• Applied Biological Chemistry
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• 제43권2호
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• pp.116-123
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• 2000

작물이 자라는 토양에서 점적 관개에 의해 일어나는 토양 수분의 분포와 이동을 3차원 직교 좌표계로 예측할 수 있는 수학적 모델을 개발하였다. 모델은 지면 증발과 증산을 고려하였으며, 이들의 계절적 현화와 하루 중의 시간변화 뿐 아니라 작물 뿌리의 성장 및 뿌리의 토양 중 분포형태도 고려하였다. 모델의 해는 block centered grid system등을 적용하여 Crank-Nicolson법과 Gauss-Seidel 반복법을 사용하여 구하였다. 모델은 실험을 통해 검증하였으며, 점적 관개의 특성을 알기 위하여 모델을 이용한 컴퓨터 모사를 실시하였고, 본 연구의 조건으로부터 다음의 결과를 얻었다. (1) 관수된 물은 점적기에서 멀어짐에 따라 그 유속이 크게 감소하였고, 관수 시간이 증가함에 따라 습윤구역의 크기가 증가하는 속도도 급격히 감소하였다. (2) 1점 관수의 경우 습윤구역은 수평 방향보다는 수직 방향으로 더 깊이까지 도달하였다. (3) 본 연구조건에서 물이용 효율은 지하 25cm지점의 4점 관수가 가장 좋았으며, 지표면 1점 관수보다 증산량은 10% 증가, 지면 증발량은 20% 감소하였다. (4) disk tension infiltrometer에 의한 토양의 수분보유도 함수는 토양수분 압출에 의한 젖음 곡선과는 상당한 차이를 나타내는 것도 알 수 있었다.

• 한국재료학회지
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• 제10권4호
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• pp.295-300
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• 2000

반응성 이온 식각과 산화막을 이용한 첨예화 공정을 통하여 균일한 실리콘 팁 어레이를 제작한 후, 그 위에 Pd을 증착하여, Pd 코팅이 전계 방출특성에 미치는 영향에 대해 조사하였다. 어레이에 존재하는 표면 산화막을 제거한 후의 전계 방출 특성의 향상은 매우 작았으나, $100{\AA}$의 Pd을 코팅한 후에는 30V의 구동전압이 감소하는 등 전계 방출특성이 크게 향상되었다. 이는 Pd 코팅에 의해 팁의 표면 거칠기가 증가하고, 전자가 방출되는 팁 끝부분의 반경이 감소하였기 때문이다. 한편 Pd을 코팅한 에미터는 높은 방출 전류 영역에서 우수한 동작 안전성을 보였다. 이를 통하여 Pd이 코팅된 실리콘 에미터가 고온에서의 동작과 표면안정성에서 우수한 특성을 보임을 알 수 있었다.

• 한국진공학회지
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• 제20권6호
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• pp.436-441
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• 2011

각종 전자 방출원 및 디스플레이 응용 분야에서 뛰어난 가능성을 보이고 있는 탄소나노튜브의 전계 방출 특성을 개선하고 전자방출의 신뢰성을 개선하기 위해 탄소나노튜브의 표면에 수 nm 두께의 금속 코팅을 적용하였다. 탄소나노튜브는 실리콘 기판위에 2 nm 두께의 Invar (52% Fe, 42% Ni, 6% Co alloy) 촉매를 사용하여 $450^{\circ}C$의 온도에서 플라즈마 화학기상 증착법으로 성장시켰다. 성장된 탄소나노튜브의 밀도 제어를 위해 성장 후 질소 플라즈마로 일부를 식각한 후 티타늄(Ti) 금속을 탄소나노튜브 표면에 5~150 nm 두께로 스퍼터링 증착하였다. 5 nm로 티타늄을 탄소나노튜브 표면에 코팅한 경우, 코팅 전에 비해 6 V/${\mu}m$의 전계에서 전류밀도가 4배 이상 증가되었으며, 전계 방출 전류의 요동(fluctuation) 또한 40% 이상 감소됨을 확인할 수 있었다. 이는 티타늄의 일함수가 4.3 eV로 탄소나노튜브의 5 eV에 비해 작을 뿐만 아니라, 탄소나노튜브의 약점으로 지적되는 기판과의 접착성과 접촉저항이 티타늄의 표면 코팅으로 인해 크게 개선된 결과로 판단된다.

• 한국기후변화학회지
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• 제9권4호
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• pp.325-342
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• 2018

The Korea Emissions Trading Scheme ( K-ETS), which manages roughly 70% of the greenhouse gas emissions in South Korea, was initiated in 2015, after implementation of its 1st basic plan and the 1st allocation plan (2014) for the 1st phase (2015-2017). During the three and a half years since the launch of K-ETS, there have been critical policy change such as adjustment of the institutions involved, development and revision of the 2030 national GHG reduction roadmap, and change in the allocation plans. Moreover, lack of liquidity and fluctuation of carbon prices in the K-ETS market during this period has forced the Korean government to adjust the flexibility mechanism and auction permits of the market stability reserve. To evaluate the policy change in the K-ETS regarding conformance to its objectives, this study defines three objectives (Environmental Effectiveness, Cost Effectiveness and Economic Efficiency) and ten indicators. Evaluation of Environmental Effectiveness of K-ETS suggests that the national GHG reduction roadmap, coverage of GHG emitters and credibility of MRV positively affect GHG mitigation. However, there was a negative policy change implemented in 2017 that weakened the emission cap during the 1st phase. In terms of the Cost Effectiveness, the K-ETS policies related to market management and flexibility mechanism (e.g. banking, borrowing and offsets) were improved to deal with the liquidity shortage and permit price increase, which were caused by policy uncertainty and conservative behavior of firms during 2016-2018. Regarding Economic Efficiency, K-ETS expands benchmark?based allocation and began auction-based allocation; nevertheless, free allocation is being applied to sectors with high carbon leakage risk during the 2nd phase (2018-2020). As a result, it is worth evaluating the K-ETS policies that have been developed with respect to the three main objectives of ETS, considering the trial?and?error approach that has been followed since 2015. This study suggests that K-ETS policy should be modified to strengthen the emission cap, stabilize the market, expand auction-based allocation and build K-ETS specified funds during the 3rd phase (2021-2025).

• 핵의학기술
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• 제23권1호
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• pp.50-53
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• 2019

본 연구는 고에너지의 베타선을 방출하는 Y-90 미세구의 경동맥방사선색전술 시 발생되는 제동복사선에 의한 불필요한 외부피폭을 줄이고자 텅스텐 차폐체를 개발하였다. 본 연구에서는 다양한 용량(1 GBq, 2 GBq, 4 GBq)의 $SIR-Spheres^{(R)}$ Y-90 미세구를 사용하여, 텅스텐 차폐체 표면으로부터 10 cm, 50 cm, 100 cm인 곳에서 GM tube식 디지털 서베이미터로 선량률을 측정하였다. 텅스텐 차폐체 표면 10 cm 위치에서 차폐율을 분석한 결과 4 GBq의 $SIR-Spheres^{(R)}$ Y-90 미세구의 경우 90.9%, 2 GBq의 경우 88.9%, 1 GBq의 경우 88.8%의 차폐율을 보였고, 표면 50 cm 위치에서 차폐율은 4 GBq의 $SIR-Spheres^{(R)}$ Y-90 미세구의 경우 89.2%, 2 GBq의 경우 87.5%, 1GBq의 경우 86.3%로 나타났다. 텅스텐 차폐체 표면 100 cm 위치에서 텅스텐 차폐체는 평균 75.1%의 차폐율을 보이는 것으로 확인할 수 있었다. 높은 용량이 함유된 $SIR-Spheres^{(R)}$ Y-90 미세구의 경동맥방사선색전술시 방사선 작업종사자와 선원간의 거리가 짧고, 작업시간이 길기 때문에 제동복사선에 의한 피폭에 노출될 수 있다. 본 연구를 통해 개발된 텅스텐 차폐체는 향후 임상에서 경동맥방사선색전술 시 제동복사선에 의한 외부피폭을 줄이는데 활용될 수 있을 것이라 기대 된다.

• 한국대기환경학회지
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• 제32권5호
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• pp.501-512
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• 2016

The study evaluated methods to measure condensable fine particles in flue gases and measured particulate matter by fuel and material to get precise concentrations and quantities. As a result of the method evaluation, it is required to improve test methods for measuring Condensable Particulate Matter (CPM) emitted after the conventional Filterable Particulate Matter (FPM) measurement process. Relative Standard Deviation (RSD) based on the evaluated analysis process showed that RSD percentages of FPM and CPM were around 27.0~139.5%. As errors in the process of CPM measurement and analysis can be caused while separating and dehydrating organic and inorganic materials from condensed liquid samples, transporting samples, and titrating ammonium hydroxide in the sample, it is required to comply with the exact test procedures. As for characteristics of FPM and CPM concentrations, CPM had about 1.6~63 times higher concentrations than FPM, and CPM caused huge increase in PM mass concentrations. Also, emission concentrations and quantities varied according to the characteristics of each fuel, the size of emitting facilities, operational conditions of emitters, etc. PM in the flue gases mostly consisted of CPM (61~99%), and the result of organic/inorganic component analysis revealed that organic dusts accounted for 30~88%. High-efficiency prevention facilities also had high concentrations of CPM due to large amounts of $NO_x$, and the more fuels, the more inorganic dusts. As a result of comparison between emission coefficients by fuel and the EPA AP-42, FPM had lower result values compared to that in the US materials, and CPM had higher values than FPM. For the emission coefficients of the total PM (FPM+CPM) by industry, that of thermal power stations (bituminous coal) was 71.64 g/ton, and cement manufacturing facility (blended fuels) 18.90 g/ton. In order to estimate emission quantities and coefficients proper to the circumstances of air pollutant-emitting facilities in Korea, measurement data need to be calculated in stages by facility condition according to the CPM measurement method in the study. About 80% of PM in flue gases are CPM, and a half of which are organic dusts that are mostly unknown yet. For effective management and control of PM in flue gases, it is necessary to identify the current conditions through quantitative and qualitative analysis of harmful organic substances, and have more interest in and conduct studies on unknown materials' measurements and behaviors.

• E2M - 전기 전자와 첨단 소재
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• 제12권7호
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• pp.7-11
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• 1999

Fully sealed field emission display in size of 4.5 inch has been fabricated using single-wall carbon nanotubes-organic vehicle com-posite. The fabricated display were fully scalable at low temperature below 415$^{\circ}C$ and CNTs were vertically aligned using paste squeeze and surface rubbing techniques. The turn-on fields of 1V/${\mu}{\textrm}{m}$ and field emis-sion current of 1.5mA at 3V/${\mu}{\textrm}{m}$ (J=90${\mu}{\textrm}{m}$/$\textrm{cm}^2$)were observed. Brightness of 1800cd/$m^2$ at 3.7V/${\mu}{\textrm}{m}$ was observed on the entire area of 4.5-inch panel from the green phosphor-ITO glass. The fluctuation of the current was found to be about 7% over a 4.5-inch cath-ode area. This reliable result enables us to produce large area full-color flat panel dis-play in the near future. Carbon nanotubes (CNTs) have attracted much attention because of their unique elec-trical properties and their potential applica-tions [1, 2]. Large aspect ratio of CNTs together with high chemical stability. ther-mal conductivity, and high mechanical strength are advantageous for applications to the field emitter [3]. Several results have been reported on the field emissions from multi-walled nanotubes (MWNTs) and single-walled nanotubes (SWNTs) grown from arc discharge [4, 5]. De Heer et al. have reported the field emission from nan-otubes aligned by the suspension-filtering method. This approach is too difficult to be fully adopted in integration process. Recently, there have been efforts to make applications to field emission devices using nanotubes. Saito et al. demonstrated a car-bon nanotube-based lamp, which was oper-ated at high voltage (10KV) [8]. Aproto-type diode structure was tested by the size of 100mm $\times$ 10mm in vacuum chamber [9]. the difficulties arise from the arrangement of vertically aligned nanotubes after the growth. Recently vertically aligned carbon nanotubes have been synthesized using plasma-enhanced chemical vapor deposition(CVD) [6, 7]. Yet, control of a large area synthesis is still not easily accessible with such approaches. Here we report integra-tion processes of fully sealed 4.5-inch CNT-field emission displays (FEDs). Low turn-on voltage with high brightness, and stabili-ty clearly demonstrate the potential applica-bility of carbon nanotubes to full color dis-plays in near future. For flat panel display in a large area, car-bon nanotubes-based field emitters were fabricated by using nanotubes-organic vehi-cles. The purified SWNTs, which were syn-thesized by dc arc discharge, were dispersed in iso propyl alcohol, and then mixed with on organic binder. The paste of well-dis-persed carbon nanotubes was squeezed onto the metal-patterned sodalime glass throuhg the metal mesh of 20${\mu}{\textrm}{m}$ in size and subse-quently heat-treated in order to remove the organic binder. The insulating spacers in thickness of 200${\mu}{\textrm}{m}$ are inserted between the lower and upper glasses. The Y\ulcornerO\ulcornerS:Eu, ZnS:Cu, Al, and ZnS:Ag, Cl, phosphors are electrically deposited on the upper glass for red, green, and blue colors, respectively. The typical sizes of each phosphor are 2~3 micron. The assembled structure was sealed in an atmosphere of highly purified Ar gas by means of a glass frit. The display plate was evacuated down to the pressure level of 1$\times$10\ulcorner Torr. Three non-evaporable getters of Ti-Zr-V-Fe were activated during the final heat-exhausting procedure. Finally, the active area of 4.5-inch panel with fully sealed carbon nanotubes was pro-duced. Emission currents were character-ized by the DC-mode and pulse-modulating mode at the voltage up to 800 volts. The brightness of field emission was measured by the Luminance calorimeter (BM-7, Topcon).