• 태양에너지
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• 제6권2호
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• pp.3-14
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• 1986

It is desirable to collect the solar thermal energy at relatively high temperature in order to minimize the size of thermal storage system and to enlarge the scope of solar thermal energy utilization. In this study, to develop a solar collector that has both advantages of collecting solar thermal energy at high temperature and fixing conveniently the collector system for long term period, a cylindrical parabolique concentrating solar collector (M.C.P.C.S.C) was designed, which has several rows of parabolique reflectors and thin thickness such as the flat-plate solar collector, maintaining the optical form of concentrating solar collector. The thermal performance of the M.C.P.C.S.C. newly designed in this study was analysed theoretically and experimentally. The results are summarized as follows: 1) prediction equation for outlet temperature, $T_o$, of heat transfer fluid and for the thermal efficiency, ${\eta}$, of the collector were derived as; o $$T_o=[C+B1_n(\frac{I_c(t)}{pv^3})]T_i$$ o $${\eta}=\frac{A}{A_c}\dot{m}[(C-1)+B1_n(E{\cdot}di^6\frac{I_c(t)}{\dot{m}^3})]\frac{T_i}{I_c(t)}$$ 2) When the insolation on the tilted solar collector surface, $I_c$, was $900-950W/m^2$ and the heat transfer fluid was not circulated in tubular absorber, the maximum temperature on the absorber surface was $100-118^{\circ}C$, this result suggested that the heat transfer fluid could be heated up to $98-116^{\circ}C$. The maximum temperature on the absorber surface was decreased with the increase of the collector shape factor, $L_p/L_w$ 3) There was a good agreement between the experimental and theoretical value of solar collector efficiency, ${\eta}$, which was proportional to the collector shape factor, $L_p/L_w$ 4) It is desirable to continue the study on the relationship between the collector shape factor, $L_p/L_w$, and the thermal efficiency of solar collector.

• 공업화학
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• 제33권6호
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• pp.606-612
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• 2022

수용액에서 수용성 염료를 소수성 염료로 전환시킨 후 마이크로 버블을 이용한 침전 및 부상응집에 의한 염료를 제거하는 연구를 수행하였다. 양이온성 염료에 음이온 collector를 반응시키며, 또한 음이온성 염료에 양이온 collector를 첨가하여 소수성으로 변환시켰다. 소수성으로 전환된 염료 용액을 회분식 반응기에 저장하여 마이크로 버블을 분사시켜 색을 제거하였다. 염료 용액을 제조하기 위해 Basic Yellow 1 및 Direct Orange 10을 사용하였으며, sodium dodecyl sulfate, oleic acid sodium salt 및 amine류와 같은 음이온 및 양이온 collector를 사용하면 색 제거에 효과적이었으며, 모든 색은 8분 이내에 제거되었다. 색 제거는 collector의 첨가량과 수용액 pH의 영향을 받으며, 염료농도에 비해 극히 소량의 계면활성제를 첨가하였을 경우에는 pH에 의존하였으나, 염료농도와 비슷한 collector 양을 첨가하였을 경우에는 pH에 의존하지 않았음을 알 수 있었다. 그 이유는 collector와 염료가 1:1M로 반응하여 소수성이 완전히 부여되어야 제거됨을 알 수 있었다.

• 공업화학
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• 제10권4호
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• pp.576-580
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• 1999

Column에 공기를 분사시켜 수용액으로부터 색을 제거하기 위한 연구를 수행하였다. 착색 용액을 제조하기 위해 Basic Yellow 28 및 Direct Orange 31을 사용하였으며, 모든 색은 8분 이내에 제거되었다. Sodium dodecyl sulfate, oleic acid sodium salt 및 amines와 같은 collector는 색 제거에 효과적이었다. 색 제거는 collector의 첨가량과 수용액 pH의 영향을 받는다고 할 수 있으나, 소량의 collector를 첨가하였을 경우에는 pH에 의존하였으나, 많은 양을 첨가하였을 경우에는 pH에 의존하지 않았음을 알 수 있었다.

• 전자공학회논문지D
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• 제36D권3호
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• pp.66-74
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• 1999

HMC(Hybrid Monte Carlo)시뮬레이션을 이용하여 InAlGaAs/InGaAs HBT의 비평형 고속전송을 해석하였고, 전송시간 및 차단주파수를 향상시키기 위하여 에미터-베이터 이종접합과 콜렉터 구조를 최적 설계 하였다. 시뮬레이션 결과, 에미터 조성경사영역에서 Al 몰비를 xf=1.0에서 xf=0.5로 변화시킬 경우 베이스 전송시간이τb=0.21ps로 가장 짧았다. 콜렉터 전송시간을 단축시킬 목적으로 콜렉터와 베이스 사이에 n\sup +\형 (콜렉터-Ⅰ), I형(콜렉터-Ⅱ), p형(콜렉터-Ⅲ), 콜렉터를 삽입하여 베이스-콜렉터 공간전하영역의 전계분포를 전자의 비평형고속전송을 유지하도록 설계하였다. 콜렉터-Ⅲ 구조에서는 전자의 음이온화된 억셉터가 콜렉터의 전계를 감소시킴으로써 전자가 Γ 밸리에서 먼 거리까지 전송을 가능하게 하여 가장 짧은 콜렉터 전송시간을 나타내었다. 결론적으로 가장 짧은 전송시간 τec는 Al 몰비가 xf=0.5인 에미터 구조와 콜렉터-Ⅲ에서 0.87psec이었고, 차단주파수 ft=183GHz를 나타내었다.

• 한국전기전자재료학회논문지
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• 제19권10호
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• pp.907-911
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• 2006

In this paper, we propose a new structure that improves the on-state voltage drop and switching speed in Insulated Gate Bipolar Transistors(IGBTs), which can be widely used in high voltage semiconductors. The proposed structure is unique in that the collector area is divided by $SiO_2$, whereas the conventional IGBT has a planar P+ collector structure. The process and device simulation results show remarkably improved on-state and switching characteristics. Also, the current and electric field distribution indicate that the segmented collector structure has increased electric field near the $SiO_2$ corner, which leads to an increase of electron current. This results in a decrease of on-state resistance and voltage drop to $30%{\sim}40%$. Also, since the area of the P+ region is decreased compared to existing structures, the hole injection decreases and leads to an increase of switching speed to 30 %. In spite of some complexity in process procedures, this structure can be manufactured with remarkably improved characteristics.

• 전기학회논문지P
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• 제66권1호
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• pp.38-42
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• 2017

The wear of the third track power collector is one of the essential check factors for safe train operation. Rapid wear of the current collector accelerates the line of the catenary. In addition, the arc generated when the catenary line is turned off causes a malfunction in the minute portion of the catenary line, thereby shortening the life of the catenary line. In this paper, to analyze the mechanical wear of the current collector during driving according to the environmental factor of the Maglev(magnetic levitation train), it was divided into dry season and wet season. the wear of metallized collector, copper alloy collector and carbon collector were measured and compared with each other. The wear rate was measured according to the position of the wire, the position of the power collector and the position per hour. Microscopic photographs of the cross section and surface of the power collector were measured. The electrical currents of the metallized collector, copper alloy collector and carbon collector were measured.

• Journal of Biosystems Engineering
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• 제10권1호
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• pp.54-68
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• 1985

It is desirable to collect the solar thermal energy at relatively high temperature in order to minimize the size of thermal storage system and to enlarge the scope of solar thermal energy utilization. So far the concentrating solar collector has been developed to collect solar thermal energy at relatively high temperature, but it has some difficulties in maintaining the volumetric body of solar collector for long term utilization. On the other hand, the flat-plate solar collector has been developed to collect the solar thermal energy at low temperature, and it has advantages in maintaining the system for long term utilization, since it's thickness is thin and not volumetric. In this study, to develop a solar collector that has both advantages of collecting solar thermal energy at high temperature and fixing conveniently the collector system for long term period, a cylindrical parabolic concentrating solar collector was designed, which has two rows of parabolic reflectors and thin thickness such as the flat-plate solar collector, maintaining the optical form of concentrating solar collector. The characteristics of the concentrating parabolic solar collector newly designed was analysed and the results are summarized as follows; 1. The temperature of the air enclosed in solar collector was all the same as $50^{\circ}C$ in both cases of the open and closed loop, and when the heat transfer fluid was not circulated in tubular absorber, the maximum surface temperature of the absorber was $118-120^{\circ}C$, this results suggested that the heat transfer fluid could be heated up to $118^{\circ}C$. 2. In case of longitudinal installation of the solar collector, the temperature difference of heat transfer fluid between inlet and outlet was $4^{\circ}-6^{\circ}C$ at the flow rate of $110-130{\ell}/hr$, and the collected solar energy per unit area of collector was $300-465W/m^2$. 3. The collected solar energy per unit area for 7 hours was 1960 Kcal/$m^2$ for the open loop and 220 Kcal/$m^2$ for the closed loop. Therefore it is necessary to combine the open and closed loop of solar collectors to improve the thermal efficiency of solar collector. 4. The thermal efficiency of the solar collector (C.P.C.S.C.) was proportional to the density of solar radiation, indicating the maximum thermal efficiency ${\eta}_{max}=58%$ with longitudinal installation and ${\eta}_{max}=45%$ with lateral installation. 5. The thermal efficiency of the solar collector (C.P.C.S.C.) was increased in accordance with the increase of flow rate of heat transfer fluid, presenting the flow rate of $110{\ell}/hr$ was the value of turning point of the increasing rate of the collector efficiency, therefore the flow rate of $110{\ell}/hr$ was considered as optimum value for the test of the solar collector (C.P.C.S.C.) performance when the heat transfer fluid is a liquid. 6. In both cases of longitudinal and lateral installation of the solar collector (C.P.C.S.C.), the thermal efficiency was decreased linearly with an increase in the value of the term ($T_m-T_a$)/Ic and the increasing rate of the thermal efficiency was not effected by the installation method of solar collector.

• 한국환경과학회지
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• 제7권1호
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• pp.36-40
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• 1998

This study was carried out to investigate the collection Efficiency of mass in collector step at the different of physical gas characterization. This work has focused on the dependence of the collection efficiency of mass in the collector zone of a two-stage set up field with gas temperature T and the dew point tmeperature. To identify the dependence of the mass collection efficiency on the Bounded plate of the collector zone MP.k by the spectre electric resistance of dust $p_e$. and the relative humidify ${\varphi}$, 20 at- tempts have been made with three different gas temperature ($50{\circ}C, 80{\circ}C, 110{\circ}C$) at different dew point. At the specific electric resistance of dust $p_e$=$10^6{\Omega}m$ which relative humidity corresponds to $\phi$ > 15%, a easy rise of the sounded plate secluded dust mass share was measured atwain. As the result of the higher cohesion imprisonment power due to the adsorbtion of particle, the rinse of the relative humidity developed on the particle surface. Therefore, the collection efficiency of mass was not predominant the high temperature T in the collector zone, neither was the pecific ellectric resistance of dust dependent.

• 대한기계학회논문집
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• 제8권2호
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• pp.145-153
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• 1984

본 연구에서는 먼저 집열기의 열성능에 관한 가장 전형적인 Hottel-Whillier- Bliss의 모델을 사용하여 모의 실험을 수행하였다. 모의 실험에 사용한 집열기의 주 요 변수는 덮개 유리의 수(N), 집열판의 방사율(.epsilon.$_{p}$), 집열판의 흡수율(.alpha.$_{p}$T),집열기 단위 면적당의 유량(G), 집열기 단열재의 $L_{b}$/ $K_{b}$, 집열기 경사각 (S),일사량(I) 등이며 이들 집열기 변수의 대표치(typical values)를 중심으로 각 변 수의 값을 변화시켜서 여기에 따른 집열기 효율 곡선의 변화를 조사하였다. 모의 실 험결과와 비교하고, 모의 실험에 사용한 수학적 모델이 집열기의 열성능을 평가하는 데에 적합한가를 확인하고, 운전중에 인위적으로 그 값을 조절할 수 있는 운전 변수중 특히 유량(G)의 변화에 따른 집열기 효율변화와 최적유량의 범위를 동시에 실험적으로 조사하기 위하여, 액체 가열식 집열기 시험장치의 회로를 보완하여 실제 태양 아래에 서 실험을 수행하였다.

• 자원리싸이클링
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• 제2권2호
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• pp.1-8
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• 1993

부선법에 의하여 폐수속에 함유되어 있는 철이온을 제거하기 위한 몇가지 효과적인 포수제와 최적 조건들을 알아본 실험의 결과를 요약하면 다음과 같다. 음이온 포수제인 sodium lauryl sulfate에 의해서 2가와 3가 철은 각각 pH 7과 6에서 효과적으로 제거되었다. 음이온 호수제인 aeropromotor 845에 의해서 2가와 3가철은 모두 pH pH 10~11영역에서, 3가철은 pH4~10영역에서 효과적으로 제거되었따. 따라서, 2가와 3가철은 2가와 3가 철이온침전점 이상으로 단순히 용액의 pH값을 조절하여 수산화철 침전으로 만든 다음 부선법에 의하여 효과적으로 제거된다고 할 수 있다. 그때의 효과적은 pH 조절제는 NaOH와 $Na_2CO_3$였고, 효과적인 포수제는 aeropromotor 845와 trimetyl dodecyl ammomum chloride 이었다.