 0.638492 0.984929 0.763112 0.987866 0.995677 0.467687

151. 1 0.995447 0.95359 0.936891 0.991686 0.999866 0.881829

152. 0.999664 0.994075 0.950164 0.836282 0.992041 0.983918 0.770748

153. 0.998746 0.985299 0.950154 0.830957 0.991463 0.997065 0.768061

154. 0.999197 0.994075 0.953563 0.847253 0.991174 0.999987 0.795384

155. 0.99768 0.983897 0.948792 0.684562 0.991139 0.990014 0.625606

156. 0.997867 0.935125 0.957127 0.91633 0.992734 0.984719 0.800035

157. 0.992356 0.991776 0.957119 0.920669 0.992758 0.994203 0.855991

158. 0.99308 0.993617 0.960581 0.924846 0.992341 0.997768 0.867955

159. 0.983017 0.994075 0.963327 0.927203 0.992281 0.992097 0.859246

160. 0.998273 0.992236 0.960565 0.924161 0.99225 0.989422 0.863259

161. 0.989069 0.91748 0.963389 0.915152 0.993092 0.991666 0.787904

162. 0.985445 0.900852 0.963381 0.91486 0.993193 0.987673 0.767513

163. 0.992603 0.900852 0.963373 0.912328 0.993061 0.998985 0.779668

164. 0.986768 0.638492 0.963289 0.902544 0.992927 0.996161 0.541803

165. 0.992603 0.894269 0.963281 0.905427 0.992791 0.994589 0.764454

166. 0.997958 0.993154 0.885279 0.899035 0.994498 0.992203 0.778377

167. 0.997913 0.91748 0.862313 0.896365 0.995014 0.998071 0.702797

168. 0.998094 0.862931 0.948666 0.831975 0.998568 0.976342 0.662752

169. 0.985266 0.853433 0.908754 0.807548 0.998803 0.955134 0.588683

170. 0.984313 0.784447 0.908735 0.805158 0.998351 0.954947 0.538613

171. 0.997913 0.94273 0.936424 0.827495 0.998189 0.96844 0.704698

172. 0.99175 0.982497 0.936412 0.824785 0.998039 0.978127 0.734655

173. 0.996529 0.940205 0.892667 0.850558 0.995209 0.979353 0.693362

174. 0.995396 0.253551 0.885056 0.847305 0.995166 0.981667 0.184898

(23)

176. 0.998229 0.942227 0.853868 0.887338 0.994386 0.995494 0.705439

177. 0.992101 0.822465 0.785398 0.883803 0.994271 0.998071 0.562063

178. 0.992187 0.751958 0.785398 0.872863 0.993993 0.983139 0.499829

179. 0.996997 0.891497 0.907278 0.85063 0.995324 0.977114 0.667121

180. 0.985266 0.82438 0.907278 0.855822 0.995662 0.983661 0.617678

2.5 Fitness function

To find out the weights corresponding to each responses by optimisation algorithms fitness function and constraints are developed, considering the objective of maximizing the overall desirability values and constraint is that sum of the weights should be equal to one,

So the fitness function is, Max f(x) = D1+ D2+ D3+ D4+ ………. + D20

Where D1= d1,1w1 x d1,2w2 x d1,3w3 x d1,4w4 x d1,5w5 x d1,6w6

Subjected to w1 + w2 + ……. + w6 =1

The above equation can be written as

Maximize

 

  20 1 6 1 , ) ( ) ( i j w j i j d x f Subjected to

2.6 Particle Swarm Optimisation (PSO)

The procedure for implementing PSO is given by the following steps

(i) Initialize a population of particles with random positions and velocities in the n-dimensional problem space using a uniform probability distribution function;

(ii) For each particle in swarm, evaluate its fitness value;

(iii) Compare each particle’s fitness evaluation, with the current particle’s Pbest. If current value is better than Pbest, set its Pbest value to the current value and the Pbest location to the current location in n-dimensional space;

(iv) Compare the fitness evaluation with the population’s overall previous best. If current value is better than Gbest, then reset Gbest to the current particle’s array index and value;

(v) Change the velocity and position of the particle using eqn (5) and (6)

(vi) Loop to step (ii) until a stopping criterion is met, usually a maximum number of iterations (generations). (5)

(6)

Where i = 1, 2. . . N is the particle’s index. Variables c1 and c2 are two positive constants, called Cognitive learning rate and Social learning rate, respectively and w is the inertia Weight factor. According to its previous position and its velocity, the variable w is responsible for dynamically adjusting the velocity of the particles. So it is responsible for balancing between local and global search. Hence requiring less iteration for the algorithm to converge. A low value of inertia weight implies a local search, while a high value leads to a global search. Applying a large inertia weight at the start of the algorithm and making it decay to a small value through the PSO execution makes the algorithm search globally at the beginning of the search, and search locally at the end of the execution. In this problem have total six variables, sum of the variables equal to one, constrained particle swarm optimisation is used for solving the problem. Step by step procedure of PSO implementation for this study is described with the help of flow chart in Fig.4

(24)

Fig.4.Flow chart

3 Results and discussion

3.1 Particle swarm optimization

(25)

0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

x 104 102

104 106 108 110 112 114 116 118

Fig.5.Convergence graph

3.2 Ranking

To rank the tools based on the global desirability values, main effect table is constructed by taking average of Global Desirability value corresponding to each tool, pulse on time and off time. Based on Global Desirability value, the tools are rated and the best suited pulse on time and off time is selected, which are shown in the table 6.They ranked the tools as follows; Graphite, Titanium, Niobium, Tungsten, Tantalum. The machinability of workpieces increases when SiC contribution increases till 25% then it start decreasing. Pulse on time of 7 µs and off time of 1 µs is selected as best combination

Table.6.Main effect table

FACTOR/LEVEL 1 2 3 4 5

Max-Min Rank PULSE ON 33.67232 44.6762 38.39074 11.00392 1

PULSE OFF 39.16023 38.77993 38.79914 0.380294 3

workpiece 28.42613 28.5447 30.79568 28.97279 2.369547 2 Tool 26.95299 24.55785 22.5169 21.10954 21.60202

3.3 Analysis of variance

(26)

Table.7.ANOVA table

Factors

SS D.O.F Mean

square F

% Contribution F value table

A 0.6447 4 0.1612 9.372093 8.2989 3.01

B 1.0159 2 0.5079 29.52907 13.0767 3.63

AC 0.61 12 0.050 2.906977 7.8643 2.69

AB 0.15 8 0.019

1.104651 1.9338 2.59

AD 0.22 8 0.027 1.569767 2.8363 2.59

BC 0.31 6 0.052 3.023256 3.9966 2.74

CD 0.44 6 0.074 4.302326 5.6726 2.74

BD 0.56 4 0.14 8.139535 7.2197 3.01

ABC 0.68 24 0.028 1.627907 8.7667 2.24

ACD 0.64 24 0.027 1.569767 8.251 2.24

ABD 0.78 16 0.049 2.848837 10.056 2.364

BCD 0.39 12 0.032 1.860465 5.028 2.69

ABCD 1.23 48 0.026 1.511628 15.8575 2.152 Pure

Error

0.08606 5 0.0172

0.479109 Total

7.7686 179

4 Conclusions

EDM of ZrB2-SiC using five different electrodes is carried out at three levels of pulse on and off time. Six responses are considered for optimizing the parameters using desirability functional analysis using PSO. They ranked the tools as follows; Graphite, Titanium, Niobium, Tungsten, Tantalum. The machinability of workpieces increases with Vol % of SiC till it reaches 25% then it starts decreasing. Workpieces with 15 Vol % of SiC shows poor machinability. Pulse on time of 7 µs and off time of 1 µs is selected as best combination.ANOVA shows that tool and pulse on time are the significant factors.

References

[1] Allor R.L. and Jahanmir, S. (1996) `Current problems and future directions for ceramic machining’, American Ceramic Society Bulletein, Vol.75 No.7, pp. 40-43.

[2] Aman Aggarwal, Hari Singh, Pradeep Kumar and Manmohan Singh. (2008) ‘Optimization of multiple quality characteristics for CNC turning under cryogenic cutting environment using desirability function’, journal of materials processing technology, Vol.205, pp.42-50.

[3] Andreas. Nearchou, C. (2011) ‘Maximizing production rate and work load smoothing in assembly lines using particle swarm

W Ti Ta Nb GR 0.75 0.70 0.65 0.60 0.55 30 25 20 15 10 7 4 0.75 0.70 0.65 0.60 0.55 5 3 1 Tool Me a n

Vol % of SiC

Pulse on Time Pulse Off Time

Main Effects Plot for Global desirability(Weights by PSO)

Data Means

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[ 4 ] Aysun Sagbas. (2011) ‘Analysis and optimization of surface roughness in the ball burnishing process using response surface methodology and desirability function’, Advances in Engineering Software, Vol.42, pp.992-998.

[5] Chang H.,Lim T.V.(1993)’Evolution of circularity tolerance using Monte Carlo simulation for coordinate measuring machine’,International journal of production research vol.31,pp.2079-2086

[6] Cutler, R. A. (1992) `Engineering property of borides in ceramics and glasses’, In S. J. Schneider (Eds.), Engineered Materials Handbook, ASM International, Materials Park, Vol. 4, pp. 787–803.

[7] Eberhart, R.C. and Kennedy, J. (1995) ‘A new optimizer using particle swarm theory’, proceedings of the sixth International symposium on Micro machine and Human Science, Nagoya, Japan, pp.39-43.

[8] Goldberg, D E. (1990) Genetic algorithms in search, optimization & machine learning, Addison Wesley

[9] Hong Zhang, Heng Li and Tam, C.M. (2006) ‘Particle swarm optimization for resource-constrained project scheduling, International Journal of Project Management’, Vol.24, pp. 83–92.

[10] Indrajit Mukherjee and Pradip Kumar Ray. (2008) ‘Optimal process design of two-stage multiple responses grinding processes using desirability functions and metaheuristic technique’, Applied Software Computing, Vol.8, pp.402–421

[ 1 1 ] In-Jun Jeong and Kwang-Jae Kim. (2009) ‘An interactive desirability function method to multiresponse optimization’, European Journal of Operational Research, Vol.195, pp.412–426

[12] In-Jun Jeong and Kwang-Jae Kim. (2009) ‘An interactive desirability function method to multiresponse optimization’, European Journal of Operational Research, Vol.195, pp.412–426.

[13] Kennedy, J. and Eberhart, R.C. (1995) ‘Particle swarm optimization. Proceedings of IEEE International conference in Neural Networks’. Piscataway, NJ, IEEE service centre. pp. 1942-1948.

[14] Khoshkish, Ashtiani and Goreyshi. ‘Effects of Tool electrode material on electrical discharging machining process of hardened tool AISI D3’, Iran Conference of Manufacturing Engineering

[15] Klocke, F. (1997) `Modern approaches for the production of ceramic components’, Journal of European Ceramic Society, vol.17, pp.457–65.

[16] Mahdavinejad, R.A. (2009) ‘EDM process optimization via predicting a controller model’, International Scientific Journal published quarterly by the Association of Computational Materials Science and Surface Engineering, Vol.1 No.3, pp.161-167

[17] McGeough, J.A. (1988) Advanced methods of machining, Chapman & Hall, New York.

[18] Monteverde, F., Bellosi, A.and Luigi Scatteia. (2008) `Processing and properties of ultra-high temperature ceramics for space applications’, Materials Science and Engineering, vol. 485, pp. 415–21.

[19] Mu-Chen,C.Du-Ming, T. Hsien-Yu,T.(1999)’A stochastic optimization approach for roundness measurements’,Pattern Recognition Letters,Vol,pp.707–719

[20] Ritchie Mae gamut and armacheska mesa. (2008) ‘Particle Swarm Optimization - Tabu Search Approach to Constrained Engineering Optimization Problem’s’, World Scientific and Engineering Academy and Society transactions on mathematics, Vol. 7 No.11,pp.666-675.

[21] Schwartz, M.M. (1995) Engineering applications of ceramic materials, American Society of Metals, Metals Park, Ohio.

[22] Surajit Pal and Susanta Kumar Gauri. (2010) ‘Assessing effectiveness of the various performance metrics for multi-response optimization using multiple regression’, Computers & Industrial Engineering, Vol.59 pp. 976–85.

[23] Thakshila Wimalajeewa and Sudharman K. Jayaweera. (2007) ‘PSO for constrained optimization optimal power scheduling for correlated data fusion in wireless sensor networks’, the 18th Annual IEEE International Symposium on Personal, Indoor and Mobile Radio Communications (PIMRC’07).

[24] Upadhya, K. Yang, J M and Hoffman, W. P. (1997) `Materials for ultrahigh temperature structural applications’. American Ceramic Society Bulletin, vol.76 No.12, pp.51–56.

Figure

Table 2 Design of experiments
Table 4.Normalized value
Table.7.ANOVA table

References

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Among the transferosomal SUT in-situ gels, the perfringens entero- toxin based transferosomes showed the best ef fi cacy in intranasal permeation of the drug due to the great ability

Improvement of in vitro embryo production techniques of livestock species, particularly in cattle, reduced the costs of creating transgenic livestock via microinjection

An argument is made that depres- sion can be viewed as a modifiable inde- pendent risk factor for development of type 2 diabetes and for progression of complications from either type

Results: The data highlight three phases: a planning phase (ten meetings over half a year), a startup phase of trials of interdisciplinary everyday rehabilitation in practice