SlideShare a Scribd company logo
Optimization of process parameters on EDM of titanium alloy
Bhiksha Gugulothu
Department of Mechanical Engineering, Malla Reddy Engineering College (Autonomous), Maisammaguda, Secunderabad, Hyderabad, Telangana 500100, India
a r t i c l e i n f o
Article history:
Received 6 September 2019
Received in revised form 28 September
2019
Accepted 26 October 2019
Available online xxxx
Keywords:
Electrical discharge machining (EDM)
Titanium alloy (Ti-6Al-4V)
Discharge current
Pulse on time
Pulse off time
Dielectric fluid
a b s t r a c t
In this research paper, the effect of process parameters on electrical discharge machining (EDM) of Ti-6Al-
4V has been investigated. The process parameters were discharge current, pulse on time, pulse off time
and three types of dielectric fluid were used, they were deionized water, drinking water and mixed (25%
deionized water with mixing of 75% drinking water) has been used for machining of Ti-6Al-4V.
Experiments were carried out using Taguchi L27 (313
) Orthogonal Layout. The output process performance
was material removal rate (MRR) and surface roughness (Ra) was evaluated. Taguchi methodology were
used to optimize the process parameters. It has been observed from the analysis, drinking water as
dielectric fluid shows maximum material removal rate and reduced the surface roughness. The maximum
material removal rate of Ti-6Al-4V was 5.46 mm3
/min and minimum surface roughness was 2.53 mm.
Ó 2019 Elsevier Ltd. All rights reserved.
Selection and Peer-review under responsibility of the scientific committee of the First International
Conference on Recent Advances in Materials and Manufacturing 2019.
1. Introduction
EDM is termed as Electrical Discharge machine which is a
machining process of combination of electro-thermal energy
whereas the electrical energy is utilized to generate an electrical
spark [1]. The purpose of using EDM is to remove the material
and to shape the material [2] from the work piece as we required.
The thermal energy is generated due to the high electrical energy
[3] of the machine. Using this generated thermal energy and elec-
trical energy [4], the material is to be molten and the unwanted
portion of the material is to be removed [5] from the work piece.
The material used in the EDM must have the high strength temper-
ature resistant alloys [6] and also electrically conductive. In EDM,
the work piece and tool should be [7] electrically conductive. Both
of these materials [8] were immersed in dielectric medium [9] like
deionized water or kerosene [10]. The workpiece and tool [11] is
separated by some distance. After this some voltage [12] or poten-
tial difference is applied between the tool and workpiece [13].
Based on the gap between workpiece and tool and the amount of
potential difference [14] applied, the electric field is to be estab-
lished [15]. Normally, this setup is having the positive terminal
[16] and also the negative terminal. The tool is connected to the
negative terminal of the generator and also the work piece is con-
nected to the positive terminal of the generator. Because the elec-
tric field is induced between the tool and workpiece, [17] the free
electrons created in the tool are applied to electrostatic forces. If
the bonding energy between material and work piece of the elec-
trons [18] is less, then a quantity of electrons is emitted from the
tool and this emitted electron is known as cold emission. Then
the emitted cold electrons are moving towards the work piece
via the dielectric medium and get the velocity and energy. After
moving towards the workpiece, [19] there is a collision is induced
between the electrons and dielectric molecule and this collision
may cause the ionization of the dielectric medium which is based
on the bonding energy of the molecule and an electron. Due to col-
lision, more amounts of negative and positive ions are accelerated
[20]. This process will enhance the concentration of the ions and
electrons in the dielectric medium between work piece and tool
[21]. The matter presented in the channel is known as plasma
and the electrical resistance [22] of this is very low. Then unfortu-
nately, huge quantity of electrons and ions are to be flow from the
tool and the workpiece [23]. This movement of electrons is called
as avalanche motion of electrons. Such movement is to be create
an electrical spark and the amount of energy is to be dissipated
in the form of heat in spark. The high velocity electrons are fall
on the workpiece and ions on the tool. The kinetic energy of the
ions and electrons are impact with the surface of the workpiece
and tool respectively and to be converted into thermal energy or
heat flux. Such intense localized heat flux leads to extreme instan-
taneous confined rise in temperature and to material removal
which would be in excess of 10,000 C [24]. The schematic diagram
https://doi.org/10.1016/j.matpr.2019.10.150
2214-7853/Ó 2019 Elsevier Ltd. All rights reserved.
Selection and Peer-review under responsibility of the scientific committee of the First International Conference on Recent Advances in Materials and Manufacturing 2019.
E-mail address: bhikshamg@gmail.com
Materials Today: Proceedings xxx (xxxx) xxx
Contents lists available at ScienceDirect
Materials Today: Proceedings
journal homepage: www.elsevier.com/locate/matpr
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150
of the Electrical Discharge Machining used in this research is illus-
trated in Fig. 1.
2. Selection of the work piece material, electrode material and
types of dielectric fluid
The workpiece material employed in this study is Ti-6Al-4V.
Copper was used as an electrode material, drinking water, deion-
ized water and combinations (25% deionized water + 75% drinking
water) were used as dielectric fluids. The chemical composition
and properties of Ti-6Al-4V were shown in Tables 1 and 2, respec-
tively. The dielectric fluid characteristics of drinking water, drink-
ing water properties and deionized water properties were shown
in Tables 3–5. The experimental setup used for conducting actual
experiments is given in Fig. 2.
2.1. Identification of the important EDM process parameters
The most important EDM Process parameters identified were
discharge current, pulse on time. Pulse of time and dielectric fluids
were used.
2.2. Determination of the levels for the process parameters and their
working range
The working range of the selected process parameters under the
present study is given in Table 6.
2.3. Selection of orthogonal array
In the present analysis, an L27 (31 3
) orthogonal array is selected.
The selected orthogonal array is presented in Table 7.
2.4. The response measures (i.e. MRR and SR)
The EDM responses was measured in terms of MRR, SR.
The MRR can be calculated as the following formulae.
Fig. 1. Schematic diagram of EDM machine.
Table 1
Chemical Composition of Ti-6Al-4V.
Element C Al V N O Fe H Ti
% Max. 0.08 5.5–6.5 3.5–4.5 0.05 0.13 0.25 0.01 Balance
Table 2
Properties of Ti-6Al-4V.
Property Quantity
Hardness (HRC) 32–34
Melting point (°C) 1649
Density (g/cm3
) 4.5
Ultimate tensile strength (MPa) 897–1000
Thermal conductivity (W/m°K) 7.2
Specific heat (J/kg°K) 560
Mean coefficient of thermal expansion 100 °C/°C 08.6x10-6
Volume electrical resistivity (ohm-cm) 170
Elastic Modulus (GPa) 114
Table 3
Characteristics of Drinking water.
Characteristic Value
Appearance Clear and Colorless
Specific gravity at 30 °C 1.0004
Flash point (°C) –
Pour point (°C) 3
Viscosity at 38 °C (cst) 0.78
Copper corrosion Not worse than 1
Dielectric strength (KV/min) –
Table 4
Drinking water properties.
Total dissolved solids 98 mg/l
Total Suspended solids 10 mg/l
Total solids 120 mg/l
Dissolved O2 7.0 mg/l
Dissolved CO2 9 mg/l
Dissolved N2 0.01 mg/l
Chlorides 20.7 mg/l
Sulphate 32.0 mg/l
Total alkalinity 34.0 mg/l
pH 6.55
Total hardness 55.1 mg/l
Resistivity at 25 °C 4000 O/cm3
2 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150
MRRðmm3
=minÞ ¼
WWL gð Þ Â 1000
qðg=cm3Þ Â machining timeðminÞ
q = Density of work piece material
The SR is referred to the roughness or smoothness and it was
measured by surface roughness tester. MRR and SR was evaluated
for all the conditions and presented in Table 8.
MINITAB 17 software was used to prepare mean of response
tables and mean of S/N graphs for MRR and SR.
Taguchi method allows evaluation of individual parameters
effects independent of the other parameters for process parame-
ters optimization. The design parameters prominently affecting
the performance measures were determined by using analysis of
variance (ANOVA).
In Fig. 3. Where S/N ratio was larger to better was considered
for MRR. In Fig. 4 S/N ratio was lower to better was considered
for SR.
Fig. 4 shows the S/N response graph for surface roughness.
Significance of each parameter were found by using percentage
of contribution of each parameters in ANOVA table. High percent-
age contribution of process parameters on EDM has prominent
effect on the response. ANOVA was applied to find out the signifi-
cance of main factors and the percentage of contribution were used
to analysis the process parameter significantly effects on the MRR
and SR. The results of ANOVA for MRR and SR were presented in
Tables 9 and 10 respectively.
3. Results and discussions
3.1. Analysis of variance (ANOVA)
The ANOVA were performed to find the effect of process
parameters on various performance measures. Percentage of con-
tribution were used to determine the relative significance of var-
ious process parameters. From the ANOVA analysis shown in
Tables 9 and 10, it is observed that the dielectric fluid (A), dis-
charge current (B) pulse on time (C) were the most significant
factor affecting to MRR and SR. It was observed from the ANOVA
tables that discharge current (B) and pulse on time (C) have a
high percentage of contribution on various performance measures
as compared to pulse off time (D).
Table 5
Deionized water properties.
chloride 6.7 mg/l
Alkalinity Nil mg/l
pH 4.96
Total Hardness 22.4 mg/l
Resistivity at 25 °C 33333 O/cm3
Fig. 2. Experimental set up.
Table 6
Working range of the process parameters and their levels.
Parameters Levels
Dielectric fluid (A) Deionised
water
Drinking
water
Mixed (25% deionised
water + 75% drinking
water)
Discharge current (B) 10 15 20
Pulse on time (C) 25 45 65
Pulse off time (D) 24 36 48
Table 7
Experimental layout using an L27 (313
) OA.
Exp. No. Dielectric fluid (A) Discharge current (B) Pulse On Time (C) Pulse Off Time (D)
1 Deionized 10 25 24
2 Deionized 10 45 36
3 Deionized 10 65 48
4 Deionized 15 25 36
5 Deionized 15 45 48
6 Deionized 15 65 24
7 Deionized 20 25 48
8 Deionized 20 45 24
9 Deionized 20 65 36
10 Drinking 10 25 24
11 Drinking 10 45 36
12 Drinking 10 65 48
13 Drinking 15 25 36
14 Drinking 15 45 48
15 Drinking 15 65 24
16 Drinking 20 25 48
17 Drinking 20 45 24
18 Drinking 20 65 36
19 Mixed (25% deionised water + 75% drinking water) 10 25 24
20 Mixed (25% deionised water + 75% drinking water) 10 45 36
21 Mixed (25% deionised water + 75% drinking water) 10 65 48
22 Mixed (25% deionised water + 75% drinking water) 15 25 36
23 Mixed (25% deionised water + 75% drinking water) 15 45 48
24 Mixed (25% deionised water + 75% drinking water) 15 65 24
25 Mixed (25% deionised water + 75% drinking water) 20 25 48
26 Mixed (25% deionised water + 75% drinking water) 20 45 24
27 Mixed (25% deionised water + 75% drinking water) 20 65 36
B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx 3
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150
3.2. Effect of machining parameters on MRR
S/N graphs of MRR was presented in Fig. 3 and the ANOVA was
shown in Table 9. It is observed that for deionized water and drink-
ing water, the MRR increases and after that it decreases in the
mixed condition (25% deionized water + 75% drinking water) due
to decrease in thermal conductivity. It is also observed that, as
the current (I) increases from 10A to 20A, the MRR increases signif-
icantly. Discharge current controls the heat energy supplied for
metal removal, as the discharge current enhances, heat energy also
enhances. Thus the MRR increased from 10A current to 20A. The
discharge current is sharing 79% and it is the first significant factor.
The material removed is directly proportional to the amount of
energy supplied in this. Thus it is the most important factor as
far as sharing and importance is concerned. As the pulse on time
increases from 25 ms to 65 ms, the MRR also increases almost non-
linearly. Its contribution is 10%. Pulse off time is the least signifi-
cant factor and shows minimum contribution. Its contribution
towards MRR is 0.7%. It is observed that as the pulse off time
increases from 24 ms to 48 ms, the MRR is improved by very small
amount. At minimum pulse off time i.e. 24 ms, the dielectric fluid
gets less time to deionize and flush away the debris.
Table 8
Average results of MRR and SR.
Exp.
No.
Dielectric (A) Discharge current
(B)
Pulse On Time
(C)
Pulse Off Time
(D)
Average MRR (mm3
/
min)
Average SR (Ra)
mm
1 Deionized 10 25 24 1.6957 2.25
2 Deionized 10 45 36 2.1310 2.49
3 Deionized 10 65 48 2.46345 3.00
4 Deionized 15 25 36 2.5608 2.51
5 Deionized 15 45 48 4.0500 3.48
6 Deionized 15 65 24 3.2522 3.22
7 Deionized 20 25 48 3.4784 3.47
8 Deionized 20 45 24 4.4352 2.78
9 Deionized 20 65 36 4.5760 3.63
10 Drinking 10 25 24 2.2988 2.68
11 Drinking 10 45 36 2.4922 2.95
12 Drinking 10 65 48 2.6334 2.94
13 Drinking 15 25 36 3.7856 2.61
14 Drinking 15 45 48 4.1169 2.72
15 Drinking 15 65 24 4.0691 3.06
16 Drinking 20 25 48 4.2823 2.93
17 Drinking 20 45 24 4.5074 3.10
18 Drinking 20 65 36 5.4258 3.22
19 Mixed (25% deionised water + 75% drinking
water)
10 25 24 1.8950 2.91
20 Mixed (25% deionised water + 75% drinking
water)
10 45 36 2.2254 3.03
21 Mixed (25% deionised water + 75% drinking
water)
10 65 48 2.7238 3.18
22 Mixed (25% deionised water + 75% drinking
water)
15 25 36 3.0563 2.72
23 Mixed (25% deionised water + 75% drinking
water)
15 45 48 3.4300 2.89
24 Mixed (25% deionised water + 75% drinking
water)
15 65 24 3.6542 3.40
25 Mixed (25% deionised water + 75% drinking
water)
20 25 48 3.7967 3.12
26 Mixed (25% deionised water + 75% drinking
water)
20 45 24 4.5128 3.48
27 Mixed (25% deionised water + 75% drinking
water)
20 65 36 4.6655 3.49
Fig. 3. Influence of EDM parameters on S/N graph for material removal rate.
4 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150
3.3. Effect of machining parameters on SR
Fig. 4 presents the S/N graph and Table 10 presents ANOVA for
SR. It is observed that for the dielectric fluid as deionized water and
drinking water the SR decreases and after that it increases in the
mixed condition (25% deionized water + 75% drinking water)
which is due to lower thermal conductivity of water. Fig. 4 show
that as the discharge current increases from 10A to 20A, the SR
increases. As the discharge current increases the bombarding
impulsive force of electrons also increases. In case of negative
polarity, the bombardment of electrons takes place from work
piece to electrode. The SR is higher at 10A as the amount of mate-
rial deposited is less. When the discharge current is increased to
20A, the larger impulsive force produces deeper and greater craters
with more amount of material being deposited. Hence the surface
roughness is more. The contribution of dielectric fluid on the SR is
12% and it is the third largest. The contribution of discharge current
is 23% and its significance is the second highest. The material
removed by using the electrode is directly proportional to the
amount of energy supplied. Thus it is the most significant factor.
As the pulse on time increases from 25 ms to 65 ms, the SR also
increases. Its contribution is 33%. Pulse off time is the least signif-
icant factor and shows minimum contribution as far as SR is con-
cerned. Its contribution towards SR is 6%. It is observed that as
the pulse off time increases from 24 ms to 48 ms, the SR becomes
Fig. 4. Influence of EDM parameters on S/N graph for SR.
Table 9
ANOVA analysis for material removal rate (MRR).
Factor Sum square Degrees of freedom Mean sum of square Per. contribution (%)
(A) 10.78 2 5.39 5.58
(B) 153.72 2 76.86 79.69
(AXB) 0.67 4 0.16 0.34
C 19.33 2 9.66 10.02
AXC 2.45 4 0.61 1.27
D 1.45 2 0.72 0.75
AXD 1.02 4 0.25 0.53
Error 3.44 6 0.57 1.78
St 192.88 26 100
Table 10
ANOVA analysis for surface roughness (SR).
Parameter Sum square Degrees of freedom Mean sum of square Per.contribution
(A) 4.510561504 2 2.25 12.22
(B) 8.579256394 2 4.28 23.25
(AXB) 3.730956924 4 0.93 10.11
C 12.35823198 2 6.17 33.49
AXC 0.048866944 4 0.012 0.13
D 2.352982883 2 1.176 6.37
AXD 1.635441424 4 0.408 4.43
Error 3.678515757 6 0.613 9.97
St 36.89481381 26 100
Table 11
Optimum values of the machining performance evaluation parameters.
Parameters Optimum condition Predicted Optimum value
MRR (mm3
/min) A2B3C3D3 5.46
SR (mm) A2B1C1D2 2.53
B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx 5
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150
low. At minimum TON of 24 ms, the dielectric fluid employed rela-
tively less time to de-ionize and flush away the debris. Thus stabil-
ity of the machining process and SR is influenced the optimum
values of the machining performance evaluation parameters were
given in Table 11 and the optimum results were given in Table 12.
4. Conclusions
In this study, the influence of dielectric fluid i.e. deionized
water, drinking water and mixed (25% deionized water + 75%
drinking water), the process parameters and optimization of tita-
nium alloy (Ti-6Al-4V) in the die sinking EDM was studied by using
Taguchi method. From the results it was found that drinking water,
discharge current, pulse on time and pulse off time have been
found to play significant role in EDM operations. Also, it was found
that the optimal levels of the factors for MRR and SR are differing
from each other. From ANOVA, pulse on time is more significant
than discharge current for SR whereas discharge current is more
significant than pulse on time for MRR. On the other hand, interac-
tion between dielectric fluid and discharge current is also signifi-
cant in case of SR.
References
[1] Afzaal Ahmed et al., A comparative study on the modelling of EDM and hybrid
electrical discharge and arc machining considering latent heat and
temperature-dependent properties of Inconel 718, Int. J. Adv. Manuf.
Technol. 94 (5-8) (2018) 2729–2737.
[2] A.P. Tiwary, B.B. Pradhan, B. Bhattacharyya, Investigation on the effect of
dielectrics during micro-electro-discharge machining of Ti-6Al-4V, Int. J. Adv.
Manuf. Technol. 95 (1-4) (2018) 861–874.
[3] Robert M. Jones, Mechanics of Composite Materials, CRC Press, 2018.
[4] Khaled Bataineh, Ahmad Gharaibeh, Optimal design for sensible thermal
energy storage tank using natural solid materials for a parabolic trough power
plant, Solar Energy 171 (2018) 519–525.
[5] Nishant K. Singh, Anand Poras, Electrical discharge drilling of D3 die steel using
air assisted rotary tubular electrode, Mater. Today: Proceedings 5 (2) (2018)
4392–4401.
[6] Kurt Amplatz, et al. Multi-layer braided structures for occluding vascular
defects and for occluding fluid flow through portions of the vasculature of the
body, U.S. Patent No. 9,877,710. 30 Jan. 2018.
[7] Sagil James, Sharadkumar Kakadiya, Experimental study of machining of shape
memory alloys using dry micro electrical discharge machining process, ASME
2018 13th International Manufacturing Science and Engineering Conference.
American Society of Mechanical Engineers, 2018.
[8] Anthony Wright et al., The influence of a full-time, immersive simulation-
based clinical placement on physiotherapy student confidence during the
transition to clinical practice, Adv. Simulation 3 (1) (2018) 3.
[9] Welborn, Valerie Vaissier, Luis Ruiz Pestana, Teresa Head-Gordon,
Computational optimization of electric fields for better catalysis design, Nat.
Catal. (2018):
[10] Yang Yang, Kartik Ramaswamy, Kenneth S. Collins, Steven Lane, Gonzalo
Antonio Monroy, Lucy Chen, Yue Guo, and Eswaranand Venkatasubramanian,
Plasma reactor with electron beam of secondary electrons, U.S. Patent
Application 15/948,949, filed September 27, 2018.
[11] Qiu Mingbo, et al., Energy distribution in cool electrode of electrical discharge
machining based on wave-particle dualism, Mach. Sci. Technol. (2018) 1–15.
[12] Bin Kan et al., Fine-tuning the energy levels of a nonfullerene small-molecule
acceptor to achieve a high short-circuit current and a power conversion
efficiency over 12% in organic solar cells, Adv. Mater. 30 (3) (2018) 1704904.
[13] Simone Blayer et al., Accelerated process development and stockpile for MERS,
Lassa Nipah Viral Vaccine (2018).
[14] Detlef Loffhagen et al., Impact of hexamethyldisiloxane admixtures on the
discharge characteristics of a dielectric barrier discharge in argon for thin film
deposition, Contrib. Plasma Phys. 58 (5) (2018) 337–352.
[15] Singla, Anuj, A.P.S. Sethi, Inderpreet Singh Ahuja, An empirical examination of
critical barriers in transitions between technology push and demand pull
strategies in manufacturing organizations, World J. Sci. Technol. Sustainable
Development (2018).
[16] Hadad, Mohammadjafar, Lan Quang Bui, Cong Thanh Nguyen, Experimental
investigation of the effects of tool initial surface roughness on the electrical
discharge machining (EDM) performance, Int. J. Adv. Manuf. Technol. 95.5-8
(2018) 2093–2104.
[17] Tug˘rul Özel, Erol Zeren, Finite element modeling the influence of edge
roundness on the stress and temperature fields induced by high-speed
machining, Int. J. Adv. Manuf. Technol. 35 (3-4) (2007) 255–267.
[18] Abbas, Norliana Mohd, Darius G. Solomon, Md Fuad Bahari, A review on
current research trends in electrical discharge machining (EDM), Int. J. Mach.
Tools Manuf. 47.7-8 (2007) 1214–1228.
[19] Jin-Seong Park et al., Improvements in the device characteristics of amorphous
indium gallium zinc oxide thin-film transistors by Ar plasma treatment, Appl.
Phys. Lett. 90 (26) (2007) 262106.
[20] Rudolph A. Marcus, On the theory of oxidation-reduction reactions involving
electron transfer. I, J. Chem. Phys. 24 (5) (1956) 966–978.
[21] S.I. Tkachenko et al., Distribution of matter in the current-carrying plasma and
dense core of the discharge channel formed upon electrical wire explosion,
Plasma Phys. Rep. 35 (9) (2009) 734.
[22] R Lawrence Ives, Micro fabrication of high-frequency vacuum electron devices,
IEEE Trans. Plasma Sci. 32 (3) (2004) 1277–1291.
[23] K.S. Banker, A.D. Oza, R.B. Dave, Performance capabilities of EDM machining
using aluminum, brass and copper for AISI 304L material, Int. J. Appl. Innov.
Eng. Manage. 2 (2013) 186–191.
[24] L. Selvarajan, Narayanan, C. Sathiya, Jeyapaul et al. Optimization of EDM Hole
Drilling Parameters in Machining of MoSi2-SiC Intermetallic/Composites for
Improving Geometrical Tolerances, J. Adv. Manuf. Syst. (14) 4 (2015) 259–272,
World Scientific Publishing Company, DOI: 10.1142/S0219686715500171
Table 12
The optimum results.
Parameter Optimum
condition
Predicted
Optimum value
Experimental
values
MRR (mm3
/min) A2B3C3D3 5.46 5.90
SR (mm) A2B1C1D2 2.53 2.98
6 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx
Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/
10.1016/j.matpr.2019.10.150

More Related Content

PDF
N130305105111
PDF
A comparative study of PSO, GSA and SCA in parameters optimization of surface...
PDF
J1303057185
PDF
IRJET- Block Chain Technology-An Overview
PDF
Study and Analysis of Energy Utilization in Casting and Forging Industry
PDF
30120140506002
PDF
An Electrode Shape Configuration on the Performance of Die Sinking Electric D...
PDF
Optimization of Electrical Discharge Machining Process Parameters using SCM42...
N130305105111
A comparative study of PSO, GSA and SCA in parameters optimization of surface...
J1303057185
IRJET- Block Chain Technology-An Overview
Study and Analysis of Energy Utilization in Casting and Forging Industry
30120140506002
An Electrode Shape Configuration on the Performance of Die Sinking Electric D...
Optimization of Electrical Discharge Machining Process Parameters using SCM42...

What's hot (19)

PDF
Kill Cancer Tumour Cells using Radio-Frequency Ablation
PDF
L1303059097
PDF
Ijarcet vol-2-issue-7-2217-2222
PDF
Study of surface roughness for discontinuous
PDF
Thermal barrier Analysis in Diesel
PDF
Taguchi on mrr (C07)
PDF
Applying fuzzy ahp to evaluate the carbon foot print on the workplace in educ...
PDF
Optimization of “T”-Shaped Fins Geometry Using Constructal Theory and “FEA” C...
PDF
Stability criterion of periodic oscillations in a (6)
PDF
Significance and Need of Computational Analysis and Finite Element Modelling ...
PDF
The effect of magnetic field direction on thermoelectric and thermomagnetic c...
PDF
ESTIMATION AND ANALYSIS OF CYCLE EFFICIENCY FOR SHELL AND TUBE HEAT EXCHANGER...
PDF
Fem based modelling of the influence of thermophysical properties
PDF
IRJET- Experimental Analysis for Thermal Performance of Muffler Guard Hero Xt...
PDF
Optimization of Tool Wear: A Review
PDF
A compromise between the temperature difference and performance in a standing...
PDF
INVESTIGATION OF THE EFFECT OF CURRENT ON TENSILE STRENGTH AND NUGGET DIAMETE...
PDF
Artificial Neural Network based computing model for wind speed prediction: A ...
PDF
FORMULATION OF A FIELD DATA BASED MODEL TO ESTIMATE THE NOISE LEVEL IN A DIES...
Kill Cancer Tumour Cells using Radio-Frequency Ablation
L1303059097
Ijarcet vol-2-issue-7-2217-2222
Study of surface roughness for discontinuous
Thermal barrier Analysis in Diesel
Taguchi on mrr (C07)
Applying fuzzy ahp to evaluate the carbon foot print on the workplace in educ...
Optimization of “T”-Shaped Fins Geometry Using Constructal Theory and “FEA” C...
Stability criterion of periodic oscillations in a (6)
Significance and Need of Computational Analysis and Finite Element Modelling ...
The effect of magnetic field direction on thermoelectric and thermomagnetic c...
ESTIMATION AND ANALYSIS OF CYCLE EFFICIENCY FOR SHELL AND TUBE HEAT EXCHANGER...
Fem based modelling of the influence of thermophysical properties
IRJET- Experimental Analysis for Thermal Performance of Muffler Guard Hero Xt...
Optimization of Tool Wear: A Review
A compromise between the temperature difference and performance in a standing...
INVESTIGATION OF THE EFFECT OF CURRENT ON TENSILE STRENGTH AND NUGGET DIAMETE...
Artificial Neural Network based computing model for wind speed prediction: A ...
FORMULATION OF A FIELD DATA BASED MODEL TO ESTIMATE THE NOISE LEVEL IN A DIES...
Ad

Similar to Optimization of process parameters on edm of ti 6 al-4v- materials today paper (20)

PDF
20320140501003 2
PDF
IRJET- A Review Study of Thermal Electrical Model using ANSYS Software
PDF
Experimental Study of Static and Rotary Electrode on Electrical Discharge Mac...
PDF
Optimization of EDM Process Parameters using Response Surface Methodology for...
PDF
Optimization of MRR and SR by employing Taguchis and ANOVA method in EDM
PDF
MULTI RESPONSE OPTIMISATION OF DIE SINKER EDM FOR ALSIC COMPOSITE
PDF
Multi-Objective Optimization of EDM process parameters using Taguchi-Grey Rel...
PDF
IRJET-Experimental Analysis Optimization of Process Parameters of Wire EDM on...
PDF
Optimization of machining parameters of Electric Discharge Machining for 202 ...
PDF
Study of surface roughness for discontinuous ultrasonic vibration assisted el...
PDF
30120140507009 2
PDF
30120140507009
PDF
30120140507009 2
PDF
ELECTRO CHEMICAL MACHINING AND ELECTRICAL DISCHARGE MACHINING PROCESSES MICRO...
PDF
INFLUENCE OF CONTROL PARAMETERS ON MRR IN ELECTRICAL DISCHARGE MACHINING (EDM...
PDF
C1071521
PDF
International Journal of Engineering Research and Development
PDF
Optimization of edm for mrr of inconel 600 using taguchi method
PDF
Optimization of WEDM Process Parameters on Titanium Alloy Using Taguchi Method
PDF
Modeling of wedm process for complex shape using multilayer perceptron and re...
20320140501003 2
IRJET- A Review Study of Thermal Electrical Model using ANSYS Software
Experimental Study of Static and Rotary Electrode on Electrical Discharge Mac...
Optimization of EDM Process Parameters using Response Surface Methodology for...
Optimization of MRR and SR by employing Taguchis and ANOVA method in EDM
MULTI RESPONSE OPTIMISATION OF DIE SINKER EDM FOR ALSIC COMPOSITE
Multi-Objective Optimization of EDM process parameters using Taguchi-Grey Rel...
IRJET-Experimental Analysis Optimization of Process Parameters of Wire EDM on...
Optimization of machining parameters of Electric Discharge Machining for 202 ...
Study of surface roughness for discontinuous ultrasonic vibration assisted el...
30120140507009 2
30120140507009
30120140507009 2
ELECTRO CHEMICAL MACHINING AND ELECTRICAL DISCHARGE MACHINING PROCESSES MICRO...
INFLUENCE OF CONTROL PARAMETERS ON MRR IN ELECTRICAL DISCHARGE MACHINING (EDM...
C1071521
International Journal of Engineering Research and Development
Optimization of edm for mrr of inconel 600 using taguchi method
Optimization of WEDM Process Parameters on Titanium Alloy Using Taguchi Method
Modeling of wedm process for complex shape using multilayer perceptron and re...
Ad

Recently uploaded (20)

PDF
A comparative analysis of optical character recognition models for extracting...
PPTX
20250228 LYD VKU AI Blended-Learning.pptx
PDF
Building Integrated photovoltaic BIPV_UPV.pdf
PDF
Build a system with the filesystem maintained by OSTree @ COSCUP 2025
PDF
Unlocking AI with Model Context Protocol (MCP)
PPTX
Programs and apps: productivity, graphics, security and other tools
PPTX
Tartificialntelligence_presentation.pptx
PPTX
1. Introduction to Computer Programming.pptx
PDF
Mobile App Security Testing_ A Comprehensive Guide.pdf
PDF
MIND Revenue Release Quarter 2 2025 Press Release
PPTX
KOM of Painting work and Equipment Insulation REV00 update 25-dec.pptx
PDF
gpt5_lecture_notes_comprehensive_20250812015547.pdf
PDF
Encapsulation_ Review paper, used for researhc scholars
PDF
Assigned Numbers - 2025 - Bluetooth® Document
PDF
Getting Started with Data Integration: FME Form 101
PDF
Spectral efficient network and resource selection model in 5G networks
PPTX
SOPHOS-XG Firewall Administrator PPT.pptx
PDF
Encapsulation theory and applications.pdf
PDF
Per capita expenditure prediction using model stacking based on satellite ima...
PDF
Reach Out and Touch Someone: Haptics and Empathic Computing
A comparative analysis of optical character recognition models for extracting...
20250228 LYD VKU AI Blended-Learning.pptx
Building Integrated photovoltaic BIPV_UPV.pdf
Build a system with the filesystem maintained by OSTree @ COSCUP 2025
Unlocking AI with Model Context Protocol (MCP)
Programs and apps: productivity, graphics, security and other tools
Tartificialntelligence_presentation.pptx
1. Introduction to Computer Programming.pptx
Mobile App Security Testing_ A Comprehensive Guide.pdf
MIND Revenue Release Quarter 2 2025 Press Release
KOM of Painting work and Equipment Insulation REV00 update 25-dec.pptx
gpt5_lecture_notes_comprehensive_20250812015547.pdf
Encapsulation_ Review paper, used for researhc scholars
Assigned Numbers - 2025 - Bluetooth® Document
Getting Started with Data Integration: FME Form 101
Spectral efficient network and resource selection model in 5G networks
SOPHOS-XG Firewall Administrator PPT.pptx
Encapsulation theory and applications.pdf
Per capita expenditure prediction using model stacking based on satellite ima...
Reach Out and Touch Someone: Haptics and Empathic Computing

Optimization of process parameters on edm of ti 6 al-4v- materials today paper

  • 1. Optimization of process parameters on EDM of titanium alloy Bhiksha Gugulothu Department of Mechanical Engineering, Malla Reddy Engineering College (Autonomous), Maisammaguda, Secunderabad, Hyderabad, Telangana 500100, India a r t i c l e i n f o Article history: Received 6 September 2019 Received in revised form 28 September 2019 Accepted 26 October 2019 Available online xxxx Keywords: Electrical discharge machining (EDM) Titanium alloy (Ti-6Al-4V) Discharge current Pulse on time Pulse off time Dielectric fluid a b s t r a c t In this research paper, the effect of process parameters on electrical discharge machining (EDM) of Ti-6Al- 4V has been investigated. The process parameters were discharge current, pulse on time, pulse off time and three types of dielectric fluid were used, they were deionized water, drinking water and mixed (25% deionized water with mixing of 75% drinking water) has been used for machining of Ti-6Al-4V. Experiments were carried out using Taguchi L27 (313 ) Orthogonal Layout. The output process performance was material removal rate (MRR) and surface roughness (Ra) was evaluated. Taguchi methodology were used to optimize the process parameters. It has been observed from the analysis, drinking water as dielectric fluid shows maximum material removal rate and reduced the surface roughness. The maximum material removal rate of Ti-6Al-4V was 5.46 mm3 /min and minimum surface roughness was 2.53 mm. Ó 2019 Elsevier Ltd. All rights reserved. Selection and Peer-review under responsibility of the scientific committee of the First International Conference on Recent Advances in Materials and Manufacturing 2019. 1. Introduction EDM is termed as Electrical Discharge machine which is a machining process of combination of electro-thermal energy whereas the electrical energy is utilized to generate an electrical spark [1]. The purpose of using EDM is to remove the material and to shape the material [2] from the work piece as we required. The thermal energy is generated due to the high electrical energy [3] of the machine. Using this generated thermal energy and elec- trical energy [4], the material is to be molten and the unwanted portion of the material is to be removed [5] from the work piece. The material used in the EDM must have the high strength temper- ature resistant alloys [6] and also electrically conductive. In EDM, the work piece and tool should be [7] electrically conductive. Both of these materials [8] were immersed in dielectric medium [9] like deionized water or kerosene [10]. The workpiece and tool [11] is separated by some distance. After this some voltage [12] or poten- tial difference is applied between the tool and workpiece [13]. Based on the gap between workpiece and tool and the amount of potential difference [14] applied, the electric field is to be estab- lished [15]. Normally, this setup is having the positive terminal [16] and also the negative terminal. The tool is connected to the negative terminal of the generator and also the work piece is con- nected to the positive terminal of the generator. Because the elec- tric field is induced between the tool and workpiece, [17] the free electrons created in the tool are applied to electrostatic forces. If the bonding energy between material and work piece of the elec- trons [18] is less, then a quantity of electrons is emitted from the tool and this emitted electron is known as cold emission. Then the emitted cold electrons are moving towards the work piece via the dielectric medium and get the velocity and energy. After moving towards the workpiece, [19] there is a collision is induced between the electrons and dielectric molecule and this collision may cause the ionization of the dielectric medium which is based on the bonding energy of the molecule and an electron. Due to col- lision, more amounts of negative and positive ions are accelerated [20]. This process will enhance the concentration of the ions and electrons in the dielectric medium between work piece and tool [21]. The matter presented in the channel is known as plasma and the electrical resistance [22] of this is very low. Then unfortu- nately, huge quantity of electrons and ions are to be flow from the tool and the workpiece [23]. This movement of electrons is called as avalanche motion of electrons. Such movement is to be create an electrical spark and the amount of energy is to be dissipated in the form of heat in spark. The high velocity electrons are fall on the workpiece and ions on the tool. The kinetic energy of the ions and electrons are impact with the surface of the workpiece and tool respectively and to be converted into thermal energy or heat flux. Such intense localized heat flux leads to extreme instan- taneous confined rise in temperature and to material removal which would be in excess of 10,000 C [24]. The schematic diagram https://doi.org/10.1016/j.matpr.2019.10.150 2214-7853/Ó 2019 Elsevier Ltd. All rights reserved. Selection and Peer-review under responsibility of the scientific committee of the First International Conference on Recent Advances in Materials and Manufacturing 2019. E-mail address: bhikshamg@gmail.com Materials Today: Proceedings xxx (xxxx) xxx Contents lists available at ScienceDirect Materials Today: Proceedings journal homepage: www.elsevier.com/locate/matpr Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150
  • 2. of the Electrical Discharge Machining used in this research is illus- trated in Fig. 1. 2. Selection of the work piece material, electrode material and types of dielectric fluid The workpiece material employed in this study is Ti-6Al-4V. Copper was used as an electrode material, drinking water, deion- ized water and combinations (25% deionized water + 75% drinking water) were used as dielectric fluids. The chemical composition and properties of Ti-6Al-4V were shown in Tables 1 and 2, respec- tively. The dielectric fluid characteristics of drinking water, drink- ing water properties and deionized water properties were shown in Tables 3–5. The experimental setup used for conducting actual experiments is given in Fig. 2. 2.1. Identification of the important EDM process parameters The most important EDM Process parameters identified were discharge current, pulse on time. Pulse of time and dielectric fluids were used. 2.2. Determination of the levels for the process parameters and their working range The working range of the selected process parameters under the present study is given in Table 6. 2.3. Selection of orthogonal array In the present analysis, an L27 (31 3 ) orthogonal array is selected. The selected orthogonal array is presented in Table 7. 2.4. The response measures (i.e. MRR and SR) The EDM responses was measured in terms of MRR, SR. The MRR can be calculated as the following formulae. Fig. 1. Schematic diagram of EDM machine. Table 1 Chemical Composition of Ti-6Al-4V. Element C Al V N O Fe H Ti % Max. 0.08 5.5–6.5 3.5–4.5 0.05 0.13 0.25 0.01 Balance Table 2 Properties of Ti-6Al-4V. Property Quantity Hardness (HRC) 32–34 Melting point (°C) 1649 Density (g/cm3 ) 4.5 Ultimate tensile strength (MPa) 897–1000 Thermal conductivity (W/m°K) 7.2 Specific heat (J/kg°K) 560 Mean coefficient of thermal expansion 100 °C/°C 08.6x10-6 Volume electrical resistivity (ohm-cm) 170 Elastic Modulus (GPa) 114 Table 3 Characteristics of Drinking water. Characteristic Value Appearance Clear and Colorless Specific gravity at 30 °C 1.0004 Flash point (°C) – Pour point (°C) 3 Viscosity at 38 °C (cst) 0.78 Copper corrosion Not worse than 1 Dielectric strength (KV/min) – Table 4 Drinking water properties. Total dissolved solids 98 mg/l Total Suspended solids 10 mg/l Total solids 120 mg/l Dissolved O2 7.0 mg/l Dissolved CO2 9 mg/l Dissolved N2 0.01 mg/l Chlorides 20.7 mg/l Sulphate 32.0 mg/l Total alkalinity 34.0 mg/l pH 6.55 Total hardness 55.1 mg/l Resistivity at 25 °C 4000 O/cm3 2 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150
  • 3. MRRðmm3 =minÞ ¼ WWL gð Þ Â 1000 qðg=cm3Þ Â machining timeðminÞ q = Density of work piece material The SR is referred to the roughness or smoothness and it was measured by surface roughness tester. MRR and SR was evaluated for all the conditions and presented in Table 8. MINITAB 17 software was used to prepare mean of response tables and mean of S/N graphs for MRR and SR. Taguchi method allows evaluation of individual parameters effects independent of the other parameters for process parame- ters optimization. The design parameters prominently affecting the performance measures were determined by using analysis of variance (ANOVA). In Fig. 3. Where S/N ratio was larger to better was considered for MRR. In Fig. 4 S/N ratio was lower to better was considered for SR. Fig. 4 shows the S/N response graph for surface roughness. Significance of each parameter were found by using percentage of contribution of each parameters in ANOVA table. High percent- age contribution of process parameters on EDM has prominent effect on the response. ANOVA was applied to find out the signifi- cance of main factors and the percentage of contribution were used to analysis the process parameter significantly effects on the MRR and SR. The results of ANOVA for MRR and SR were presented in Tables 9 and 10 respectively. 3. Results and discussions 3.1. Analysis of variance (ANOVA) The ANOVA were performed to find the effect of process parameters on various performance measures. Percentage of con- tribution were used to determine the relative significance of var- ious process parameters. From the ANOVA analysis shown in Tables 9 and 10, it is observed that the dielectric fluid (A), dis- charge current (B) pulse on time (C) were the most significant factor affecting to MRR and SR. It was observed from the ANOVA tables that discharge current (B) and pulse on time (C) have a high percentage of contribution on various performance measures as compared to pulse off time (D). Table 5 Deionized water properties. chloride 6.7 mg/l Alkalinity Nil mg/l pH 4.96 Total Hardness 22.4 mg/l Resistivity at 25 °C 33333 O/cm3 Fig. 2. Experimental set up. Table 6 Working range of the process parameters and their levels. Parameters Levels Dielectric fluid (A) Deionised water Drinking water Mixed (25% deionised water + 75% drinking water) Discharge current (B) 10 15 20 Pulse on time (C) 25 45 65 Pulse off time (D) 24 36 48 Table 7 Experimental layout using an L27 (313 ) OA. Exp. No. Dielectric fluid (A) Discharge current (B) Pulse On Time (C) Pulse Off Time (D) 1 Deionized 10 25 24 2 Deionized 10 45 36 3 Deionized 10 65 48 4 Deionized 15 25 36 5 Deionized 15 45 48 6 Deionized 15 65 24 7 Deionized 20 25 48 8 Deionized 20 45 24 9 Deionized 20 65 36 10 Drinking 10 25 24 11 Drinking 10 45 36 12 Drinking 10 65 48 13 Drinking 15 25 36 14 Drinking 15 45 48 15 Drinking 15 65 24 16 Drinking 20 25 48 17 Drinking 20 45 24 18 Drinking 20 65 36 19 Mixed (25% deionised water + 75% drinking water) 10 25 24 20 Mixed (25% deionised water + 75% drinking water) 10 45 36 21 Mixed (25% deionised water + 75% drinking water) 10 65 48 22 Mixed (25% deionised water + 75% drinking water) 15 25 36 23 Mixed (25% deionised water + 75% drinking water) 15 45 48 24 Mixed (25% deionised water + 75% drinking water) 15 65 24 25 Mixed (25% deionised water + 75% drinking water) 20 25 48 26 Mixed (25% deionised water + 75% drinking water) 20 45 24 27 Mixed (25% deionised water + 75% drinking water) 20 65 36 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx 3 Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150
  • 4. 3.2. Effect of machining parameters on MRR S/N graphs of MRR was presented in Fig. 3 and the ANOVA was shown in Table 9. It is observed that for deionized water and drink- ing water, the MRR increases and after that it decreases in the mixed condition (25% deionized water + 75% drinking water) due to decrease in thermal conductivity. It is also observed that, as the current (I) increases from 10A to 20A, the MRR increases signif- icantly. Discharge current controls the heat energy supplied for metal removal, as the discharge current enhances, heat energy also enhances. Thus the MRR increased from 10A current to 20A. The discharge current is sharing 79% and it is the first significant factor. The material removed is directly proportional to the amount of energy supplied in this. Thus it is the most important factor as far as sharing and importance is concerned. As the pulse on time increases from 25 ms to 65 ms, the MRR also increases almost non- linearly. Its contribution is 10%. Pulse off time is the least signifi- cant factor and shows minimum contribution. Its contribution towards MRR is 0.7%. It is observed that as the pulse off time increases from 24 ms to 48 ms, the MRR is improved by very small amount. At minimum pulse off time i.e. 24 ms, the dielectric fluid gets less time to deionize and flush away the debris. Table 8 Average results of MRR and SR. Exp. No. Dielectric (A) Discharge current (B) Pulse On Time (C) Pulse Off Time (D) Average MRR (mm3 / min) Average SR (Ra) mm 1 Deionized 10 25 24 1.6957 2.25 2 Deionized 10 45 36 2.1310 2.49 3 Deionized 10 65 48 2.46345 3.00 4 Deionized 15 25 36 2.5608 2.51 5 Deionized 15 45 48 4.0500 3.48 6 Deionized 15 65 24 3.2522 3.22 7 Deionized 20 25 48 3.4784 3.47 8 Deionized 20 45 24 4.4352 2.78 9 Deionized 20 65 36 4.5760 3.63 10 Drinking 10 25 24 2.2988 2.68 11 Drinking 10 45 36 2.4922 2.95 12 Drinking 10 65 48 2.6334 2.94 13 Drinking 15 25 36 3.7856 2.61 14 Drinking 15 45 48 4.1169 2.72 15 Drinking 15 65 24 4.0691 3.06 16 Drinking 20 25 48 4.2823 2.93 17 Drinking 20 45 24 4.5074 3.10 18 Drinking 20 65 36 5.4258 3.22 19 Mixed (25% deionised water + 75% drinking water) 10 25 24 1.8950 2.91 20 Mixed (25% deionised water + 75% drinking water) 10 45 36 2.2254 3.03 21 Mixed (25% deionised water + 75% drinking water) 10 65 48 2.7238 3.18 22 Mixed (25% deionised water + 75% drinking water) 15 25 36 3.0563 2.72 23 Mixed (25% deionised water + 75% drinking water) 15 45 48 3.4300 2.89 24 Mixed (25% deionised water + 75% drinking water) 15 65 24 3.6542 3.40 25 Mixed (25% deionised water + 75% drinking water) 20 25 48 3.7967 3.12 26 Mixed (25% deionised water + 75% drinking water) 20 45 24 4.5128 3.48 27 Mixed (25% deionised water + 75% drinking water) 20 65 36 4.6655 3.49 Fig. 3. Influence of EDM parameters on S/N graph for material removal rate. 4 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150
  • 5. 3.3. Effect of machining parameters on SR Fig. 4 presents the S/N graph and Table 10 presents ANOVA for SR. It is observed that for the dielectric fluid as deionized water and drinking water the SR decreases and after that it increases in the mixed condition (25% deionized water + 75% drinking water) which is due to lower thermal conductivity of water. Fig. 4 show that as the discharge current increases from 10A to 20A, the SR increases. As the discharge current increases the bombarding impulsive force of electrons also increases. In case of negative polarity, the bombardment of electrons takes place from work piece to electrode. The SR is higher at 10A as the amount of mate- rial deposited is less. When the discharge current is increased to 20A, the larger impulsive force produces deeper and greater craters with more amount of material being deposited. Hence the surface roughness is more. The contribution of dielectric fluid on the SR is 12% and it is the third largest. The contribution of discharge current is 23% and its significance is the second highest. The material removed by using the electrode is directly proportional to the amount of energy supplied. Thus it is the most significant factor. As the pulse on time increases from 25 ms to 65 ms, the SR also increases. Its contribution is 33%. Pulse off time is the least signif- icant factor and shows minimum contribution as far as SR is con- cerned. Its contribution towards SR is 6%. It is observed that as the pulse off time increases from 24 ms to 48 ms, the SR becomes Fig. 4. Influence of EDM parameters on S/N graph for SR. Table 9 ANOVA analysis for material removal rate (MRR). Factor Sum square Degrees of freedom Mean sum of square Per. contribution (%) (A) 10.78 2 5.39 5.58 (B) 153.72 2 76.86 79.69 (AXB) 0.67 4 0.16 0.34 C 19.33 2 9.66 10.02 AXC 2.45 4 0.61 1.27 D 1.45 2 0.72 0.75 AXD 1.02 4 0.25 0.53 Error 3.44 6 0.57 1.78 St 192.88 26 100 Table 10 ANOVA analysis for surface roughness (SR). Parameter Sum square Degrees of freedom Mean sum of square Per.contribution (A) 4.510561504 2 2.25 12.22 (B) 8.579256394 2 4.28 23.25 (AXB) 3.730956924 4 0.93 10.11 C 12.35823198 2 6.17 33.49 AXC 0.048866944 4 0.012 0.13 D 2.352982883 2 1.176 6.37 AXD 1.635441424 4 0.408 4.43 Error 3.678515757 6 0.613 9.97 St 36.89481381 26 100 Table 11 Optimum values of the machining performance evaluation parameters. Parameters Optimum condition Predicted Optimum value MRR (mm3 /min) A2B3C3D3 5.46 SR (mm) A2B1C1D2 2.53 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx 5 Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150
  • 6. low. At minimum TON of 24 ms, the dielectric fluid employed rela- tively less time to de-ionize and flush away the debris. Thus stabil- ity of the machining process and SR is influenced the optimum values of the machining performance evaluation parameters were given in Table 11 and the optimum results were given in Table 12. 4. Conclusions In this study, the influence of dielectric fluid i.e. deionized water, drinking water and mixed (25% deionized water + 75% drinking water), the process parameters and optimization of tita- nium alloy (Ti-6Al-4V) in the die sinking EDM was studied by using Taguchi method. From the results it was found that drinking water, discharge current, pulse on time and pulse off time have been found to play significant role in EDM operations. Also, it was found that the optimal levels of the factors for MRR and SR are differing from each other. From ANOVA, pulse on time is more significant than discharge current for SR whereas discharge current is more significant than pulse on time for MRR. On the other hand, interac- tion between dielectric fluid and discharge current is also signifi- cant in case of SR. References [1] Afzaal Ahmed et al., A comparative study on the modelling of EDM and hybrid electrical discharge and arc machining considering latent heat and temperature-dependent properties of Inconel 718, Int. J. Adv. Manuf. Technol. 94 (5-8) (2018) 2729–2737. [2] A.P. Tiwary, B.B. Pradhan, B. Bhattacharyya, Investigation on the effect of dielectrics during micro-electro-discharge machining of Ti-6Al-4V, Int. J. Adv. Manuf. Technol. 95 (1-4) (2018) 861–874. [3] Robert M. Jones, Mechanics of Composite Materials, CRC Press, 2018. [4] Khaled Bataineh, Ahmad Gharaibeh, Optimal design for sensible thermal energy storage tank using natural solid materials for a parabolic trough power plant, Solar Energy 171 (2018) 519–525. [5] Nishant K. Singh, Anand Poras, Electrical discharge drilling of D3 die steel using air assisted rotary tubular electrode, Mater. Today: Proceedings 5 (2) (2018) 4392–4401. [6] Kurt Amplatz, et al. Multi-layer braided structures for occluding vascular defects and for occluding fluid flow through portions of the vasculature of the body, U.S. Patent No. 9,877,710. 30 Jan. 2018. [7] Sagil James, Sharadkumar Kakadiya, Experimental study of machining of shape memory alloys using dry micro electrical discharge machining process, ASME 2018 13th International Manufacturing Science and Engineering Conference. American Society of Mechanical Engineers, 2018. [8] Anthony Wright et al., The influence of a full-time, immersive simulation- based clinical placement on physiotherapy student confidence during the transition to clinical practice, Adv. Simulation 3 (1) (2018) 3. [9] Welborn, Valerie Vaissier, Luis Ruiz Pestana, Teresa Head-Gordon, Computational optimization of electric fields for better catalysis design, Nat. Catal. (2018): [10] Yang Yang, Kartik Ramaswamy, Kenneth S. Collins, Steven Lane, Gonzalo Antonio Monroy, Lucy Chen, Yue Guo, and Eswaranand Venkatasubramanian, Plasma reactor with electron beam of secondary electrons, U.S. Patent Application 15/948,949, filed September 27, 2018. [11] Qiu Mingbo, et al., Energy distribution in cool electrode of electrical discharge machining based on wave-particle dualism, Mach. Sci. Technol. (2018) 1–15. [12] Bin Kan et al., Fine-tuning the energy levels of a nonfullerene small-molecule acceptor to achieve a high short-circuit current and a power conversion efficiency over 12% in organic solar cells, Adv. Mater. 30 (3) (2018) 1704904. [13] Simone Blayer et al., Accelerated process development and stockpile for MERS, Lassa Nipah Viral Vaccine (2018). [14] Detlef Loffhagen et al., Impact of hexamethyldisiloxane admixtures on the discharge characteristics of a dielectric barrier discharge in argon for thin film deposition, Contrib. Plasma Phys. 58 (5) (2018) 337–352. [15] Singla, Anuj, A.P.S. Sethi, Inderpreet Singh Ahuja, An empirical examination of critical barriers in transitions between technology push and demand pull strategies in manufacturing organizations, World J. Sci. Technol. Sustainable Development (2018). [16] Hadad, Mohammadjafar, Lan Quang Bui, Cong Thanh Nguyen, Experimental investigation of the effects of tool initial surface roughness on the electrical discharge machining (EDM) performance, Int. J. Adv. Manuf. Technol. 95.5-8 (2018) 2093–2104. [17] Tug˘rul Özel, Erol Zeren, Finite element modeling the influence of edge roundness on the stress and temperature fields induced by high-speed machining, Int. J. Adv. Manuf. Technol. 35 (3-4) (2007) 255–267. [18] Abbas, Norliana Mohd, Darius G. Solomon, Md Fuad Bahari, A review on current research trends in electrical discharge machining (EDM), Int. J. Mach. Tools Manuf. 47.7-8 (2007) 1214–1228. [19] Jin-Seong Park et al., Improvements in the device characteristics of amorphous indium gallium zinc oxide thin-film transistors by Ar plasma treatment, Appl. Phys. Lett. 90 (26) (2007) 262106. [20] Rudolph A. Marcus, On the theory of oxidation-reduction reactions involving electron transfer. I, J. Chem. Phys. 24 (5) (1956) 966–978. [21] S.I. Tkachenko et al., Distribution of matter in the current-carrying plasma and dense core of the discharge channel formed upon electrical wire explosion, Plasma Phys. Rep. 35 (9) (2009) 734. [22] R Lawrence Ives, Micro fabrication of high-frequency vacuum electron devices, IEEE Trans. Plasma Sci. 32 (3) (2004) 1277–1291. [23] K.S. Banker, A.D. Oza, R.B. Dave, Performance capabilities of EDM machining using aluminum, brass and copper for AISI 304L material, Int. J. Appl. Innov. Eng. Manage. 2 (2013) 186–191. [24] L. Selvarajan, Narayanan, C. Sathiya, Jeyapaul et al. Optimization of EDM Hole Drilling Parameters in Machining of MoSi2-SiC Intermetallic/Composites for Improving Geometrical Tolerances, J. Adv. Manuf. Syst. (14) 4 (2015) 259–272, World Scientific Publishing Company, DOI: 10.1142/S0219686715500171 Table 12 The optimum results. Parameter Optimum condition Predicted Optimum value Experimental values MRR (mm3 /min) A2B3C3D3 5.46 5.90 SR (mm) A2B1C1D2 2.53 2.98 6 B. Gugulothu / Materials Today: Proceedings xxx (xxxx) xxx Please cite this article as: B. Gugulothu, Optimization of process parameters on EDM of titanium alloy, Materials Today: Proceedings, https://doi.org/ 10.1016/j.matpr.2019.10.150