• 대한전기학회:학술대회논문집
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• 대한전기학회 1994년도 하계학술대회 논문집 C
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• pp.1428-1430
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• 1994

The accumulation of space charge in PE/PE/PE laminates was investigated using the low density polyethylenes having different melt indices from 0.25 to 45 g/10 min. Both heterocharge and homocharge accumulated in parent polyethylenes depend on the value of melt index. A general rule found in this study was that the heterocharge decreases as the melt index increases and finally the homocharge accumulates when the melt index is very high. Because of this reason, PE laminates showed different charge formation characteristics depending on melt index of polyethylene. Details of up to date results are described in the text.

• 한국전기전자재료학회논문지
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• 제11권8호
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• pp.587-595
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• 1998

Transient thermal analysis simulations are carried out using a modeling program to understand the human body model HBM ESD. The devices were simulated a one-dimensional device subjected to ESD stress by solving Poison's equation, the continuity equation, and heat flow equation. A ramp rise with peak ESD voltage during rise time is applied to the device under test and then discharged exponentially through the device. LDD and NMOS structures were studied to evaluate ESD performance, snap back voltages, device heating. Junction heating results in the necessity for increased electron concentration in the space charge region to carry the current by the ESD HBM circuit. The doping profile adihacent to junction determines the amount of charge density and magnitude of the electric field, potential drop, and device heating. Shallow slopes of LDD tend to collect the negative charge and higher potential drops and device heating.

• Journal of Korean Vacuum Science & Technology
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• 제2권1호
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• pp.13-19
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• 1998

We have calculated the electronic structure of impurity atoms in metal host by using the tight binding model in the recursion method. For a self-consistent calculation, we assumed that the effect of impurity introduction was localized only at the impurity site and its neighbours. We calculated the Madelung term by limiting the contribution to Vm of the charge perturbations to the first shell around the impurity with Evjen technique. The calculated local density of states and charge transfer values have been compared with the experimental values for a single impurity in metal host. We fund that d-reso-nance state came from the repulsive interaction between impurity d-state and host band, and the position of d-resonance state depended on the difference of valence electrons between the host and the impurity. the results also showed that the charge transfer value between an impurity and host metal was comparable to the ionicity difference between them.

• 한국안전학회지
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• 제18권3호
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• pp.54-59
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• 2003

The discharge energy by electrostatic discharge of the charged human body is calculated under the assumption that the stored charge is dissipated completely. However, it is well-known that the charge is slightly remained after electrostatic discharge. Therefore, The Rompe-Weisel model of the discharge analysis, which has somewhat more of a physical justification than the conventional energy equation, is proposed. It is proposed that the electrical conductivity of the arc should be proportional to the energy density transferred to it by Ohmic dissipation. For the electrostatic discharge energy analysis, the Rompe-Weisel model was compared by quasi static analysis. As a consequence, a study on a reliable energy evaluation based on simulation models during electrostatic discharge is carried out in this paper and is adopted to estimate the explosion hazards of flammable gases.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1990년도 하계학술대회 논문집
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• pp.459-461
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• 1990

Me performed an experiment about preionization electron number density of charge transfer type KrF excimer laser. At the total pressure of 1.8 and 2.2 atm with helium (He) buffer gas, the experimental range of the electron number density is 8-9 ${\times}$ 10 cm The distance between electrode and preionization pin is 15 mJ at charging voltage of 27kV,gas pressure of 2.2 atm,gas mixture of F /Kr/He = 0.3/396.7(%).

• 전기의세계
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• 제27권3호
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• pp.31-35
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• 1978

In this paper, in order to clarify the mature of traps in polymer, the thermally stimulated current (TSC) measurements were mad on high density polyethylene by changing the condition of the high-field treatment such as the strength of the field (Fe), the treatment time (te) and the heating rate (.betha.). In addition, the TSC measured from the HDPE was compared with that from LDPE having different crystallinity. The obtained results can suggest that the trapping proceeds during the high-field treatment and the trap associated with the peak P$_{2}$ may have the closed relation to drystallinity and the release of trapped charge is enhanced by the molecular motion.

• Bulletin of the Korean Chemical Society
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• 제14권2호
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• pp.238-243
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• 1993

A self-consistent-field Green's matrix method for the calculation of electronic properties of chemisorbed system is devised and applied to the methanol on copper(110) surface. The method is based on CNDO Hartree-Fock approximation. Contour integration in the complex energy plane is used for an efficient calculation of the charge-density bond-order matrix. The information on each fragment prior to chemisorption is efficiently used and a small number of iterations are needed to reach the self-consistency. The changes of density of states and other quantities of methanol due to chemisorption are consistent with reported experimental results.

• 대한약학회:학술대회논문집
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• 대한약학회 2003년도 Proceedings of the Convention of the Pharmaceutical Society of Korea Vol.1
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• pp.294.1-294.1
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• 2003

At pH 7.4 (physiological pH), skin is permselective to cations, due to the net negative charge of the current passing channels (pores) in skin. This causes the convective solvent flow (electroosmotic flow) from anode to cathodal direction. In this work, we have investigated several factors (pH. current density and ionic strength) that can affect the electroosmotic flow. (omitted)

• 통합자연과학논문집
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• 제3권4호
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• pp.226-230
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• 2010

Calculation of partial charge is important in chemistry. However, because there are many methods developed, it is of considerable interest to know how to calculate and apply properly to address various chemical problems. For basis set, usually double zeta quality is acceptable, and double zeta polarization function would be enough for most cases. To describe electronic state more accurately, Many electron configurations would be necessary to describe highly strained or anionic species. The NPA population introduced new concept about amide bonds, i.e., the planar geometry of nitrogen atom may not come from resonance, but from the lowering of p-orbital energy by electronegative carbonyl carbon atom. The issues for hypervalent atomic charges was also addressed by various charge derivation scheme. When the charge schemes were applied to organolithium compounds, the ionic nature of boding was revealed. This comes from the fact that previous Mulliken partial atomic charges overemphasized the covalent character, wihout much justification. The other partial charge derivation schemes such as NPA(natural population analysis), IPP (Integrated Projected Population) showed that much more ionic picture. ESP potential derived charges are generally believed to be suitable to describe intermolecular interactions, therefore they are used for molecular dynamics simulations and CoMFA (comparative molecular field analysis). The charge derivation schemes using multipole polarization was mainly applied to reproduce experimental infrared spectroscopy. In some reports these schemes are also suitable for intermecular electrostatic interactions. Charges derived from electron density gradient have shown the some bonds are not straight, but actually bent. The proper choice of charge-calculation method along with suitable level of theory and basis set are briefly discussed.

• 한국의학물리학회지:의학물리
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• 제19권1호
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• pp.73-79
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• 2008

망막색소변성(retinitis pigmentosa: RP)과 연령 관련 황반변성(age-related Macular Degeneration: AMD)은 망막변성으로 인해 실명에 이르는 대표적인 질환이며 망막이식장치의 개발을 통해 치료될 수 있다고 간주되고 있다. 최근에 국내에서도 망막이식장치 개발을 위한 연구팀이 조직되었다. 성공적인 망막이식장치 개발을 위하여 여러 가지 선결요소가 필요하지만 그 중 한 가지가 이식장치에 인가할 전기자극을 최적화하는 것이다. 변성망막의 전기적 특성은 정상 망막과 다르리라 예측되므로 우리는 장차 개발될 망막 이식장치에 인가할 전기자극 최적화를 위한 가이드라인을 제공하기 위해 정상 망막과 변성 망막의 전압자극 파라미터에 관한 실험을 하였다 망막을 분리한 후 망막절편을 신경절세포 층이 다채널전극의 표면을 향하게 하여 전극에 붙인다 in-vitro 상태에서 망막 신경절세포의 전기신호를 기록하기 위해 전극 직경: $30{\mu}m$, 전극간 거리: $200{\mu}s$, 전극 임피던스 1kHz 에서 $50k{\Omega}$인 8행 8열의 다채널전극을 사용하였다. 다채널전극의 60채널 중 두 채널을 자극전극과 접지로 사용하여 단극전기자극을 인가하였고 나머지 전극을 기록전극으로 사용하였다. 가한 전기자극은 전압자극으로 전하균형을 맞춘 이상성자극을 아노딕 사각파를 먼저 주고 캐쏘딕 사각파가 나중에 나오는 형태로 두 사각파간의 지체는 없도록 하였으며 동일한 자극을 2초 간격으로 50회 반복하여 인가하였다. 다양한 전기자극을 사용하였는 바 첫째는 사각파의 크기를 달리하였다 $(0.5{\sim}3V)$. 둘째는 사각파의 시간을 달리하였다 $(100{\sim}1,200{\mu}s)$. 전하밀도는 옴의 법칙과 쿨롱의 법칙을 이용하여 계산하였다. 전기자극으로 유발된 반응은 50회 자극에 대한 평균치를 얻은 후 자극 후 히스토그램(PSTH)을 그려 분석하였다. 전압자극의 크기를 $0.5{\mu}3V$로 달리하였을 때 믿을 만한 망막신경절세포가 유발되는 자극은 1.5V이었고 이때 계산된 전하밀도의 역치는 $2.123mC/cm^2$이었다. 전압의 크기를 2V로 고정하고 자극 지속시간을 $100{\sim}1,200{\mu}s$로 달리하였을 때 믿을 만한 망막신경절세포가 유발되는 자극의 역치는 $300{\mu}s$에서 관찰되었다. 이때 계산된 전하밀도의 역치는 $1.698mC/cm^2$이었다. L-(1)-2-amino-4-phosphonobutyric acid (APB)을 사용하여 ON-경로를 차단한 후에 전기자극을 인가하였을 때도 자극에 의해 망막신경절 세포의 반응이 유발되는 것을 확인하였다. APB-변성망막에서 전압의 크기를 2V로 고정하고 자극 지속시간을 $100{\sim}1,200{\mu}s$로 달리하였을 때 믿을 만한 망막신경절세포가 유발되는 자극의 역치는 $300{\mu}s$에서 관찰되었으며 이는 정상망막의 결과와 같았다. 추후 APB-변성망막을 가지고 좀더 실험이 진행되어야 정상망막과 변성망막의 전하밀도에 관한 명료한 비교가 가능할 것이다.