Development of EDM Tool for Fabrication of Microchannel Heat … · Electrical discharge machining...
Transcript of Development of EDM Tool for Fabrication of Microchannel Heat … · Electrical discharge machining...
IJIRST –International Journal for Innovative Research in Science & Technology| Volume 2 | Issue 09 | February 2016 ISSN (online): 2349-6010
All rights reserved by www.ijirst.org 63
Development of EDM Tool for Fabrication of
Microchannel Heat Sink and Optimization of
Single Response Parameter of EDM by Taguchi
Method
Mahesh B. Mohite Prof. V. P. Gaikwad
PG Scholar Professor
Department of Mechanical Engineering Department of Mechanical Engineering
D.K.T.E.’S TEI Ichalkaranji D.K.T.E.’S TEI Ichalkaranji
Abstract
Electrical discharge machining (EDM) is one of the advanced methods of machining. EDM is best option for extremely difficult
hard materials and complicated geometry materials which are very difficult to machine. The main aim of this work is to develop
electrode for natural leaf shape of microchannel heat sink to reduce fabrication time and investigated the single response
parameter optimization on EDM machine for microchannel heat sink of Aluminium 6061 .The performance of microchannel is
depend upon parameters of machining is selected during fabrication. The optimal set of process parameters such as current, pulse
ON and OFF time in Electrical Discharge Machining (EDM) process were used to study the response of single parameter such as
rate of material removal and surface roughness value on the Aluminium 6061 work piece material. The methodology based on
orthogonal array Taguchi’s analysis of variance (ANOVA) and signals to noise ratio (S/N Ratio) were employed to optimize the
performance characteristics like material removal rate and surface roughness of Aluminium 6061.
Keywords: Microchannel heat sink, EDM Electrode, Electrical Discharge Machining, Taguchi Method, ANNOVA,
Material Removal Rate, Surface Roughness, Orthogonal Array Signal-to-Noise ratio
_______________________________________________________________________________________________________
I. INTRODUCTION
There are different shapes like Square, triangular and trapezoidal shapes of microchannel are used for cooling purpose in several
scientific and commercial applications like Micro-Electro-Mechanical System (MEMS), Electronic cooling system, Biomedical
Engineering; Miniaturization and Biochemistry etc. In this work natural leaf shape pattern of microchannel heat sink is designed
and Electrode is developed for fabrication of designed microchannel on EDM. The main aim of this work is to develop electrode
for leaf shape microchannel to reduce fabrication time and study the single response parameter of EDM by using Taguchi
method. Many authors have presented their works on the Optimization of process parameters for various machining processes.
Raghuraman S et al. [1] have done EDM process optimization with multiple performance characteristics based on orthogonal
array with grey relational analysis for Mild Steel 2026 with copper electrode. R.Boopathi et al. [2] studied Influence of Process
Parameters for Electrical Discharge Machine Using Nano Particle and Brass Electrode. Response surface methodology has been
used by Tarun Modi et.al. [3] For Electrical Discharge Machining process with air hardening tool steel. Gaurav Raghav et.al [4]
investigated on Optimization of Material Removal Rate in Electric Discharge Machining Using Mild Steel.
II. EXPERIMENTAL DETAILS
Materials and Methods Used:
For this work Aluminium 6061 material is chosen for fabrication of microchannel heat sink. Aluminium 6061 has good ability to
absorb heat and have also good surface finish. Table 1 and Fig.1 material properties of electrode. Table - 1
Properties of Electrode Material
Properties Value
Melting point 1083ºC
Elastic modulus(E) 1.23×105 N/mm2
Poisson’s ratio 0.26
Density 8.9 gm./cm3
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 64
Fig. 1: Drawing of Leaf Shape Micro channel Heat Sink
Fig. 2: 3D model of Micro channel
Development of EDM Electrode:
With the help of designed drawing of leaf shape micro channel, the electrode is developed. The details of electrode is shown in
fig.3
Fig. 3: Details of developed tool
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 65
Fig. 4: Developed Copper electrode used for experiment
Machine is provided with fixed pulse voltage. The current, pulse ON time and pulse OFF time were selected from the range.
Table 2 shows the Machine specifications and Table 2 shows the working conditions and description of EDM. Table - 2
Machine specifications
Description Details
Supply voltage 75V
Discharge current 30A
Servo system Electromechanical
Power consumption 2kW
Model ELECTRONICA
Fig. 5: EDM machine
Table – 3
Working conditions and description of EDM
Working conditions Description
Work piece aluminium (6061)
Electrode Copper
Discharge current 2,3,5 amps
Pulse ON time 30,50,90 μs
Pulse OFF time 5,7,9 μs
Dielectric medium EDM oil
Fabrication of Leaf Shape Microchannel by Using Developed Electrode:
With the help of developed electrode the microchannel is fabricated on EDM machine. During fabrication of microchannel the
different parameter is studied and finding the response of single parameter of EDM. The microchannel is fabricated by using
developed tool is shown in fig.6
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 66
Fig. 6: Image of fabricated micro channel heat sink
Defining Levels of Critical Parameters:
In this work, three factors are selected. Levels indicate variation in the factors used for research work. Three levels of each
parameter are selected for experimentation. These three levels are as follows. Table - 4
Response parameters and control parameters with their levels
Response
Parameters
Material Removal Rate (mm3 /min.)
Surface Roughness (μm)
Control Parameters Levels
1 2 3
Discharge current (A) 2 3 5
Pulse ON time (μs) 30 50 90
Pulse OFF time (μs) 5 7 9
Design of Experiment:
Design of experiment is technique used for experimentation. There are various forms of DOE viz. Response surface method,
Taguchi method, and Factorial design methods are used for experimentation. Taguchi technique is used for this work. In
experimentation, according to Taguchi design of L9 array, total 9 trials are experimented.
Analysis of Samples by Simulation Method:
After creating design by using Taguchi technique all experimental trials are carried according to Taguchi experimentation plots,
samples are segregated for testing. This includes Surface roughness (Ra value in µm) using surface roughness tester as per the
tagging applied to the samples, and evaluating the MRR value by using equation 1.
Finding Optimal Solution:
After Experimentation carried, all the results obtained are plotted according to their trial numbers. Analysis of optimal solution is
based on requirement. There are three conditions at which we get optimal solution.
- Larger is better = -10log 10 (sum (1/Y2)/n)
- Nominal the better = -10log 10 (Y2)
- Smaller the better = -10log 10 (sum (Y2/N))
For this research work, Larger the better condition is used for response variable Material removal rate needs to maximize to
get good results. And Smaller the better condition is used for response variable surface roughness needs to minimize to get good
results.
Validation:
Validation of result is very important to know our obtained results are true or wrong Hence validation gives evidence behind
every experimental result. Validation can be either way. One way, is comparing both experimental and analytical result. Other
way is to set target value and experimenting other value to ensure not to cross targeted value.
Conclusion:
Conclusion is based on result obtained and validation part. Conclusion is what we have observed with results and graph obtained.
It tells about effect and contribution of input parameters on response value.
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 67
III. EXPERIMENTATION
Design of Experiments:
The experimental layout for the process parameters using the L9 orthogonal array was used in this study. This array consists of
three control parameters and three levels, as shown in table 3. In the Taguchi method, most all of the observed values are
calculated on the ‘higher the better’ and the ‘smaller the better’. Thus in this study, the observed values of Material Removal
Rate were set to maximum as desired values and surface roughness were set to minimum desired values. Table - 5
Design Matrix of L9 Orthogonal Array
Exp. No Parameters
A B C
1 1 1 1
2 1 2 2
3 1 3 3
4 2 1 2
5 2 2 3
6 2 3 1
7 3 1 3
8 3 2 1
9 3 3 2
Material Removal Rate:
The material removal rate of the work piece is the volume of the material removed per minute. It can be calculated using the
following relation.
MRR = (𝑊𝑖 − 𝑊𝑓) × 1000
(𝐷𝑤 × 𝑡) (1)
MRR – Material Removal Rate (mm3/min)
Wi - Initial weight of work piece (gm.)
Wf - Final weight of work piece (gm.)
Dw - Density of the work piece (gm. /cm3)
t - Period of trial (min)
Surface Roughness:
The parameter mostly used for general surface roughness is Ra. It measures average roughness by comparing all the peaks and
valleys to the mean line, and then averaging them all over the entire cut-off length. The surface roughness is measured by surface
roughness tester machine, which is shown in Fig.7
Fig. 7: Equipment for Surface Roughness Measurement
IV. EXPERIMENTAL RESULTS
Determination of Optimal Process Parameters for Material Removal Rate:
In this section, L9 orthogonal array is used to determine the optimal process parameters. The results are reported in S/N ratio and
ANOVA analysis. In Taguchi method, there are three performance characteristics such as higher-is-better, nominal-is-better and
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 68
lower-is-better. Here higher-is-better characteristics are used to find the optimal process parameter for material removal rate. The
experimental value of MRR and S/N ratio for MRR is listed in table Table - 6
Signal-to-Noise ratios for MRR
Exp.
No
Current
(A)
Pulse ON
Time (μs)
Pulse OFF
Time (μs)
MRR
(mm3/min) S/N RATIO FOR MRR (dB)
1 2 30 5 0.0105 -39.5762
2 2 50 7 0.0085 -41.4116
3 2 90 9 0.0082 -41.7237
4 3 30 7 0.0105 -39.5762
5 3 50 9 0.0102 -39.8279
6 3 90 5 0.0138 -37.2024
7 5 30 9 0.0105 -39.5762
8 5 50 5 0.0140 -37.0774
9 5 90 7 0.0105 -39.5762
Fig. 8: Graph 1 Main Effect Plot for SN ratio (MRR)
Above graph is obtained from table 6. Hence from above figure it is clear that, best combination obtained for MRR if Current
of level-3, T ON of level-2, and T OFF of level-1.
Analysis Means of S/N Ratio for Material Removal Rate:
As the experimental design is orthogonal, so it is possible to separate out the effect of each process parameter at different levels. Table - 7
Means of S/N ratio for MRR
Level Current T ON T OFF
1 -40.9038 -39.5762 -37.952
2 -38.8688 -39.4389 -40.188
3 -38.7432 -39.5007 -40.3759
Delta 2.1606 0.1373 2.429
Rank 1 2 3
Total Mean of S/N ratio -38.7113 dB
From table 6 the Means of S/N ratio for MRR is calculated and the process parameters are obtained such Current of level-3, T
ON of level-2, and T OFF of level-1.
Anova for Material Removal Rate:
The purpose of the ANOVA is to find the statistical significance of process parameters on the response shown in table
according to F value T OFF is most significant effect on MRR
Table - 8
ANNOVA for Material Removal Rate
Source DF Adj. SS Adj.MS F-Value P- Value % Contribution
current 2 0.0000127 0.0000064 23.73 0.040 40.32
321
-38
-39
-40
-41
321
321
-38
-39
-40
-41
A
Me
an
of
SN
ra
tio
s
B
C
Main Effects P lot for S N ratios
Data Means
S igna l-to-noise: Larger is better
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 69
T -ON 2 0.0000003
0.0000001
0.51
0.660
0.96
T -OFF 2 0.0000185
0.0000092
34.47
0.028
58.74
Error 2 0.0000005 0.0000003 0.02
Total 8 0.0000315
Determination of Optimal Process Parameters for Surface Roughness (Ra):
In this process, S/N ratio for surface roughness is obtained based on response of surface roughness, ‘Lower is better’ criteria are
chosen for surface roughness. Results obtained are plotted in tabular form, which is given in table 9. Table - 9
Signal-to-Noise ratios for Surface Roughness
TRIAL A B C SURFACE ROUGHNESS IN µm S/N RATIO FOR SR(DB)
1 1 1 1 1 0
2 1 2 2 1.01 -0.0864
3 1 3 3 0.955 0.3999
4 2 1 2 1.025 -0.2144
5 2 2 3 0.995 0.0435
6 2 3 1 1.04 -0.3406
7 3 1 3 1.085 -0.7085
8 3 2 1 1.09 -0.7485
9 3 3 2 1.1 -0.8278
Analysis Means of S/N Ratio for Surface Roughness:
Similarly, the S/N ratio for surface roughness is calculated. Here, lower-is-better characteristics are used to find the optimal
process parameter for surface roughness (Ra). From the means of response of S/N ratio for Ra from table, the optimal process
parameters are obtained such as Current of level-1, T- ON of level-3 and T- OFF of level-3. Table - 10
Means of S/N ratio for SR
Level Current T ON T OFF
1 0.1333 -0.3076 -0.3630
2 -0.1703 -0.7914 -0.3762
3 -0.7016 -0.3013 -0.1335
Delta 0.8349 0.4901 0.2427
Rank 1 2 3
Total Mean of S/N ratio -0.1004 dB
Fig. 9: Graph 2 Main Effect Plot for SN ratio (SR)
From the above graph, it is clear that, Surface Roughness with lower value is better results for good combination. Hence, from
above figure we conclude that, Current of level-1, T -ON of level-3 and T- OFF of level-3 is best combination result.
321
0.0
-0.2
-0.4
-0.6
-0.8
321
321
0.0
-0.2
-0.4
-0.6
-0.8
A
Me
an
of
SN
ra
tio
s
B
C
Main Effects P lot for S N ratios
Data Means
S igna l-to-noise: S m alle r is better
Development of EDM Tool for Fabrication of Microchannel Heat Sink and Optimization of Single Response Parameter of EDM by Taguchi Method (IJIRST/ Volume 2 / Issue 09/ 011)
All rights reserved by www.ijirst.org 70
ANOVA for Surface Roughness (Ra):
ANOVA for surface roughness (Ra) is listed in the table XII. From the table it is clearly found that Current with highest
contributing parameter for surface roughness. Therefore, Current is the most significant parameter for Ra followed by T -OFF
and T- ON. Table - 11
ANNOVA for Surface Roughness (Ra)
Source DF Adj. SS Adj.MS F-Value P- Value %Contribution
Current 2 0.0168167 0.0084083 23.47 0.041 88.59
T ON 2 0.0000500 0.0000250 0.07 0.935 0.26
T OFF 2 0.0021167 0.0010583 2.95 0.253 11.15
Error 2 0.0007167 0.0003583 0
Total 8 0.0189834
V. CONCLUSIONS
1) With the help of developed electrode the fabrication process of leaf shape micro channels is become very easy and time
consuming.
2) According to result obtained by parameter optimization of material removal rate is Current of level-3, T -ON of level-2, and
T -OFF of level-1, T -OFF is most significant effective parameter for MRR as compare to Current and T- ON.
3) According to responses of S/N ratio for Surface roughness Current of level-1, T -ON of level-3 and T-OFF of level-3.
Current is most significant effective parameter for surface roughness, followed by T-OFF and T-ON.
4) According to ANOVA table for MRR, T-OFF is most significant effective parameter for MRR.
5) According to ANOVA table for Surface roughness, Current is most significant effective parameter for surface roughness.
REFERENCES
[1] Raghuraman s, Thiruppathi k, Panneerselvam t, Santosh s, “Optimization of EDM parameters using Taguchi method and grey relational analysis for mild
steel is 2026”, international journal of innovative research in science, engineering and technology, vol. 2, issue 7, July 2013. [2] R.Boopathi and S.Sundaram , “Influence of Process Parameters for Electrical Discharge Machine Using Nano Particle and Brass Electrode”,
International Journal of Research in Advent Technology, Vol.2, No.11, November 2014.
[3] Tarun Modi, Shaileshbhai sanawada, Jignesh Patel, “A review paper on Optimization of process parameter of EDM for air hardening tool steel”, Tarun Modi et al Int. Journal of Engineering Research and Applications ISSN : 2248-9622, Vol. 5, Issue 1( Part 1), January 2015, pp.32-37.
[4] Gaurav Raghav, B.S. Kadam, Manjeet Kumar, “Optimization of Material Removal Rate in Electric Discharge Machining Using Mild Steel”, International
Journal of Emerging Science and Engineering (IJESE) ISSN: 2319–6378, Volume-1, Issue-7, May 2013.
[5] Dhirendra nath mishra ,Aarti Bhatia ,Vaibhav rana , “Study on Electro Discharge Machining (Edm)”, The International Journal Of Engineering And
Science (IJES), ISSN(e): 2319 – 1813 ISSN(p): 2319 – 1805. [6] Kuldeep Ojha, R. K. Garg,K. K. Singh, “MRR Improvement in Sinking Electrical Discharge Machining: A Review”, Journal of Minerals & Materials
Characterization & Engineering, Vol. 9, No.8, pp.709-739, 2010.
[7] Yan-Cherng Lin & Ho-Shiun Lee, “Optimization of machining parameters using magnetic-force assisted EDM based on gray relational analysis”, Int J Adv Manuf Technol (2009) 42:1052–1064.
[8] K. M. Patel & Pulak M. Pandey & P. Venkateswara Rao,“Optimisation of process parameters for multi-performance characteristics in EDM of Al2O3
ceramic composite”, Int J Adv Manuf Technol (2010) 47:1137–1147. [9] T. A. El-Taweel, “Multi-response optimization of EDM with Al–Cu–Si–TiC P/M composite electrode”, Int J Adv Manuf Technol (2009) 44:100–113.
[10] E. Aliakbari & H. Baseri,“Optimization of machining parameters in rotary EDM process by using the Taguchi method”, Int J Adv Manuf Technol (2012)
62:1041–1053. [11] Yusuf Keskin. H. Selc¸uk Halkacı Mevl ¨ut Kizil,“Anexperimental study for determination of the effects of machining parameters on surface roughness in
electrical discharge machining (EDM)”, Int J Adv Manuf Technol (2006) 28: 1118–1121.
[12] Ai-Huei Chiou & Chung-Chen Tsao & Chun-Yao Hsu, “A study of the machining characteristics of micro EDM milling and its improvement by electrode coating”, Int J Adv Manuf Technol.
[13] S. Singh, “Optimization of machining characteristics in electric discharge machining of 6061Al/Al2O3p/20P composites by grey relational analysis”, Int J
Adv Manuf Technol (2012) 63:1191–1202.
[14] C. Anbumeenakshi, M. R. Thansekhar, ( 2014 ) “Experimental Investigation of the Combined Effect of Coating and Header Combination in
Microchannel”, 2nd International Conference on Innovations in Automation and Mechatronics Engineering, 520 – 527. [15] Mushtaq Ismael Hasan, Hayder Mohammed Hasan, Ghassan Adnan Abid, (2014) “Study of the axial heat conduction in parallel flow” , Journal of King
Saud University – Engineering Sciences 26, 122–131.
[16] Deewakar Sharmaa, Parbar Pratham, Singha, Harry Gargb, ( 2013 ) “Comparative Study of Rectangular and Trapezoidal Microchannels Using Water and Liquid Metal”, Chemical, Civil and Mechanical Engineering Tracks of 3rd Nirma University International Conference, 791 – 796.
[17] Md. Jane Alam Khan, Md. Rakibul Hasan, Md. Arif Hasan Mamun, ( 2013 ) “Flow behavior and temperature distribution in micro-channels for constant
wall heat flux”, 5th BSME International Conference on Thermal Engineering, 350 – 356. [18] Rohit S.Khedka, Shriram S. Sonawane, Kailas L Wasewar, ( 2013 ) “Water to Nanofluids heat transfer in concentric tube heat exchanger: Experimental
study”, Chemical, Civil and Mechanical Engineering Tracks of 3rd Nirma University International Conference on Engineering, 318 – 323.
[19] Ahmed Mohammed Adhama, Normah Mohd-Ghazalib, Robiah Ahmadc, ( 2013 ), “Cooling of microchannel heat sinks with gaseous coolants”, 5th BSME International Conference on Thermal Engineering, 337 – 343.
[20] Baodong Shao, Lifeng Wang, Heming Cheng, Jianyun Li, (2012) “Optimization and Numerical Simulation of Multi-layer Microchannel Heat Sink”,
International Conference on Advances in Computational Modeling and Simulation, 928 – 933. [21] B. Sajadi, M.H. Saidi, (2012) “Pumping effect of bubble growth and collapse in microchannel”, Thermo-hydraulic modeling Sharif University of
Technology 19 (3), 431–436.