• 대한전기학회논문지
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• 제39권9호
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• pp.964-975
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• 1990

This paper aims at the design of high voltage electrode contour under specified field condition. Defining the contour with B-Spline curve, the number of contour variables can be reduced and very smooth electrode can be obtained. For the analysis of the electric field, Surface Charge Method which has advantages in practical model has been used. As an initial contour, the rod-plane gap has been used since the difference between maximum and minimum field value is relatively large. Various field conditions including uniform field condition are given to the end of the rod electrode. Under uniform field condition, authors designed an electrode whose field-deviation was under 0.5%. Finally, the relation between the curvature and field of the electrode has been checked, which showed that B-Spline curve is appropriate for the shape function.

• 소음진동
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• 제7권2호
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• pp.231-238
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• 1997

진동하는 구조물의 평면 진동장을 측정하기 위해, 자동화된 스캐닝 레이저 도플러 진동 측정기를 개발하고 이의 성능을 시험하였다. 광섬유를 사용하여 레이저 탐침이 진동체 표면을 따라 움직일 수 있도록 하였으며, 시스템의 자동화를 이루기 위한 알고리즘을 고안하였다. 시스템의 자동화과정은, 레이저 탐침이 진동체 표면을 따라 움직이도록 하며, 표면의 각 측정 점마다 두 레이저 광선들의 초점을 맞추고, 진동 신호 데이터를 얻고 저장하는 모든 과정을 포함한다. 따라서 이 자동화 과정을 이용하여 구조물의 표면 진동장을 측정할 수 있도록 하였다. 이 진동 측정기의 성능을 시험하기 위하여, 연속신호로 가진되는 압전 원통 셸의 진동과 펄스 신호에 의해 가진되는 평판의 진동을 측정하였다. 측정결과로부터, 구조물의 평면 진동장을 측정하고 표면을 따라 전파되는 탄성파들을 분리해내기 위하여, 이 자동화된 스캐닝 레이저 도플러 진동 측정기가 유용한 측정 도구가 될 수 있음을 보였다.

• 한국강구조학회 논문집
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• 제19권3호
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• pp.291-301
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• 2007

재료비선형 수치해석기법 중, 오버레이 모델은 같은 평면상에 여러 개의 레이어를 배치해 각 레이어의 평균한 값을 모델 전체의 값으로 사용하는 원리를 사용하는 모델로서 구성레이어의 변형률 경화계수, 단면적 및 항복응력 등을 파라메타로 설정함으로써 바우싱거 효과 및 변형률 경화현상을 표현하기에 적합한 모델지만, 응력-변형률관계의 기하학적 특징을 직접적으로 근사하기 위한 파라메타의 설정이 복잡하다는 단점이 있다. 본 논문에서는 평면응력상태를 대상으로 하며, 변형률 경화를 고려한 오버레이 모델의 정식화를 열역학을 사용하여 구체적으로 정의한다. 수치해석에 있어 전체적인 해석파라메타로서는 항복응력분포만을 고려하였으며, 항복응력분포의 설정 방법 및 그에 따른 항복응력분포함수의 p, q, r값을 정성적으로 비교분석한다. 최종적으로 탄소강과 합금강에 대한 일축, 다축응력의 실험결과와 제안한 수치해석기법의 해석결과를 비교하여 타당성을 검토한다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1995년도 하계학술대회 논문집 C
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• pp.1098-1101
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• 1995

NbTi thin films were prepared on Si wafer and Cu substrate by rf magnetron sputtering in the range of sputtering pressure $3{\times}10^{-2}$torr to $3{\times}10^{-4}$torr at room temperature. The influence of sputtering pressure and substrate type on crystallographic orientation and morphology of NbTi thin films was investigated by using X-ray diffraction(XRD) and scanning electron microscopy(SEM), respectively. And the effect of crystallographic orientation and morphology of NbTi film on electromagnetic behaviors was estimated by measuring critical current in various applied magnetic field. The film morphology changed from porous structure consisting of tapered crystallites to densely deposited film decreasing with sputtering pressure. The change of crystallographic orientation with the sputtering pressure and rf power was calculated from the texture coefficient of(002) plane based on XRD patterns. It was found that a change of texture coefficient of(002) plane increased with decreasing sputtering pressure. From observation of critical current in various applied magnetic field, we have identified that the change of critical current abruptly decrease applying with magnetic field and NbTi film produced at high sputtering pressure does not exhibit superconductivity but at low sputtering pressure shows superconductivity.

• 대한수학회지
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• 제38권3호
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• pp.595-611
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• 2001

Let Q(n,1) be the set of even unimodular positive definite integral quadratic forms in n-variables. Then n is divisible by 8. For A[X] in Q(n,1), the theta series $\theta$(sub)A(z) = ∑(sub)X∈Z(sup)n e(sup)$\pi$izA[X] (Z∈h (※Equations, See Full-text) the complex upper half plane) is a modular form of weight n/2 for the congruence group Γ$_1$(8) = {$\delta$∈SL$_2$(Z)│$\delta$≡()mod 8} (※Equation, See Full-text). If n$\geq$24 and A[X], B{X} are tow quadratic forms in Q(n,1), the quotient $\theta$(sub)A(z)/$\theta$(sub)B(z) is a modular function for Γ$_1$(8). Since we identify the field of modular functions for Γ$_1$(8) with the function field K(X$_1$(8)) of the modular curve X$_1$(8) = Γ$_1$(8)＼h(sup)* (h(sup)* the extended plane of h) with genus 0, we can express it as a rational function of j(sub) 1,8 over C which is a field generator of K(X$_1$(8)) and defined by j(sub)1,8(z) = $\theta$$_3$(2z)/$\theta$$_3$(4z). Here, $\theta$$_3$ is the classical Jacobi theta series.

• 대한전자공학회논문지
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• 제9권2호
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• pp.17-23
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• 1972

본논문에서는 운동매질내에서 크기가 파장과 동등정도이거나 그 이상인 circular loop antenna의 방사특성을 전류분포가 정현파적인 경우에 대하여 고찰하였다. 고찰결과로는 방사특성이 매질속도의 영향을 받는다는 사실과 그 영향으로는 정지매질의 radiation pattern 과 비교하여 방사지향성이 loop antenna면에 평행인 매질속도성분에만 영향을 받고 수직성분속도에는 무관하며 radiation pattern의 최대지향성은 loop면에 평행인 속도성분방향으로 이동하고 이와 반대방향으로는 Pattern의 크기가 증가하게 된다. 또 이와 같은 운동매질의 영향은 매질속도도가 오고 전류주파수가 높을수록 antenna의 직경이 클수록 더욱 현저하게 된다는 사실을 알게 되었다.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2004년도 추계학술대회 논문집
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• pp.86-89
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• 2004

One most feasible way to measure the concentration field in the micro-channel is using micro-LIF(Laser Induced Fluorescence) method. However, an accurate concentration field at a given cross plane in a micro-channel has not been successfully achieved so far due to various limitations in the light illumination and fluorescence signal detection. The present study demonstrates a novel method to provide an ultra thin laser sheet beam having five(5) microns thickness by use of a micro focus laser line generator. The laser sheet beam illuminates an exact plane of concentration measurement field to increase the signal to noise ratio and considerably reduce the depth uncertainty. Nile Blue A was used as fluorescent dye for the present LIF measurement. The enhancement of the fluorescent intensity signals was performed by a solvent mixture of water $(95\%)$ and ethanol (EtOH)/methanol (MeOH) $(5\%)$ mixture. To reduce the rms errors resulted from the CCD electronic noise and other sources, an expansion of grid size was attempted from $1\times1$ to 3(3 or 5(5 pixel data windows and the pertinent signal-to-noise level has been noticeably increased accordingly.

• Architectural research
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• 제13권3호
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• pp.19-29
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• 2011

Visibility of a space have been defined in several different ways: such as the axial line covering a convex space, a convex space defining the fattest shape in a space and an Isovist field formed by a field of vision at a given vantage point. Isovist fields are referred to as a descriptive medium to describe a movement by reviewing and analyzing geometric properties in them. Many descriptive methods for analysis of three-dimensional isovist are applied to analyzing the morphological properties in a 3D space more realistically. Although these models are regarded as a more advanced method for describing spatial properties, they have pros and cons such as complex mathematical calculations and somewhat arbitrary calibration in addition to huge consumption of memory space. These difficulties lead to the development of a three-dimensional visual accessibility model that explores the implication of building shape on the calculation of isovist fields drawn on a 2D plane. We propose a conceptual framework of how to measure the isovist field not as a 3D volume but as a combination of 2D plane on the ground with the 3D building shape of it's facade.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2004년도 Proceedings of 2004 Korea-Japan Joint Seminar on Particle Image Velocimetry
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• pp.65-74
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• 2004

Measurement of concentration distributions of suspended particles in a micro-channel is out of the most crucial necessities in the area of Lab-on-a-chip to be used for various bio-chemical applications. One most feasible way to measure the concentration field in the micro-channel is using micro-LIF(Laser Induced Fluorescence) method. However, an accurate concentration field at a given cross plane in a micro-channel has not been successfully achieved so far due to various limitations in the light illumination and fluorescence signal detection. The present study demonstrates a novel method to provide an ultra thin laser sheet beam having five(5) microns thickness by use of a micro focus laser line generator. The laser sheet beam illuminates an exact plane of concentration measurement field to increase the signal to noise ratio and considerably reduce the depth uncertainty. Nile Blue A was used as fluorescent dye for the present LIF measurement. The enhancement of the fluorescent intensity signals was performed by a solvent mixture of water $(95\%)$ and ethanol (EtOH)/methanol (MeOH) $(5\%)$ mixture. To reduce the rms errors resulted from the CCD electronic noise and other sources, an expansion of grid size was attempted from $1\times1\;to\;3\times3\;or\;5\times5$ pixel data windows and the pertinent signal-to-noise level has been noticeably increased accordingly.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 C
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• pp.1494-1495
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• 2006

A complete finite element analysis method for discharge onset process, which is governed and coupled by charge transport equation and electric field equation, was presented. The charge transport equation of first order was transformed into a second-order one by utilizing the artificial diffusion scheme. The two second-order equations were analyzed by the finite element formulation which is well-developed for second-order ones. The Fowler-Nordheim injection boundary condition was adopted for charge transport equation. After verifying the numerical results by comparing to the analytic solutions using parallel plane electrodes with one carrier system, we extended the result to blade-plane electrodes in 2D xy geometry with three carriers system. Radius of the sharp tip was taken to be 50 ${\mu}m$. When this sharp geometry was solved by utilizing the space discretizing methods, the very sharp tip was found to cause a singularity in electric field and space charge distribution around the tip. To avoid these numerical difficulties in the FEM, finer meshes, a higher order shape function, and artificial diffusion scheme were employed.