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Analysis of AC Breakdown Characteristics of Fly Ash Cenosphere/Epoxy Composite

  • Seo, Cheong-Won (School of Electrical and Electronic Engineering, Chungbuk National University, Korea.) ;
  • Kwon, Jung-Hun (School of Electrical and Electronic Engineering, Chungbuk National University, Korea.) ;
  • Cha, Young-Gwang (Vitzro Material R&D center.) ;
  • Park, Su-Min (Vitzro Material R&D center.) ;
  • Lim, Kee-Joe (Corresponding Author: School of Electrical and Electronic Engineering, Chungbuk National University, Korea)
  • Received : 2015.11.12
  • Accepted : 2016.05.11
  • Published : 2016.09.01

Abstract

Keywords

1. Introduction

The studies on the eco-friendly insulating materials have been carried out, as the restrictions on environmental contamination have increased due to global environmental pollution problems. However, it is not easy to change over to ecofriendly materials due to their lower performance compared to conventional insulating materials [1-4]. The fly ash cenosphere is one of byproducts of coal combustion at thermal power plants [5]. Cenospheres are typically hollow spherical particles with particle size of 10 ~ 600 μm, density of 0.3 ~ 0.6 g/cm3, and shell wall thickness of 2 ~ 10 μm, which are composed of alumina, silica, calcium oxide, etc. [6, 7]. Cenospheres have been used in a wide variety of products, including fire- and heat-protection devices, and automobile bodies. Due to their special characteristics, they are primarily used as lightweight fillers. Their physical properties, particularly their low density (due to their hollow structure) and low thermal conductivity, make them popular as fillers for polymer compositions for structural materials [8-11]. With the increasing demand for compact and ecofriendly electrical equipment, several researches on the effect of cenosphere in polymer composites have investigated. Sharma et al. investigated the dielectric properties in cenosphere/LDPE composites and found that the dielectric constant decreased as cenosphere content increased [12]. Manjunath et al. investigated the possibility of cenospheres as fillers for cable insulation material and found that the mechanical and thermal properties of cenosphere/PVC composite made it applicable to cable insulation material [10]. Deepthi et al. investigated the mechanical properties and thermal stability of surface treated cenosphere/HDPE composite and found improved mechanical and thermal properties [13]. However, studies on the electrical breakdown of cenosphere/epoxy composite are somewhat limited. In this study, the electrical breakdown strength and thermal properties of cenosphere/ epoxy composite are investigated. The breakdown strength is investigated in 25℃, 100℃, 125℃. The properties of the composite are also compared to those of silica/epoxy composite.

 

2. Experimental

2.1 Specimen preparation

Fig. 1 shows an optical microscope photograph of the cenosphere and silica used in this study. The properties of cenosphere and silica used as filler are listed in Table 1. The composite specimens were consisted of base epoxy resin (bisphenol-A), hardener (anhydrides), and filler as shown in Table 2 and Table 3. As shown in Table 3, this study has been performed on the five kinds of epoxy-based composites with different wt% contents of silica or cenosphere filler. The filler particles were dried at 150℃ for 1 hour before casting. Standard procedures for mixing, degassing, casting, and curing as recommended by epoxy manufacturers were used to prepare the samples as shown Fig. 2. The resin was mixed in a screw-type homogenizer at 2000 rpm for about 1 hour at 80℃. Thickness of the prepared specimen is about 1 mm.

Fig. 1.Optical microscope photograph of particle shape; (a) Cenosphere and (b) Silica powder

Table 1.Properties of cenosphere and silica

Table 2.Properties of base resin

Table 3.Component of specimen

Fig. 2.Sample preparation process

2.2 Electrical breakdown and permittivity measurement

The electrical breakdown strength under the AC field was measured according to IEC 60243-1. The voltage was increased at a rate of 1kV/s until breakdown occurred. Fig. 3 shows the circuit schematic diagram used to measure the breakdown strength, which consists of AC high-voltage generator and a couple of spherical electrodes with diameter of 10 mm. The breakdown strength was measured at 25℃, 100℃, and 125℃. More than ten specimens were tested under the same conditions. The scale parameters in Weibull distribution from test data are fixed as the breakdown strength. It is well known that the decreases of breakdown strength of solid polymeric insulators are severe above glass transition temperature. The temperatures of all specimen were in the range of 100 ~ 110℃, depending on a particular composition, as described later. The temperature ranges in breakdown test were selected by considering the glass transition temperature. The permittivity of specimens was measured by C & tan delta meter (Tettex 2818, Tettex Co.) at room temperature under 1 kV.

Fig. 3.Scheme of AC breakdown experimental setup

2.3 Thermal properties measurement

The coefficient of thermal linear expansion (CTE) and glass transition temperature (Tg) were measured using a Thermo-mechanical analyzer (TMA 2940, TA Instruments). A thermal scan of the specimen was run at a heating rate of 5℃/min in the temperature range from 25 to 200℃.

 

3. Results and discussion

3.1 Breakdown strength and permittivity

Fig. 4 shows the breakdown strength of each specimen at 25℃, 100℃, and 125℃. The breakdown strength of the specimens is decreased with increasing temperature. The results show a typical breakdown characteristic in high temperature region. The breakdown mechanism may be explained by thermal breakdown as considering the temperature dependency of breakdown strength and the time to breakdown (about 1sec.) together [14]. The decreasing rates of the breakdown strength with temperature above 100℃ are also depended on the glass transition temperature of samples as shown Fig. 4 and 7. The decreasing rates are smaller in the higher glass transition temperature of samples. These facts may be explained by the increases of heat generation by the dielectric relaxation α loss above glass transition temperature. Fig. 4 also shows that the breakdown strength is decreased with increasing the wt% contents of fillers. These results are similar to the tendency of breakdown in traditional insulating epoxy composites filled with inorganic micro-particles.

Fig. 4.AC breakdown strength of epoxy composite according to temperature

Fig. 5.Relative permittivity of epoxy composite

Fig. 6.Schematic of breakdown mechanism in resin: (a) hollow microsphere; (b) filled microsphere

Fig. 7.Tg and CTE of epoxy composite

The decreases of breakdown strength depending on wt% contents of cenosphere are smaller than those of silica. For specimens with the same contents of filler, cenosphere/epoxy composite has higher breakdown strength than that of silica/epoxy composite at the experimental temperature ranges. These facts may be explained in terms of details of breakdown process as follows. In case of cenosphere/epoxy composite, the gas discharge is firstly initiated inside hollow sphere of cenosphere particles by application of AC voltage, because the electrical stress is concentrated at the hollow part with lower permittivity. The gas discharges lead to the erosion of the microsphere walls followed by the breakdown of the whole material as shown Fig. 6(a) [16-17]. But the other hand, in case of silica/epoxy composite, the AC field leads to an increase in the electrical field in the epoxy resin between adjacent micro silica particles followed by a breakdown of the whole material as shown Fig. 6(b). Strauchs et al. reported that the electrical breakdown was initiated by gas discharges inside the hollow sphere in the hollow microsphere under the AC field [18]. Anderson et al. also, reported that breakdown strength of glass micro-balloon was higher than conventional gas discharge criterion to the voids, because the deceases of triggering free electrons might reduce the rate of field emission or field ionization events [19-20]. The performance of breakdown of cenosphere/epoxy composites is better than that of silica/epoxy composites.

The relative permittivity of samples is shown in Fig. 5. The permittivity of cenosphere/epoxy composite depending on the content of filler is lower than that of silica/epoxy composites. The results may be explained by the Maxwell-Garnett formula. It is needed to match permittivity for reducing the electric field concentration in practical hybrid insulation system. The lower permittivity insulators are also desirable in hybrid insulation system. In this standpoint, the cenosphere/epoxy shows better performance than silica/epoxy composite

3.2 Thermal properties

The measured results of the thermal properties are given in Fig. 7. The glass transition temperature, Tg of the specimen is increased as filler content is increased. This result may be explained by interaction between polymer matrix and surface of filled particles. Particles are caused to restrict the movement of the polymer chain in the polymer composite at increasing temperature, thus causing the Tg of the composite to increase. The coefficient of thermal linear expansion, CTE of the material is one of important properties. At practical application of epoxybased composite in power apparatus, a larger difference of CTE between metals and epoxy composite may cause to generate peeling off or imperfection at interface between two kinds of materials during heat cycle. An epoxy-based composite with smaller CTE is desired. The CTE of cenosphere/epoxy composite is smaller than that of silica/epoxy composite.

 

4. Conclusion

In this investigation, the breakdown strength, permittivity, glass transition temperature, and coefficient of thermal linear expansion of fly ash cenosphere/epoxy composites were measured and discussed. The performances of the composite are also compared to those of conventional silica/epoxy composites. The electrical breakdown strength of cenosphere/epoxy composite is higher than that of silica/epoxy in the experimental temperature range. The decreases of breakdown strength of cenosphere/epoxy composite above 100℃ are also smaller than those of silica/epoxy composite. These results may be explained by the details of breakdown process and glass transition temperature of specimen. As results of the Tg and CTE experiment, cenosphere/epoxy composite has similar or better thermo-mechanical performance than silica/epoxy composite. According to the above discussions, it is concluded that cenosphere can be considered as useful filler for epoxy-based insulation composite due to its electrical and thermo-mechanical properties. However, for practical application of cenosphere/epoxy composite as insulation in power equipment, further study is needed.

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