• Title/Summary/Keyword: AC Electric Fields Dispersion

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A Study on Electric Field Dispersion Techniques of Epoxy-Nanocomposites for Application of High Voltage Power Apparatus (고전압 전력기기응용을 위한 에폭시-나노콤포지트의 전기장 분산기술연구)

  • Lee, Chang-Hoon;Kim, Hyo-Chul;Cho, Young-Haw;Kim, Hyun;Jo, Sung-Choe;Park, Jae-Jun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.97-97
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    • 2010
  • A new electric application method was developed to prepare epoxy/organoclay nanocomposite for the electrical insulation in the AC electric fields and it could be also used in the field of various viscous polymer/organoclay systems. The applied AC electric field condition was as follows; (1) inter-electrode distance: 40 mm, (2) application voltage: 3-11 kV, (3) frequency: 60~1,000 Hz, and (4) application time: 0~60 min. To characterize the epoxy/clay nanocomposite, WAXS and TEM analyses were confirmed. In order to explain how the organic modifier affects the exfoliation phenomena, a mechanism of the oscillating collision of the quaternary ammonium head was proposed and the effects of the AC voltage and frequency and the organoclay content were studied.

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AC Insulation Breakdown Properties of the EMNC to Application of Distribution Molded Transformer (배전용 몰드변압기 적용을 위한 EMNC의 교류절연파괴특성 연구)

  • Park, Jae-Jun
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.62 no.5
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    • pp.649-656
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    • 2013
  • A conventional epoxy-microsilica composite (EMC) and an epoxy-microsilica-nanosilicate composite (EMNC) were prepared in order to apply them to mold-type transformers, current transformers (CT) and potential transformers (PT). Nanosilicate was exfoliated in a epoxy resin using our electric field dispersion process and AC insulation breakdown strength at $30{\sim}150^{\circ}C$, glass transition temperature and viscoelasticity were studied. AC insulation breakdown strength of EMNC was higher than that of EMC and that value of EMNC was far higher at high temperature. Glass transition temperature and viscoelasticity property of EMNC was higher than those of EMC at high temperature. These results was due to the even dispersion of nanosilicates among the nanosilicas, which could be observed using transmission electron microscopy (TEM). That is, the nanosilicates interrupt the electron transfer and restrict the mobility of the epoxy chains.

Thermal, Mechanical, and Electrical Properties for EMNC_60 and EMNC_65 (EMNC_60과 EMNC_65에 대한 열적, 기계적, 전기적 특성 연구)

  • Park, Jae-Jun
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.25 no.11
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    • pp.895-901
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    • 2012
  • In order to application for high voltage heavy electric equipments, epoxy/microsilica 60 wt%/nano layered silicate composites (EMNC_60) and epoxy/microsilica 65 wt%/nano layered silicate composites (EMNC_65) respectively was synthesized by our electric field dispersion method and the result was obtained completely dispersion state. Thermal properties such as glass transition temperature (Tg) and thermal expansion coefficient, and DMA characteristics were studied, and mechanical properties such as tensile and flexural tests were performed. AC electrical insulation strength was also tested. The study on thermal property, EMNC_65 was better than EMNC_60 and mechanical, electrical properties much improved EMNC_60 compared with EMNC_65.

Electrical Properties for Micro-and-Nano- Mixture Composites using Electric Field Dispersion (전기장분산법을 이용한 나노와 마이크로 혼합된 콤포지트의 전기적 특성)

  • Cho, Dae-Lyoung;Kim, Jong-Ho;Park, Jae-Jun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.03b
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    • pp.32-32
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    • 2010
  • A epoxy/multilayered silicate nanocomposite was prepared by a new AC electric application method and micro silica particle was poured into the nanocomposite in order to prepare epoxy/micro-and-nano- mixed composites (EMNC). Electric insulation breakdown strength was measured in a sphere-sphere electrode system designed for the prevention of edge breakdown and the data were estimated by Weibull plot. As the exfoliated silicate nano-plates were homogeniously dispersed in the micro silica particles, the insulation property was higherd.

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Electric Field Dispersion Techniques of Epoxy-Layered Silicate Nanocomposites (에폭시-층상실리케이트 나노콤포지트의 전기장 분산기술)

  • Lee, Chang-Hoon;Lee, Jae-Yeong;Park, Jae-Jun
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.03b
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    • pp.30-30
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    • 2010
  • In order to prepare a epoxy/multilayered silicate nanocomposite, various mixing processes were tried and it was found that the silicate could not be fully exfoliated in the epoxy matrix through various mechanical mixing process. In this study, a new AC electric application method was developed to prepare epoxy/multilayered silicate nanocomposite. The exfoliation of the silicate was confirmed by XRD (X-Ray Diffraction) and TEM observation.

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Electric Circuits Modeling of Magnetoelectric Bulk Composites in Low Frequency (ME 소자의 저주파 등가회로 모델링)

  • Chung, Su-Tae;Ryu, Ji-Goo
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.26 no.7
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    • pp.515-521
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    • 2013
  • Magnetoelectric(ME) bulk composites with PZT-PNN-PZN/$Fe_2O_4$ were prepared by using a conventional ceramic methods and investigated on the ME voltage vs frequency of ac magnetic fields. We made the electric equivalent circuits by using the Maxwell-Wagner model and simulated the frequency dependence of ME voltage in low frequency region. ME devices were described by a series of two equivalent circuits of piezoelectric and magnetic, which have the relaxation time ${\tau}$ due to the interaction between ME device and load resistor. Equivalent circuit of piezoelectric material is independent of frequency. However ferrite magnetic materials have Debye absorption and dipolar dispersion, whose equivalent circuit is a function of frequency. Therefore we suggest the resistance in the equivalent circuit is proportion to $1+{\omega}^2{\tau}^2$ and the capacitance is in inverse proportion to $1+{\omega}^2{\tau}^2$ in the magnetic materials.