• Title/Summary/Keyword: charge-density method

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Investigation of Charge distribution in an Electric double layer capacitor (전기이중층 캐패시터 내의 전하분포 고찰)

  • Endrowednes, Kuantama;Jessi, Darma;Sung, Youl-Moon;Kim, Kwang-Tae
    • Proceedings of the Korean Institute of IIIuminating and Electrical Installation Engineers Conference
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    • 2008.10a
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    • pp.201-204
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    • 2008
  • The use of the pulsed electro acoustic (PEA) method allowed us to perform the direct observations of spatio-temporal charge distributions in Electric double layer capacitors (EDLCs) based on polarizable nanoporous carbonaceous electrode. The negative charge density became the maximum, about 205 C/$m^3$ at the region where was near to collector layer in EDLCs for case $V_{DC}$ = 2.5 V, while the positively charged density became the maximum, about 61.1 C/$m^3$ at the region where it was located around the cathode layer. The PEA measurement used here is a very useful method to quantitively investigates the spatio-temporal charge distribution in EDLCs.

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Analysis on Induced Current Density by Electric Field of Human under the 765 kV Transmission Line Considering Permittivity and Conductivity (유전율 및 도전율을 고려한 765kV 송전선하의 전계에 의한 인체내부 유도 전류밀도 해석)

  • 민석원;송기현;양광호;주문노
    • The Transactions of the Korean Institute of Electrical Engineers A
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    • v.53 no.8
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    • pp.461-465
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    • 2004
  • This paper analysed the induced current density by electric field of human body under the 765 kV transmission line considering permittivity and conductivity. As permittivity of human body is very high as $10^6$ at 60 Hz, special numerical computation technique in Surface Charge Method(SCM) for composite media with extremely different properties is applied to reduce calculation error of induced current density and electric field inside the human body. Calculation results show that the average of the induced current density inside human body is about 3mA/$m^2$, which is less than ICNIRP criterion (10mA/$m^2$).

Electrical Resistivity and Charge Density of Bismuth Telluride Doped with Erbium

  • Yeom, Tae-Ho
    • Journal of Magnetics
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    • v.10 no.4
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    • pp.149-151
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    • 2005
  • The electric properties of a single crystal bismuth telluride doped with a small concentration of Erbium, $Bi_{z-x}Er_xTe_3$ with x = 0.002, are investigated as a function of temperature. The resistivity was obtained by using the van der Pauw method. The measured electrical resistivity is 78 ${\mu}{\Omega}cm$ at 4.2 K. The charge density of $Bi_{z-x}Er_xTe_3$ is found to be $2{\times}10^{19}/cm^3$ at 4.2 K. It turns out that $Bi_{z-x}Er_xTe_3$ is a p-type semiconductor. It is discussed that the high mobility and less density support that $Bi_{z-x}Er_xTe_3$ is a potential sensor with high energy resolution. Comparison with an established material (i.e. Au:Er alloy) is also discussed.

A Study on A Spiral Charge for 3 Dimensional Charge Simulation Method (3차원 전하 중첩법용 나선 전하의 특성에 관한 연구)

  • 민석원;박은서;송기현
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.15 no.4
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    • pp.31-36
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    • 2001
  • This paper investigates characteristics of spiral charge for 3 dimensional charge simulation method to calculate electric fields of special conductor bundles with spiral rods in 765kV transmission line. We finds the simulating spiral charge as constant charge density give less potential calculation error than sinusoidal charge falsity. When a spiral rod is simulated as spiral charge, we also knows two spiral charge can simulate spiral rod best.

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Influence of Endurance tests on Space Charge Distribution of 160kV HVDC XLPE Cable

  • Liu, Yun-Peng;Liu, He-Chen
    • Journal of Electrical Engineering and Technology
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    • v.12 no.1
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    • pp.302-309
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    • 2017
  • The ageing of XLPE cable insulation will lead to the accelerating accumulation of space charge, which will greatly affect the safe operation of the HVDC cable. In order to investigate the influence of different ageing modes on the space charge distribution of the HVDC cable, thermal stressed, electrical stressed and electro-thermal stressed endurance tests were carried out on the XLPE peelings. The tested XLPE peelings were obtained from 160kV HVDC cable insulation. The endurance tests were carried at thermal stress of 363K, electrical stress of 20kV/mm DC and a combination of both. The Pulsed Electro-Acoustic (PEA) method was used to measure the space charge distribution of the samples. The influences of ageing on the trap energy distribution were analyzed based on the isothermal relaxation theory and the decay characteristics of the space charge. The results showed that thermal ageing would help to improve the crystalline morphologies of the XLPE at the early stage. The total amount of space charge decreased compared to the ones before thermal ageing. The long term of electrical stress would result in the cleavage of polymer molecule chains which would intensify the accumulation of space charge and increase the density and depth of electron traps. With a combination of electrical and thermal stress, the injection and migration of space charge were more significant. Besides, the depth and density of electron traps increased rapidly with the increase of endurance time.

Determination of Cation Charge Density in Mica-type Layered Aluminosilicates by N-alkylammonium Method (N-alkylammonium법에 의한 Mica형 층상 규산 알루미늄의 양이온 전하 밀도의 측정)

  • 최진호;박중철;김창은;이창교
    • Journal of the Korean Ceramic Society
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    • v.22 no.4
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    • pp.3-8
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    • 1985
  • The layer charge densities and interlayer C. E. C(cation exchange capacity) of ten mica-type aluminosilicates from Yong-il Pohang-prefacture were determined by n-alkylammonium method which is based on the mo-nolayer-doubelelayer structural transition of ni-alkylammonium ion in interlayer space of the layered silcates. The upper and lower limits of layer charge and interlyer C, E, C estimated were about 0.25~0.36 eq/(Si, $Al)_4$ O10 and 69~99meq/100g, respectively.

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Charge Accunmulation Characteristics in LDPE (저밀도 폴리에틸렌의 전하축적 특성)

  • ;;Tatsuo Takada
    • The Transactions of the Korean Institute of Electrical Engineers
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    • v.41 no.1
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    • pp.42-49
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    • 1992
  • Charge accumulation characteristics in low density polyethylene (LDPE) has been discussed based upon the internal charge distrubution measured by the pulsed electroacoustic technique. When the negative voltage with respect to earth is applied to the upper electrode, the negative charges near the anode and the positive charges near the cathode are accumulated in LDPE. Also, there was an asymmetric behavior of charge accumulation exhibiting that the charge accumulation near the anode keeps increasing whereas that near the cathode increases first and then decreases. Besides, under the present test conditions the internal charge distrubution becomes stabilized eventually. When the positive voltage with respect to earth is applied to the upper electrode, on the other hand, no such asymmetric charge accumulation was found. Therefore, it can be concluded that the heterocharges are accumulated at the surface region of LDPE subjected to high do voltages and that the begavior of charge accumulation depends on the polarity of do voltage and the position of charge accumulation.

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Charge pumping method를 이용한 MOSFET소자의 Trap분포 연구

  • Kim, Sun-Gon;Choe, Byeong-Deok
    • Proceedings of the Korean Vacuum Society Conference
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    • 2015.08a
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    • pp.216.2-216.2
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    • 2015
  • 본 연구에서는 charge pumping method에서 사용되는 변수들의 변화를 이용하여 hot carrier stress가 MOSFET소자의 oxide내에서의 trap 분포에 어떤 영향을 미치는지에 대해서 연구하였다. trap 분포를 확인하기 위해 스트레스 전 후에 reverse bias와 주파수에 따른 trap의 양을 측정 하였다. 스트레스 전과 후에 reverse bias와 주파수가 감소할수록 trap이 증가하는 모습이 나타났고, 스트레스 후에는 전과 비교하여 전반적으로 trap의 양이 증가하였다. 또한, 스트레스 전과 후에 MOSFET소자의 trap density는 center region에서 $2.89{\times}$10^10에서 $1.64{\times}$10^10으로 감소하였고, drain region에서 $2.83{\times}$10^10에서 $5.26{\times}$10^10으로 증가한 것을 확인하였다. 이는 reverse bias와 주파수의 가변에 따라서 trap의 공간적 분포를 측정할 수 있다는 것을 의미한다.

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A Study on the Development of the Rock Blastability Classification and the Methods for Minimizing Overbereak in Tunnel (터널 굴착면 여굴 최소화를 위한 발파암 분류(안) 및 공법 개발 연구)

  • 이태노;김동현;서영화
    • Proceedings of the Korean Geotechical Society Conference
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    • 2002.10a
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    • pp.303-310
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    • 2002
  • Overbreak occurred inevitably in a tunnel excavation, Is the main factor for increasing cost and time in tunnel projects. Furthermore the damage to the remained rock mass related to the overbreak can give rise to a serious safety problem in tunnels. As a rule of thumb, causes for the overbreak are inaccuracy in drilling, the wrong design of blasting and selection of explosives, and heterogeneity in rock mass. Specially, the geological features of the rock mass around periphery of an excavation are very important factors, so a lot of researches have been conducted to describe these phenomena. But the quantitative geological classification of the rock mass for the overbreak and the method for decreasing the amount of the overbreak have not been established. Besides, the technical improvement of the charge method is requested as explosives for the smooth blasting have not functioned efficiently. In this study, the working face around periphery of an excavation has been continuously sectionalized to 5∼6 parts, and the new Blastability Index for the overbreak based on 6 factors of RMD(Rock Mass Description), UCS(Uniaxial Compressive Strength) JPS(Joint Plane Spacing), JPO(Joint Plane Orientation), JPA(Joint Plane Aperture) and FM(Filling Material) is proposed to classify sections of the working face. On the basis of this classification, the distance between contour holes and the charging density are determined to minimize the overbreak. For controlling the charging density and improving the function of explosives, the New Deck Charge(N.D.C) method utilizing the deck charge method and detonation transmission in hole has been developed.

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Electric Field Analysis Using Three Dimensional Boundary Integral Equation Method (3차원 경계적분방정식법을 이용한 정전장 해석)

  • Kim, Jae-Hong;Kim, Dong-Hun;Park, Il-Han
    • Proceedings of the KIEE Conference
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    • 2000.07b
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    • pp.828-830
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    • 2000
  • This paper describes BIEM(Boundary Integral Equation Method) for computation of three dimensional electric field distribution and numerical method that an equivalent charge density is unknown variable. After computing numerically the surface charge distribution. the distribution of both potential and electric field are obtained. Finally, this numerical method is applied to the concentric sphere and the coaxial cylindrical model and numerical result is compared to the analytic solution.

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