- Open Access
- Total Downloads : 204
- Authors : M. R. Shivakumar, Dr. N. V. R. Naidu
- Paper ID : IJERTV3IS10761
- Volume & Issue : Volume 03, Issue 01 (January 2014)
- Published (First Online): 01-02-2014
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Studies on Tensile Response of Aluminium Alloy/Soda lime Glass Composites at Elevated Temperature through Taguchi’s Orthogonal Array Approach
M. R. Shivakumar1, Dr. N. V. R. Naidu2
1Assistant Professor, Department of Industrial Engineering and Management
2Professor, Department of Industrial Engineering and Management
M. S. Ramaiah Institute of Technology, Bangalore-560054, India.
Abstract
Al-Si eutectic based metal matrix composites with soda lime glass powder as reinforcement were produced using stir casting technique. Glass particles of average size 75, 125 and 210 micron, at three different levels (1.5, 3.0 and 4.5 wt.%) formed the reinforcement. Taguchis orthogonal array approach was used to design the experiments. Ultimate tensile strength (UTS) was evaluated at elevated temperatures for these composites and the significant factors that influence the UTS were identified. A regression analysis was employed to analyze the variation of UTS.
Keywords: Ultimate tensile strength, Composite materials, glass particles, Al-Si alloy, Taguchis orthogonal array.
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Introduction
Aluminium and its alloys have wide use in engineering applications, especially in the aerospace and automobile fields. Aluminium alloys inherently have high strength-to-weight ratio but suffer from inadequate yield strength, low wear resistance and poor thermal properties. As alloy development has almost reached saturation, the enhanced demands have to be met by newer class of materials such as metal matrix composites (MMCs). Tailoring of specific properties is achieved in MMCs by incorporating a controlled amount of ceramic particles or fibers in a base metal matrix. A number of material combinations have been attempted and documented in the literature. Applications of MMCs range from structural components to electronic packaging.
Substantial development work has been carried out on aluminium based MMCs with ceramics (silicon carbide, alumina, zirconia, silica and graphite) as the reinforcement [1]. However, the use of non- refractory materials such as glass powder as reinforcement in MMCs has not been attempted extensively [2]. Compared to the other reinforcing
materials in use, glass offers several advantages, in particular on the fronts of availability and cost. Likewise, several aluminium alloys have been investigated by previous workers as the matrix, but the most versatile cast alloy viz., Al-Si eutectic (LM6 alloy) has not been exploited so much. Therefore, there seems to be scope and immediate need to undertake an experimental investigation to produce LM6 based, glass powder reinforced MMCs and to characterize the MMCs thus produced for physical, mechanical thermal and other properties and micro- structural features.
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Experimental details
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Preparations of composites
LM6 aluminum alloy (eutectic alloy) is the most widely used aluminum cast alloy. Hence, this alloy was chosen for the present work as matrix and soda lime glass powder as the reinforcement material. Soda lime glass powder of required fineness was obtained after crushing and sieving commercially available soda lime glass sheets. The compositions of the base alloy LM6 and soda lime glass are shown in Table 1 and 2 respectively.
Table 1. Chemical composition of LM6 alloy
Element
Wt. %
Si
11.24
Cu
0.08
Mg
0.1
Fe
0.46
Mn
0.14
Ti
0.16
Ni
0.01
Zn
0.01
Lead
0.01
Al
Balance
Constituent
Wt. %
SiO2
71-73
Na2O2
14-15
CaO
8-10
MgO
1.5-3.5
Al2O3
0.5-1.5
Table 2. Chemical composition of commercial soda lime glass
work were prepared with the three control variables viz., weight fraction, particle size and pre-heat temperature of reinforcement, each at three levels listed in Table 3.
The L9 array of Taguchi for the test is shown in
Pre-treatment of reinforcement particles consists of cleaning the particles with alcohol and drying them before pre-heating. Pre-treatment and pre-heating of reinforcement improve the wetting a n d dispersion of particles in the matrix. In addition, a s m a l l amount of m a g n e s i u m (0.50%) was added to t h e m e l t to promote wetting of glass powder by the liquid alloy. Optimization of the process parameters and procedure was r e q u i r e d to produce composite materials with homogeneous distribution of reinforcement particles and to get composites w i t h minimum level of micro-structural defects. Earlier trials showed that the temperature of the matrix alloy before the introduction of glass powder is one of the important parameter [4]. Furthermore, the rate of introduction of the particles, pre-treatment of reinforcement and stirring parameters are also important to achieve good quality composites.
LM6 alloy ingots were charged into a graphite crucible and melted in a resistance heated furnace. When the melt reached 720oC, which is well above the melting temperature of LM6 alloy, about 10 gm of magnesium was added in order to improve wetting. This was followed by degassing with hexa- chloro-ethane.
Melt was positioned under the stirrer and stirred at a fixed stirring speed of 400 RPM to form a sufficiently large vortex. Pre-heated soda lime glass powder was added at the rate of 20 gm per min. to the vortex point. After adding the particles, impeller was driven for some more time till the temperature of the melt lowered to 640oC. Soon after, the melt mixture was poured into the metallic die pre-heated to 200oC.
LM6 alloy /soda lime glass particles composites with 1.5%, 3.0% and 4.5 % (weight fraction), and 75, 125 and 210 micron (average particle size) at different pre-heated temperatures (260oC, 380oC and 500oC) of soda lime glass powder were produced using above procedure.
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Design of experiments
Taguchis orthogonal array (OA) for three factors (each at three levels) was used in planning the experimentation. Based on the degrees of freedom on levels of factors, L9(34) OA was selected. LM6 alloy/soda lime glass particulate composites in this
Table 4. The influence of reinforcement parameters was evaluated using Signal-to-Noise ratio (SN ratio) analysis.
i
SN ratio for larger is the better quality characteristic = -10 log10 (1/n) ( 1/y 2)
(n is the number of observations and yi is the observed data).
Table 3.Levels of the reinforcement parameters
Control factor
Level
1
2
3
A: Weight Percent
1.5
3.0
4.5
B: particle size
(micron)
75
125
210
C: Pre-heat temperature
(oC)
260
380
500
Table 4.Taguchi orthogonal array L9(34)
Test Run
A: Weight percent
B: Particle size
(micron)
C: Pre-heat temperature
(oC)
1
1.5
75
260
2
1.5
125
380
3
1.5
210
500
4
3.0
75
380
5
3.0
125
500
6
3.0
210
260
7
4.5
75
500
8
4.5
125
260
9
4.5
210
380
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Assessment of UTS
INSTRON tensile testing machine was used to determine the UTS of the test specimens ( prepared as per ASTM standard Designation: E 8/E 8M 08) at elevated temperatures. The specimen was enclosed in the heating furnace and tested at the selected elevated temperature maintained by the furnace. Thermocouples and regulators control the temperature in the furnace. The machine is interfaced with computer having suitable software.
Figure 1. INSTRON Tensile test equipment
-
-
Results and Discussions
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Microstructures
Micro-structural examination of the composite was conducted to confirm uniform distribution and interface bonding of reinforced glass particles in the LM6 alloy matrix. Typical microstructures are shown in the Figures 2(a) and 2(b). It may be inferred that glass particles are uniformly distributed in the LM6 alloy matrix. The cast microstructure of the LM6 alloy is not significantly affected by the presence of the reinforcing glass phase. In particular, no casting defect such as porosity was found at the interface between the glass particle and the matrix. This indicates that the glass particles are almost perfectly
-
1.5%glass reinforcement (400X)
-
4.5% glass reinforcement (100X)
Figure 2.Microstructure of LM6 alloy/ glass composite
embedded inside the LM6 alloy matrix without any interface de-bonding. This is due to adequate wettability between glass particles and LM6 alloy matrix.
-
-
Tensile Behavior
Nine samples of LM6 alloy/soda lime glass particles composites were produced as per the design parameter combinations as per the L9 (34) orthogonal array. The experimental runs were done each with three replications. UTS values were assessed and SN ratio was calculated for every run. Tensile tests were carried out at three different test temperature conditions viz., 30oC, 100oC and 200oC respectively. The results were analyzed using the commercial software MINITAB14, specifically meant for design of experiment applications. The influence of reinforcement parameters on UTS was then evaluated using SN ratio response table. The ranking of the process parameters using SN ratios obtained for different parameter levels for UTS are shown in Tables 8, 9 and 10 respectively corresponding to test temperatures of 30oC, 100oC and 200oC.
-
Main Effect Plot
Figures 4, 5 and 6 show the main effects plots (data means) for SN ratio corresponding to the three test temperatures viz., 30oC, 100oC and 200oC. It may be seen that among all the factors, weight percent of glass powder is the most significant, followed by particle size. Pre-heat temperature of the glass particle has the least or almost no significant influence on UTS. The UTS corresponding to factor A (weight percent) is maximum at level 1 compared to levels 2 and 3. For factor B (particle size), at level 1, UTS is maximum. The analysis of the responses based on SN ratio leads to the conclusion that factor combination A1:B1 results in the maximum UTS. The optimum combination of reinforcement parameter levels were selected for the higher SN ratio values and the results are tabulated in Table 11. Results distinctly reveal that soda lime glass particle reinforcements do reduce the UTS significantly. It is also observed UTS of the MMCs decrease steadily at elevated temperatures.
Table 5. Experimental data with mean UTS and SN ratio (test temperature: 30oC)
Test Run
A
B
C
Observed values of
UTS (MPa)
Mean
UTS (MPa)
SN ratio
(dB)
1
1.5
75
260
195.30
159.10
172.30
175.567
44.7970
2
1.5
125
380
180.36
158.74
165.80
168.300
44.4854
3
1.5
210
500
167.91
151.19
168.34
162.480
44.1830
4
3.0
75
380
142.40
159.60
143.21
148.403
43.3935
5
3.0
125
500
150.01
135.12
142.21
142.447
43.0493
6
3.0
210
260
139.83
127.38
136.80
134.670
42.5646
7
4.5
75
500
108.77
132.92
120.85
120.847
41.5574
8
4.5
125
260
119.23
100.64
98.89
106.253
40.4362
9
4.5
210
380
97.87
80.90
91.87
90.213
39.0231
Table 6. Experimental data with mean UTS and SN ratio (test temperature: 100oC)
Test Run
A
B
C
Observed values of UTS (MPa)
Mean UTS (MPa)
SN ratio (dB)
1
1.5
75
260
149.24
148.33
150.10
149.223
43.4764
2
1.5
125
380
150.13
141.20
149.32
146.883
43.3294
3
1.5
210
500
149.86
142.56
137.67
143.363
43.1130
4
3.0
75
380
138.23
141.10
140.72
140.017
42.9225
5
3.0
125
500
152.55
120.46
142.16
138.390
42.6930
6
3.0
210
260
135.94
142.45
130.81
136.400
42.6805
7
4.5
75
500
132.23
127.78
127.13
129.047
42.2110
8 4.5
125
260
122.1
121.29
116.92
120.103
41.5863
9
4.5
210
380
118.10
116.42
114.51
116.343
41.3128
Table7. Experimental data with mean UTS and SN ratio (test temperature: 200oC)
Test Run
A
B
C
Observed values of UTS (MPa)
Mean UTS (MPa)
SN ratio (dB)
1
1.5
75
260
143.9
146.12
143.47
144.50
43.1963
2
1.5
125
380
138.16
139.53
138.19
138.63
42.8367
3
1.5
210
500
120.10
126.78
124.44
123.77
41.8460
4
3.0
75
380
126.12
124.94
125.10
125.39
41.9648
5
3.0
125
500
122.34
122.10
121.73
122.06
41.7312
6
3.0
210
260
125.28
122.54
114.35
120.72
41.6160
7
4.5
75
500
98.87
103.56
98.74
100.39
40.0274
8
4.5
125
260
88.76
102.45
91.56
94.26
39.4374
9
4.5
210
380
92.30
84.38
81.72
86.13
38.6692
Table 8. Response table SN ratios for UTS (Test temperature: 30oC)
Table 9. Response table SN ratios for UTS (Test temperature: 100oC)
Level
A
B
C
1
44.49
43.25
42.60
2
43.00
42.66
42.30
3
40.34
41.92
42.93
Delta
4.15
1.33
0.63
Rank
1
2
3
Level
A
B
C
1
43.31
42.87
42.58
2
42.77
42.54
42.52
3
41.70
42.37
42.67
Delta
1.60
0.50
0.15
Rank
1
2
3
Table 10. Response table SN ratios for UTS (Test temperature: 200oC)
Main Effects Plot (data means) for SN ratios
A B
44
43
Mean of SN ratios
42
41
40
Level
A
B
C
1
42.63
41.73
41.42
2
41.77
41.34
41.16
3
39.38
40.71
41.20
Delta
3.25
1.02
0.26
Rank
1
2
3
1.5
44
43
42
41
40
260
3.0
C
380
4.5
500
75 125
210
Signal-to-noise: Larger is better
Figure 3.Main effects plot (data mean) for SN ratios (Test temperature- 30oC)
43.5
43.0
Mean of SN ratios
42.5
42.0
41.5
Main Effects Plot (data means) for SN ratios
A B
Main Effects Plot (data means) for SN ratios
A B
43
42
Mean of SN ratios
41
40
39
43.5
43.0
42.5
42.0
41.5
1.5
260
3.0
C
380
4.5 75
500
125
210
1.5
43
42
41
40
39
3.0
C
4.5
75 125
210
Signal-to-noise: Larger is better
260
380
500
Figure 4.Main effects plot (data mean) for SN ratios (Test temperature- 100oC)
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Regression Analysis
The weight percent, particle size and temperature of the glass particles were considered in the development of mathematical models for UTS. The correlation between factors and UTS on LM6 alloy/soda lime glass composite was obtained through multiple linear regressions. The standard commercial statistical software package MINITAB14 was used in the model. Following are the regression equations thus developed.
Regression equation (Test temperature- 30oC):
UTS(MPa) = 216 – 21.0 A – 0.139 B + 0.0129 C
[R2 = 97.9%]Regression equation (Test temperature- 100oC):
UTS(MPa) = 165 – 8.22 A – 0.0528 B + 0.0070 C
[R2 = 94.3%]Regression equation (Test temperature- 200oC):
UTS(MPa) = 180 -14.0 A 0.0976 B 0.0184 C
[R2 = 94.3%]Signal-to-noise: Larger is better
Figure 5.Main effects plot (data mean) for SN ratios (Test temperature- 200oC)
In the multiple regression analysis, R2, the regression coefficient has values > 0.94 in all the models. This indicates that the fit of the experimental data is highly satisfactory. From the regression equations, it is observed that the weight percent of the glass particles plays prominent role in controlling UTS, followed by glass particle size. The negative value of the coefficient corresponding to the weight percent of the glass particles indicates that decrease in weight percent of the glass particles increases the UTS.
-
Confirmation Experiment
The experimental confirmation test is the final step in verifying the results drawn based on Taguchis design approach. Accordingly, a conformation experiment was conducted on LM6 alloy/soda lime glass composite prepared with optimal levels of the reinforce parameters (viz., A1:B1) obtained from the analysis. Tensile test was carried out at test temperatures of 30oC, 100oC and 200oC. Table 12 shows the results obtained from regression equation and the experimentation. The experimental value of the UTS compares well with the UTS calculated using the regression equation (percentage variation is only less than 1.38%).
Table 11. Optimum level of reinforcement parameters for maximum UTS
Sl. No.
Test Temperature (oC)
A:
Weight percent
B:
Particle size (micron)
C: Particle temperature (oC)
1
30
1.5
75
500
2
100
1.5
75
500
3
200
1.5
75
260
Table 12. Comparison of confirmation experiment and regression equation
Sl.
No.
Test Temperature (oC)
Experimental UTS (MPa)
Regression model UTS (MPa)
% Error
Observed values
Mean
1
30
180.45
172.34
173.56
175.75
177.57
-1.03
2
100
151.57
150.89
150.40
150.95
152.21
-0.83
3
200
145.67
143.23
145.78
144.89
146.89
-1.38
-
-
-
Conclusions
-
Mechanical mixing of the glass particles reinforcement into the LM6 alloy matrix is possible by stir casting techniques to produce MMCs.
-
Taguchis SN ratio approach adopted to analyze the effect of the reinforcement parameters, has lead to reliable results on UTS of the MMCs.
-
Soda lime glass particle reinforcement reduces UTS of the base alloy.
-
UTS of the LM6 alloy/glass composite reduces at the elevated test temperature compared to the values at room temperature.
-
Confirmation tests carried out to validate the accuracy of the analysis to justify the outcome of the investigation.
-
Regression equations developed in this work predict the UTS of the MMCs corresponding to varying reinforcement parameters with very reasonable accuracy.
Acknowledgement
The authors wish to thank Prof. S Seshan, Indian institute of Science, Bangalore for his constant help and encouragement. Financial support received from Visvesvaraya Technological University, Belgaum is gratefully acknowledged.
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