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Advances in Tribology
Volume 2013 (2013), Article ID 324952, 10 pages
http://dx.doi.org/10.1155/2013/324952
Research Article

Role of Silicon Dioxide Filler on Mechanical and Dry Sliding Wear Behaviour of Glass-Epoxy Composites

1Department of Mechanical Engineering, Vidya Vikas Institute of Engineering and Technology, Mysore 570028, India
2Department of Mechanical Engineering, PES College of Engineering, Mandya 571401, India
3Department of Mechanical Engineering, The National Institute of Engineering, Mysore 570008, India

Received 25 May 2013; Accepted 22 August 2013

Academic Editor: Marimuthu Uthayakumar

Copyright © 2013 Naveed Anjum et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

The mechanical properties and dry sliding wear behaviour of glass fabric reinforced epoxy (G-E) composite with varying weight percentage of silicon dioxide (SiO2) filler have been studied in the present work. The influence of sliding distance, velocity, and applied normal load on dry sliding wear behaviour has been considered using Taguchi's L9 orthogonal array. Addition of SiO2 increased the density, hardness, flexural, and impact strengths of G-E composite. Results of dry sliding wear tests showed increasing wear volume with increase in sliding distance, load, and sliding velocity for G-E and SiO2 filled G-E composites. Taguchi's results indicate that the sliding distance played a significant role followed by applied load, sliding velocity, and SiO2 loading. Scanning electron micrographs of the worn surfaces of composite samples at different test parameters show smooth surface, microploughing, and fine grooves under low load and velocity. However, severe damage of matrix with debonding and fiber breakage was seen at high load and velocity especially in unfilled G-E composite.

1. Introduction

Present day industries are experiencing an escalating trend in the applications of particulate and fiber reinforced polymer matrix composites. Some of these applications related to mechanical engineering experience surface interactions with the surroundings as well as with the pairing element. Such applications call for better understanding of the tribological behaviour of the material under study.

Functional fillers are added to the thermoset matrix for improving its physical, mechanical and tribological properties. The modification of the mechanical, and tribological behavior of various polymers by the addition of filler materials has shown a great promise, and hence, it has been a subject of considerable interest. The filler materials include organic, inorganic, and metallic particulates in both macro- and nanolevels. Inclusion of solid lubricants such as graphite, molybdenum disulphide (MoS2), and polytetrafluoroethylene (PTFE) into polymers has proven effective in reducing the coefficient of friction but their influence on wear resistance is not distinctly clear [1].

Wear rate was reduced with the addition of PTFE into polymers such as polyphenylene sulfide (PPS), polyvinylchloride (PVC), polyarylate (PA), polyoxymethylene (POM), and polyamide (PA) [2]. Bolvari et al. [3] reported that the PTFE filled PPS reduced the wear rate of polymer remarkably. The role of PTFE filler in modifying the tribological behavior of fiber-reinforced composites has been studied and also reported that there is a considerable reduction in wear and the coefficient of friction of aramid fiber reinforced polyamide composites.

Suresha et al. [4] investigated the influence of inorganic fillers like silicon carbide (SiC) and graphite on the wear of the glass fabric reinforced epoxy (G-E) composites under dry sliding conditions. Higher wear volume loss has been recorded with increase in sliding velocity and the coefficients of friction showed an increasing trend with increase in load and sliding velocity. Siddhartha et al. [5] have investigated titanium dioxide (TiO2) reinforced epoxy functionally graded composites. They concluded that addition of TiO2 particles into epoxy has a dramatic effect on the flexural strength, tensile modulus, and impact strength in comparison to homogeneous composites. Shi et al. [6] studied the effects of filler crystal structure and shape on the friction and wear properties of potassium titanate whisker (K2Ti4O9 whisker, K2Ti6O13 whisker) and TiO2 particles filled PTFE composites. They reported that the friction coefficients of various PTFE based composites are weakly dependent on filler shape, but they are more strongly dependent on filler crystal structure. Basavarajappa et al. [7] investigated the tribological behavior of G-E composites with SiC and graphite particles as secondary fillers. A plan of experiments based on Taguchi’s design of experiments was adopted to acquire data in a controlled manner. An orthogonal array and analysis of variance (ANOVA) were employed to investigate the influence of process parameters on the wear behaviour of these composites. They concluded that the inclusion of SiC and graphite as secondary fillers increased the wear resistance of G-E composite. Akram et al. [8] reported the mechanical proper ties of G-E with fillers, namely, aluminum oxide (Al2O3), calcium carbonate (CaCO3), silicon dioxide (SiO2), and lead oxide (PbO), incorporated to the epoxy matrix to improve the mechanical properties. They concluded that the PbO as a filler material into G-E (52% epoxy + 13% PbO + 35% glass fiber) has better tensile properties as compared to composites. However, SiO2 filler addition (52% epoxy + 13% SiO2 + 35% glass fiber) showed better torsion and hardness properties. Further, unfilled G-E (65% epoxy + 35% glass fiber) composite showed good energy absorption capability as compared to filler filled G-E composites.

The whole phenomenon of adhesive wear is a complicated matter influenced by different factors such as the properties of the materials coming in contact with each other, and the service conditions also play their part in sliding wear. A comprehensive, overall understanding of adhesion is therefore called for, and there are indeed many studies on the subject [9]. However, most research has investigated only a single dimension of relationship between the different factors involved in wear loss. Such research is valuable, accurate, and detailed but fails to allow any overall evaluation of the cumulative effect of all the factors and their interactions to be extrapolated from them. In view of the above situation, a number of statistical methods have recently been implemented in wear studies [10]. A majority of research studied detailed experimental work, that is, the effect of one factor by keeping all other factors fixed; this approach is not advisable because in actual environment there will be combined effects of interacting factors influencing the adhesive wear. Hence, in this study an attempt is being made to study main factors effect.

To achieve this, a design of experiments based on the Taguchi method is adopted. This method is advocated by Taguchi and Konishi [11]. Taguchi’s technique uses special design of orthogonal arrays to study the entire parameter space with only a small number of experiments. Taguchi’s technique also helps in optimizing the critical parameters [12].

2. Materials and Methods

2.1. Materials

Matrix material selected for the present work is epoxy resin (LAPOX L-12) supplied by ATUL India Ltd. Woven glass fabrics made of 360 g/m2 E-glass fibers of diameter of about 12 µm have been used as the reinforcing material in all the composites. SiO2 particles having average particle size of about 10 µm are taken as filler material. The details of the properties of constituent materials and composition of different composite samples are shown in Tables 1 and 2, respectively. The amount of fillers in the composite was kept below 7.5 percentage by weight because an excessive amount of filler makes the molded composite specimen fragile and poor in interfacial adhesion between the laminae.

tab1
Table 1: Properties of epoxy, E-glass fiber, and silicon dioxide.
tab2
Table 2: Fabricated composites.

2.2. Specimen Preparation

The composite slabs were made by conventional hand-lay-up technique followed by compression molding technique as shown in Figure 1. The fabrication was done by mixing the measured amount of neat epoxy resin to a known amount of K6 hardener (Aromatic amines), a low viscosity room temperature curing liquid hardener was used in the present investigation. The epoxy to hardener ratio of 100 : 12 was maintained. Before layup, a polyester film was used as releasing agent to facilitate easy removal of the composite slab from the mould after curing. Plain weave woven fabrics were cut according to the required size (500 mm × 500 mm) as shown in Figure 1(a). Then, the woven fabric is dipped into the resin mix. A roller was used to smear the resin mix to impregnate the fabrics (Figure 1(b)). Sufficient care was taken during layup to ensure a uniform sample since fabrics have a tendency to clump and tangle together. Eight layers of fabrics were used to obtain laminates of thickness of about 3 mm. Figure 1(c) shows the basic process of hand lay-up technique. The process involves 12 h of impregnation and drying for 2 h at 100°C followed by compression moulding as shown in Figure 1(d) at a temperature of 120°C and pressure of 7.35 MPa. All the composite samples with and without particulate fillers were fabricated by the same technique. The fillers were mixed thoroughly in the epoxy resin before the glass fiber mats were stacked during layup for particulate filled composites. Specimens of suitable dimensions as per ASTM standards were cut for physical, mechanical, and tribological characterization.

324952.fig.001
Figure 1: Schematic representation of composite fabrication process.
2.3. Mechanical Characterization

Densities of the composites were determined by using a high precision Mettler, Toledo machine Model AX 205 by using Archimede’s principle. Shore hardness of composite samples was also measured using a Shore-D hardness tester (Time Group, Shore-D Durometer TH210). Four readings at different points were taken, and average values were reported.

Tensile testing of polymeric materials is often performed on flat, dog bone-shaped specimens with geometry according to ASTM D638-10. The mechanical properties of the fabricated microcomposites were studied using the universal testing machine (manufactured by Shimandsu and capacity 50 kN) with wedge grips operated by pneumatic nonshift wedge grips. The tensile test was performed at a cross-head speed of 5 mm/min, and strain (mm/mm) was calculated by dividing cross-head displacement (mm) by the gage length (mm). Five samples were tested for each composition of the composites. A three-point bending technique was adopted for flexural test as per ASTM-D790 standard for all composites. The impact strength was determined using izod impact tester pendulum type (PSI make, India) as per ASTM-D256 specification.

2.4. Tribological Characterization

Dry sliding wear tests were performed using pin-on-disk equipment, conforming to ASTM G99 standards with electronic data acquisition system. Sliding tests were performed at different operating parameters as shown in Table 3. Sliding tests were interrupted at regular intervals for measuring mass loss with an accuracy of 0.1 mg.

tab3
Table 3: Experimental parameters.

Mass loss was converted into volume loss for plotting the wear data using the computed density values based on the composition. Friction force was measured using strain gages mounted on the specimen-loading arm. A minimum of three tests were conducted for each set of operating conditions, in order to ensure consistent test results, within 8% variation.

2.5. Design of Experiments by the Taguchi Technique

The present study consists of 3 levels of 4 operating parameters as shown in Table 4. Based on these experimental conditions, Taguchi’s (34) orthogonal array is applied in the present study. Table 4 shows the combination of operating parameters selected as per orthogonal array. With four parameters and three levels for each, a full factorial experiment would require runs, whereas Taguchi’s factorial experiment approach reduces the requirement to nine trials.

tab4
Table 4: ( ) orthogonal arrays.

3. Results and Discussion

3.1. Influence of Fillers on Mechanical Properties
3.1.1. Density

The experimental values of density are illustrated in Figure 2. It can be observed that addition of SiO2 filler has increased the density of the G-E composites as compared to unfilled ones. This is due to the fact that addition of high density SiO2 into G-E increased the density of G-E composite.

324952.fig.002
Figure 2: Density of SiO2 filled G-E composites.
3.1.2. Hardness

The hardness values of unfilled and SiO2 filled G-E composites are shown in Figure 3. It can be seen that Shore-D hardness is higher for SiO2 filled G-E composites as compared to that of unfilled G-E samples. Further, the hardness is found to increase with the increase in filler loading. The increase in SiO2 loading results in an increase in brittleness of the composite and hence the hardness. Particulate filled G-E composites with sufficient surface hardness are resistant to in-service scratches that can compromise fatigue strength and lead to premature failure. Therefore, under an indentation loading, microparticles would undergo elastic rather than plastic deformation, as compared to unfilled G-E composites. The improvement in hardness with incorporation of filler can be explained as follows: under the action of a compressive force, the thermoset matrix phase and the brittle fiber and filler phase will be pressed together, touch each other, and offer resistance. Thus the interface can transfer load more effectively although the interfacial bond may be poor. This results in enhancement of hardness of SiO2 filled G-E composites.

324952.fig.003
Figure 3: Hardness of SiO2 filled G-E composites.
3.1.3. Tensile Strength

Tensile test data are illustrated in Figures 4 and 5. The test data indicate that there is marginal decrease in tensile strength of composites, with increase in SiO2 filler loading. Generally, the particulate fillers increase the stiffness and decrease the tensile strength depending on the type of filler used in the fabrication of composites. Some of the fillers showed improved tensile strength as well as tensile modulus of G-E composites. However, in the present case, the SiO2 filler reduced the tensile strength and increased the stiffness of the G-E composites.

324952.fig.004
Figure 4: Typical load displacement curves.
324952.fig.005
Figure 5: Tensile strength of SiO2 filled G-E composites.
3.1.4. Flexural Strength

The flexural test data are illustrated in Figure 6. It can be observed that the flexural strength values are increased with increase in SiO2 filler content in G-E composite. This can be attributed to improved adhesion among the various phases like glass fiber, SiO2 filler and epoxy matrix.

324952.fig.006
Figure 6: Flexural strength of SiO2 filled G-E composites.

3.1.5. Impact Strength

The impact strength of unfilled and SiO2 filled G-E composites is shown in Figure 7. The test results indicate that increasing trend in the impact strength SiO2 loading. This is due to uniform dispersion of SiO2 filler loading in G-E composite.

324952.fig.007
Figure 7: Impact strength of SiO2 filled G-E composites.
3.2. Fractographic Analysis

Figures 8(a), 8(b), 9(a), and 9(b) show the scanning electron micrographs of the fractured surfaces of G-E and SiO2 filled G-E composites, respectively.

324952.fig.008
Figure 8: SEM pictures of tensile fractured surfaces of unfilled G-E composites.
324952.fig.009
Figure 9: SEM pictures of tensile fractured surfaces of 7.5% SiO2 filled G-E, (a) longitudinal direction, (b) transverse direction.

The photomicrographs reveal that the fracture is due to delamination between the layers of the composite samples as well as due to fiber-pullout (Figure 8(a)). For G-E sample, the fracture is ductile-brittle and this can be due to the plastic deformation of the matrix after fiber-matrix debonding (Figure 8(b)). It is also evident from the clean fibers on fractured surfaces. Other important failure mechanisms of composites such as fiber-matrix debonding (marked “a”), fiber fracture (marked “b”), and cohesive resin fracture (marked “c”) can also be observed from the microphotograph (Figure 8(b)). Generally, matrix fracture is found to initiate at the surface of the fibers as indicated by the direction of river lines (marked by an arrow) and propagates into the resin on either side, where cracks extend from the surfaces of adjacent fibers simultaneously.

SEM characterization of the SiO2-G-E fractured surface shows (Figures 9(a) and 9(b) (better adherence of the fibers as well as SiO2 particles to the matrix (Figure 9(b)), which is a qualitative indication of greater interfacial strength. Dis-orientation of transverse fibers, fiber bridging, fibers pull out (Figure 9(a)), and normal fracture of longitudinal fibers, matrix debris, and matrix cracking (Figure 9(b)) can also be observed from the micrographs. The improvement reported in terms of mechanical properties of the composites tested is mainly due to the enhancement of adhesion or interfacial interactions among the fibers, matrix, and SiO2 filler.

3.3. Tribological Behaviour
3.3.1. Influence of Filler Content on Tribological Characteristics

G-E composites were prepared with SiO2 contents of 5 wt.% and 7.5 wt.%, and tribological behavior of the G-E composite was studied to assess the influence of SiO2 and compare with the unfilled G-E composites. Figure 10 shows the dry sliding wear volume loss of different composites under the test conditions used in the present study. It can be observed from the test results that the wear volume loss of the samples decreases with increase in filler loading.

324952.fig.0010
Figure 10: Wear volume of SiO2 filled G-E composites.

Specific wear rate of SiO2 filled G-E composite is studied with respect to SiO2 loading (Figure 11). At the normal load of 60 N and for sliding velocity of 3.14 m/s, the specific wear rate of G-E is  mm3/Nm. The specific wear rate decreases on addition of SiO2. It decreases to the values  mm3/Nm and  mm3/Nm for the SiO2 loading of 5 and 7.5 wt.%, respectively. The wear loss decreases significantly with addition of SiO2 as compared to unfilled G-E composites. The incorporation of hard particles like TiO2, SiO2, ZrO, SiC, and Al2O3 to polymer matrix has led to better enhancement in wear resistance [1315].

324952.fig.0011
Figure 11: Specific wear rate of SiO2 filled G-E composites.

The improvement in wear resistance is due to the presence of fine SiO2 particles (10 µm) uniformly dispersed in epoxy matrix. The SiO2 particles dispersed in the epoxy acts as a barrier and also prevent large scale of fragmentation of epoxy matrix.

This behavior is clearly observed from worn surface pictures (Figures 13 and 14). The wear of unfilled G-E seems to be slightly high with some material pullout. The asperities in the steel counter face easily remove the material from the soft polymer matrix by cutting action. The wear surface of SiO2 filled G-E is smooth and fine and no material pullout is noticed. The SiO2 particles also act as secondary reinforcement, bear the load, and reduces wear rate. Hardness contribution also plays a vital role in wear property improvement as reported elsewhere [1315].

The frictional force of SiO2 filled G-E composites is studied and compared with unfilled G-E, and the data are shown in Figure 12. The frictional force of unfilled G-E is 4 N and increases with increasing sliding distance. However, it increases on addition of SiO2 to the value of 4.2 N and 5.8 N for the SiO2 loading of 5 and 7.5 wt.%, respectively. The frictional force of unfilled G-E is far better compared to the SiO2 filled G-E composites. In microcomposites, the increase in frictional force with increase in SiO2 loading is due to bigger particle size and irregularity in shape. During sliding at contact surface, the frictional force generated might have pulled out SiO2 particles along with wear debris. These pulled out particles that remain on the surface of the sample might have acted as third body and avoid the direct contact of the sample with the counter surface resulting in increased frictional force.

324952.fig.0012
Figure 12: Frictional force of SiO2 filled G-E composites.
324952.fig.0013
Figure 13: SEM of worn surface of G-E material.
324952.fig.0014
Figure 14: SEM of worn surface of 7.5 SiO2 G-E Material.
3.3.2. Worn Surface Morphology

Figure 13 indicates fiber breakage, microcracks, disorientation of fibers, and higher damage to the matrix as compared to fibers. Figure 14 indicates higher damage to the matrix and less fiber breakages. Microcracking of the epoxy matrix and higher debris formation consisting of SiO2 and broken fibers can also be observed.

3.3.3. Effect of Load on Mass Loss of Composites

Figure 15 shows typical variation of wear loss with normal load. There is an increasing trend of wear loss with increase in load, for obvious reasons. Similar trend has been observed under different operating conditions.

324952.fig.0015
Figure 15: Mass loss of SiO2 filled G-E composites.
3.3.4. Specific Wear Rate

Figure 16 indicate decreasing trend of specific wear rate with increasing normal load. This can be attributed to flattening of asperities at higher loads, thereby increasing the contact area between sliding surfaces. Increased contact area causes decreased contact pressure, resulting in reduction in wear rate. Similar trend has been observed under different operating conditions.

324952.fig.0016
Figure 16: Specific wear of SiO2 filled G-E composites.
3.3.5. Influence of Sliding Velocity on Specific Wear Rate

Figure 17 represents the variation of specific wear rate with sliding velocity. Specific wear rate is observed to decrease with increase in sliding velocity, which can be attributed to the formation of transfer film on the counter body, due to increased temperature at higher sliding velocity. Formation of transfer film would result in decreased wear rate at higher sliding velocities. Similar trend has been observed under different operating conditions.

324952.fig.0017
Figure 17: Specific wear rate of SiO2 filled G-E composites.
3.4. Analysis of Wear by the Taguchi Technique

The parametric influence on dry sliding wear behaviour of the composite test specimen has been determined by adopting the Taguchi technique. Experiments have been conducted as per standard L9 orthogonal array, using 3 levels for each of 4 operational parameters, that is, filler content, load, sliding velocity, and sliding distance. The details of orthogonal array along with the output parameter, that is, mass loss, is as shown in Table 5.

tab5
Table 5: Standard orthogonal L9 array with output result.

The influence of different operating parameters on wear loss is assessed based on the S/N ratios, which indicated in Figure 18.

324952.fig.0018
Figure 18: Main effect plot for signal-to-noise ratio.

In order to corroborate the significance of operational parameters, that is, filler content, load, sliding velocity, and sliding distance, analysis of variance (ANOVA) is performed on experimental data. The ANOVA allows analyzing the influence of each variable on the total variance of the results. Table 6, shows the results of ANOVA for the wear of the test samples. This analysis was performed with a level of confidence of 95%. From Table 6 it is evident that sliding distance plays a significant role followed by load, velocity, and filler material percentage.

tab6
Table 6: Analysis of variance table for wear loss.

4. Conclusions

Increased usage of polymeric composites for tribological applications has necessitated investigation to study the behaviour of these materials under various operating conditions. The present investigation has been carried out to study the influence of SiO2 filler on the mechanical and dry sliding wear behaviour of G-E composites. The following conclusions can be drawn based on the results obtained from the investigations.(1)The addition of the SiO2 filler material has resulted in increased mechanical properties like density, hardness, flexural strength, and impact strength of the composite structure.(2)Results of sliding wear tests indicate increase in wear volume with increase in sliding distance, load, and sliding velocity.(3)The addition of SiO2 filler material is found to decrease the wear volume and specific wear rate of different composites. Increase in percentage of SiO2 filler has resulted in better sliding wear resistance due to better mechanical properties of the composite materials.(4)Taguchi’s test data indicate that sliding distance plays a significant role followed by load, sliding velocity, and filler content.(5)Microscopic analysis of the worn out surfaces of different composite samples at different operating parameters indicate, smooth surface and microploughing under lower loads and speeds, whereas severe damage of matrix with debonding and fiber breakage at higher loads and speeds.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

References

  1. K. Tanaka, Y. Uchiyama, and S. Toyooka, “The mechanism of wear of polytetrafluoroethylene,” Wear, vol. 23, no. 2, pp. 153–172, 1973. View at Scopus
  2. Y. Yamaguchi, Tribology of Plastic Materials, vol. 7 of Tribology Series, Elsevier, 1990.
  3. A. Bolvari, S. Glenn, R. Janssen, and C. Elliset, “Wear and friction of aramid fiber and PTFE filled composites,” Sealing Technology, vol. 47, pp. 7–9, 1997.
  4. B. Suresha, G. Chandramohan, J. Prakash, and V. Balusamy, “The role of fillers on friction and slide wear characteristics in glass-epoxy composite systems,” Journal of Minerals and Materials Characterization and Engineering, vol. 5, no. 1, pp. 87–101, 2006.
  5. Siddhartha, A. Patnaika, and A. D. Bhattb, “Mechanical and dry sliding wear characterization of epoxy-TiO2 particulate filled functionally graded composites materials using Taguchi design of experiment,” Materials & Design, vol. 32, no. 2, pp. 615–627, 2011. View at Publisher · View at Google Scholar
  6. Y. J. Shi, X. Feng, H. Y. Wang, C. Liu, and X. H. Lu, “Effects of filler crystal structure and shape on the tribological properties of PTFE composites,” Tribology International, vol. 40, no. 7, pp. 1195–1203, 2007. View at Publisher · View at Google Scholar · View at Scopus
  7. S. Basavarajappa, K. Arun, and J. Davim, “Effect of filler materials on dry sliding wear behavior of polymer matrix composites—a Taguchi approach,” Journal of Minerals and Materials Characterization and Engineering, vol. 8, no. 5, pp. 379–391, 2009.
  8. W. Akram, S. K. Chaturvedi, and S. M. Ali, “Comparative study of mechanical properties of e-glass/epoxy composite materials with Al2O3, CaCo3, SiO2 AND PBO fillers,” International Journal of Engineering Research & Technology, vol. 2, no. 7, pp. 1029–1034, 2013.
  9. B. Suresha and K. N. Shivakumar, “Investigations on mechanical and two-body abrasive wear behavior of carbon/glass fabric reinforced vinyl ester composites,” Materials & Design, vol. 30, no. 6, pp. 2056–2060, 2009. View at Publisher · View at Google Scholar
  10. K. R. Roy, A Premier on Taguchi Method, Van Nostrad Reinhold, New York, NY, USA, 1990.
  11. G. Taguchi and S. Konishi, Taguchi Methods Orthogonal Arrays and Linear Graphs, American Supplier Institute, Dearborn, Mich, USA, 1987.
  12. G. Taguchi, Introduction to Quality Engineering, Asian Productivity, Tokyo, Japan, 1990.
  13. B. Suresha, G. Chandramohan, and M. A. Jawahar, “Three-body abrasive wear behavior of filled epoxy composite systems,” Journal of Reinforced Plastics and Composites, vol. 28, pp. 225–233, 2009. View at Publisher · View at Google Scholar
  14. B. Suresha, G. Chandramohan, P. R. Sadananda Rao, S. Seetharamu, and P. S. Sampathkumar, “Influence of SiC filler on mechanical and tribological behaviour of glass fabric reinforced epoxy composite systems,” Journal of Reinforced Plastics and Composites, vol. 26, no. 6, pp. 565–578, 2007. View at Publisher · View at Google Scholar
  15. M. G. Veena, N. M. Renukappa, B. Suresha, and K. N. Shivakumar, “Tribological and electrical properties of silica-filled epoxy nanocomposites,” Polymer Composites, vol. 32, no. 12, pp. 2038–2050, 2011. View at Publisher · View at Google Scholar