• 한국결정성장학회지
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• 제11권1호
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• pp.20-26
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• 2001

Ti와 B을 각각의 증발원으로 한 2원 전자빔 증착법으로 500$^{\circ}$의 기판온도에서 (100) Si 기판 위에 티타늄 붕화물 (${TiB}_{x}$) 박막을 증착시켰다. 이 방법은 여러 가지 boron-to-totanium ratio ($0{\le}B/Ti \le 2.5$)를 가지는 비당량 (${TiB}_{x}$ 박막의 표면 조도 역시 B/Ti비에 의존하여 변화되었다. 그리고 Pure Ti 박막은 (002)면의 우선 성장거동을 나타내었으나, $B/Ti{\ge}1.0$의 경우 (111)면의 우선 성장거동을 보이는 단일상의 TiB 박막이 성장되었다. 그러나 B농도가 더욱 증가됨에 따라 육방정계의 ${TiB}_{2}$상이 형성되기 시작하여 $B/Ti{\ge}2.0$ 의 조성비를 가지는 박막에서는 단일상의 ${TiB}_{2}$ 화합물을 나타내었다. 그리고 Si 기판상에 증착된 ${TiB}_{x}$ 박막의 잔류응력은 B/Ti비에 의존하나, 2원 전자빔 증착법으로 성장된 모든 박막에서 3~$20{\times}^9$dyn/$\textrm{cm}^2$ 정도의 인장응력을 나타내었다.

• 한국자기학회지
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• 제12권5호
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• pp.184-188
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• 2002

수직자기이방성을 가지는 Cu/Ni/Cu(002)/Si(100) 자성박막을 전자빔 증발법을 이용하여 초고진공에서 증착 하였다. 증착 시 RHEED로 측정 한 결과 실리콘 기판 위에 자성박막이 적층성장되었음을 확인하였다. 이러한 Cu/Ni/Cu(001)/Si(100) 자성박막에 1 MeV C 이온을 이온선량 2$\times$$10^{16}$ ions/$\textrm{cm}^2$로 조사한 후 MOKE로 자기이력곡선을 측정한 결과 이온 조사에 의해 자화용이축이 수직에서 수평방향으로 변화되었음을 확인하였다 포항 방사광가속기를 이용하여 X-선 반사도와 Grazing Incident X-ray diffraction(GE) 분석을 수행한 결과 첫 번째 Cu층과 Ni층 사이의 계면은 이온 조사 후 거칠기는 증가하였으나, Cu와 Ni의 전자밀도의 대비는 더욱 명확해졌다. 그리고, 증착 후 Cu와 Ni원자의 격자 상수 차이에 의해 Ni층이 가지고 있었던 strain은 이온 조사 후 완화되었음을 알 수 있었다. 끝으로, 이온조사 시 자성특성 변화와 직접적인 관계가 있는 strain 완화, 계면 혼합층(혹은 새로운 상)등이 생성되는 기구를 탄성충돌 및 비탄성충돌에 의한 열화학적 구동력으로 규명하였다.

• Structural Engineering and Mechanics
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• 제70권4호
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• pp.479-497
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• 2019

In the current code design, the use of a uniform internal pressure coefficient of cooling towers as internal suction cannot reflect the 3D characteristics of flow field inside the tower body with different ventilation rate of shutters. Moreover, extreme weather such as heavy rain also has a direct impact on aerodynamic force on the internal surface and changes the turbulence effect of pulsating wind. In this study, the world's tallest cooling tower under construction, which stands 210m, is taken as the research object. The algorithm for two-way coupling between wind and rain is adopted. Simulation of wind field and raindrops is performed iteratively using continuous phase and discrete phase models, respectively, under the general principles of computational fluid dynamics (CFD). Firstly, the rule of influence of 9 combinations of wind speed and rainfall intensity on the volume of wind-driven rain, additional action force of raindrops and equivalent internal pressure coefficient of the tower body is analyzed. The combination of wind velocity and rainfall intensity that is most unfavorable to the cooling tower in terms of distribution of internal pressure coefficient is identified. On this basis, the wind/rain loads, distribution of aerodynamic force and working mechanism of internal pressures of the cooling tower under the most unfavorable working condition are compared between the four ventilation rates of shutters (0%, 15%, 30% and 100%). The results show that the amount of raindrops captured by the internal surface of the tower decreases as the wind velocity increases, and increases along with the rainfall intensity and ventilation rate of the shutters. The maximum value of rain-induced pressure coefficient is 0.013. The research findings lay the basis for determining the precise values of internal surface loads of cooling tower under extreme weather conditions.

• Structural Engineering and Mechanics
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• 제66권2호
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• pp.273-283
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• 2018

Currently, the dynamic amplification effect of suction is described using the wind vibration coefficient (WVC) of external loads. In other words, it is proposed that the fluctuating characteristics of suction are equivalent to external loads. This is, however, not generally valid. Meanwhile, the effects of the ventilation rate of louver on suction and its WV are considered. To systematically analyze the effects of the ventilation rate of louver on the multi-dimensional WVC of ultra-large cooling towers under suctions, the 210 m ultra-large cooling tower under construction was studied. First, simultaneous rigid pressure measurement wind tunnel tests were executed to obtain the time history of fluctuating wind loads on the external surface and the internal surface of the cooling tower at different ventilation rates (0%, 15%, 30%, and 100%). Based on that, the average values and distributions of fluctuating wind pressures on external and internal surfaces were obtained and compared with each other; a tower/pillar/circular foundation integrated simulation model was developed using the finite element method and complete transient time domain dynamics of external loads and four different suctions of this cooling tower were calculated. Moreover, 1D, 2D, and 3D distributions of WVCs under external loads and suctions at different ventilation rates were obtained and compared with each other. The WVCs of the cooling tower corresponding to four typical response targets (i.e., radial displacement, meridional force, Von Mises stress, and circumferential bending moment) were discussed. Value determination and 2D evaluation of the WVCs of external loads and suctions of this large cooling tower at different ventilation rates were proposed. This study provides references to precise prediction and value determination of WVC of ultra-large cooling towers.

• Wind and Structures
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• 제27권1호
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• pp.11-27
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• 2018

The straight-cone steel cooling tower is a novel type of structure, which has a distinct aerodynamic distribution on the internal surface of the tower cylinder compared with conventional hyperbolic concrete cooling towers. Especially in the extreme weather conditions of strong wind and heavy rain, heavy rain also has a direct impact on aerodynamic force on the internal surface and changes the turbulence effect of pulsating wind, but existing studies mainly focus on the impact effect brought by wind-driven rain to structure surface. In addition, for the indirect air cooled cooling tower, different additional ventilation rate of shutters produces a considerable interference to air movement inside the tower and also to the action mechanism of loads. To solve the problem, a straight-cone steel cooling towerstanding 189 m high and currently being constructed is taken as the research object in this study. The algorithm for two-way coupling between wind and rain is adopted. Simulation of wind field and raindrops is performed with continuous phase and discrete phase models, respectively, under the general principles of computational fluid dynamics (CFD). Firstly, the rule of influence of 9 combinations of wind sped and rainfall intensity on flow field mechanism, the volume of wind-driven rain, additional action force of raindrops and equivalent internal pressure coefficient of the tower cylinder is analyzed. On this basis, the internal pressures of the cooling tower under the most unfavorable working condition are compared between four ventilation rates of shutters (0%, 15%, 30% and 100%). The results show that the 3D effect of equivalent internal pressure coefficient is the most significant when considering two-way coupling between wind and rain. Additional load imposed by raindrops on the internal surface of the tower accounts for an extremely small proportion of total wind load, the maximum being only 0.245%. This occurs under the combination of 20 m/s wind velocity and 200 mm/h rainfall intensity. Ventilation rate of shutters not only changes the air movement inside the tower, but also affects the accumulated amount and distribution of raindrops on the internal surface.

• 대한방사선기술학회지:방사선기술과학
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• 제35권2호
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• pp.165-172
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• 2012

VX2 암종을 이식한 토끼 뇌종양 모델에서, perfusion CT(computed tomography, CT)를 이용하여 종양과 정상 뇌조직의 혈류 특성을 알아보고자 하였다. 체중 2.4~3.0kg(평균 2.6kg)의 토끼(New Zealand white rabbit) 수놈 9마리를 대상으로, 토끼 뇌에 VX2 세포 현탁액 $1{\times}10^7$ cells/ml, 0.1 ml을 이식하고 종양이 5mm 정도 크기로 자라면 perfusion CT를 시행 하였다. GE사의 AW(advantage windows workstation, version 4.2)로 종양의 용적과 perfusion 값을 산출 하였다. 뇌종양의 평균 용적은 $316{\pm}181mm^3$ 이었고, 가장 큰 종양은 497 $mm^3$, 가장 작은 종양은 195 $mm^3$ 이었 이식된 종양 모두 단일 결절형으로 만들어졌고, 두개강 내로 전이는 발견되지 않았다. perfusion CT에서 종양 중심부의 혈류량(cerebral blood volume, CBV)은 $74.40{\pm}9.63$ 이었고, 종양쪽 정상 뇌조직에서는 $16.08{\pm}0.64$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $15.24{\pm}3.23$이었다. 혈류 속도(cerebral blood flow, CBF)는 종양 중심부에서 $962.91{\pm}75.96$ 이였고, 종양쪽 정상 뇌조직에서는 $357.82{\pm}12.82$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $323.19{\pm}83.24$ 이었다. 평균 통과시간(mean transit time, MTT)은 종양 중심부에서 $4.37{\pm}0.19$ 이었고, 종양쪽 정상 뇌조직에서는 $3.02{\pm}0.41$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $2.86{\pm}0.22$ 이었다. 투과성 표면적(permeability surface, PS)은 종양 중심부에서 $47.23{\pm}25.45$ 이었고, 종양쪽 정상 뇌조직에서는 $14.54{\pm}1.60$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $6.81{\pm}4.20$이었다. 또한, 종양 중심부에서 최고치 도달 시간(time to peak, TTP)은 $19.33{\pm}0.42$ 이었고, 종양쪽 정상 뇌조직에서는 $16.43{\pm}1.72$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $15.14{\pm}0.88$이었지만 통계적으로 유의하지 않았다. PEI(positive enhancement integral, PEI)은 종양 중심부에서 $61.56{\pm}16.07$ 이었고, 종양쪽 정상 뇌조직에서는 $12.58{\pm}2.61$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $8.26{\pm}5.55$ 이었다. 최대 증가 기울기(maximum slope of increase, MSI)는 종양 중심부에서 $13.18{\pm}2.81$ 이었고, 종양쪽 정상 뇌조직에서는 $6.99{\pm}1.73$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $6.41{\pm}1.39$ 이었다. 최대 감소 기울기(maximum slope of decrease, MSD)는 종양 중심부에서 $4.02{\pm}1.37$ 이었고, 종양쪽 정상 뇌조직에서는 $4.66{\pm}0.83$ 이었으며, 종양 반대쪽 정상 뇌조직에서는 $6.47{\pm}1.53$ 으로 나타났다. 결과적으로 정위적(stereotactic)으로 이식된 종양은 단일 결절형으로 두개강 내에 전이가 없어 정상 조직과 종양 조직의 비교 연구에 적합하며, perfusion CT 에서 얻어진 매개 변수(parameter)들은 종양과 정상 조직의 혈관 관류 상태 차이를 잘 반영해 주었다.

• 한국초전도학회:학술대회논문집
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• 한국초전도학회 1999년도 High Temperature Superconductivity Vol.IX
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• pp.152-159
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• 1999

YBa$_2Cu_3O_{7-{\delta}}$ (YBCO) films grown on CeO$_2$-buffered r-cut sapphire substrates (CbS's) were prepared and their structural and electrical properties were measured. Post-annealed CeO$_2$ films were used as buffer layers for the experiments. It turned out that the YBCO films grown on post-annealed CbS's had the rms roughness of less than 20 ${\AA}$ and peak-to-peak roughness of about 30 ${\AA}$ when the YBCO film thickness was 3000 ${\AA}$. Meanwhile, YBCO films on in-situ grown CeO$_2$ buffer layers on r-cut sapphire substrates appeared to have the peak-to-peak roughness of more than 450 ${\AA}$. X-ray diffraction data revealed that the YBCO flms were epitaxially grown along the c-axis with the typical FWHM of(005) ${\theta}$ -2 ${\theta}$ peak about 0. 16 $^{\circ}$ and ${\Delta}$ ${\omega}$ of the (005) peak about 0.5 $^{\circ}$. T$_c$ > 87 K, ${\Delta}$T < 1 K and R(look)/R(100K) ${\ge}$3 were observed from the YBCO films. Applicability of the YBCO films for high-frequency applications was described.