• Membrane Journal
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• v.22 no.2
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• pp.142-154
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• 2012

In order to remove $CO_2$ from the DME plant process, we investigated the composite membrane with rubbery polymers as the separation layer and its separation performance of $CO_2$ and $H_2$. Hollow fiber membranes for supporting layer were prepared by solution spinning method. In case of using PDMS as a separation layer, the composite membranes showed the permeation rates of $CO_2$ were over 300 GPU and minimum $CO_2/H_2$ selectivitties were 4.3 and in case of using PEBAX as a separation layer, the composite membranes showed the permeation rates of $CO_2$ were over 120 GPU and minimum $CO_2/H_2$ selectivities were 5.

• Proceedings of the Korean Vacuum Society Conference
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• 2016.02a
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• pp.215.1-215.1
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• 2016

플라즈마는 반도체, 디스플레이, 태양전지 등 다양한 산업 분야에 이용된다. 플라즈마 공정 시 수율 향상을 위해 플라즈마를 진단하는 기술이 필요한데, 대표적으로 전자온도가 있다. 반도체 공정의 낮은 압력과 높은 밀도의 플라즈마에서 전자온도는 1~10 eV 정도인데, 0.5 eV정도의 아주 적은 차이로도 공정 결과에 큰 영향을 미친다. 플라즈마의 전자온도를 측정하는 방법은 전기적 탐침 방법인 랑뮤어 탐침(Langmuir Probe)과 와이즈 프로브(Wise Probe)를 이용한 방법, 그리고 광학적 방법인 방출분광법(OES : Optical Emission Spectroscopy)이 있다. 전기적 탐침 방법은 직접 플라즈마 내부에 탐침을 넣기 때문에 불활성 기체를 사용한 공정에서는 잘 작동하지만 건식식각이나 증착에 사용할 경우 탐침의 오염으로 인한 오동작, 공정 시 생성된 샘플에 영향을 줄 수 있다는 단점이 있다. 반면에 방출분광법은 광학적 진단으로, 플라즈마를 사용하는 공정 진행 중에 외부에 광학계를 설치하여 플라즈마에서 발생하는 빛을 광학적으로 분석하기 때문에 공정에 영향을 미치지 않고, 공정 장비에 적용이 쉬운 장점을 가지고 있다. 본 연구에서는 RF Power를 인가한 유도결합플라즈마(ICP : Inductively Coupled Plasma) 공정에서 아르곤 가스와 산소 혼합가스 분압과 인가전압을 변화시켜 플라즈마 방출광 세기 변화에 따른 전자온도를 측정하였다. 전자온도 측정에는 전기적 방법인 랑뮤어 탐침, 와이즈 프로브를 이용한 방법과 광학적 방법인 방출분광법을 사용하여 측정하였으며 이를 비교 분석하였다.

• Transactions of the Korean Society of Mechanical Engineers B
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• v.27 no.8
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• pp.1051-1060
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• 2003

The heat and mass transfer on two kinds of tube surfaces (bare stainless steel tube and Teflon coated tube) in steam-air mixture flow are experimentally studied to obtain design data for the heat exchanger of the latent heat recovery from flue gas. In the test section, 3-tubes are horizontally installed, and steam-air mixture is vertically flowed from the top to the bottom. The pitch between tubes is 67mm, the out-diameter of tube is 25.4mm, and the thickness is 1.2mm ; blockage factor (cross sectional tube area over the cross sectional area of the test section) is about 0.38. All of sensors and measurement systems (RTD, pressure sensor, flow-meter, relative humidity sensor, etc.) are calibrated with certificated standard sensors and the uncertainty for the heat transfer measurement is surveyed to have the uncertainty within 7%. As experimental results, overall heat transfer coefficient of the Teflon (FEP) coated tube is degraded about 20% compared to bare stainless tube. The degradation of overall heat transfer coefficient of Teflon coated tube comes from the additional heat transfer resistance due to Teflon coating. Its magnitude of heat transfer resistance is comparable to the in-tube heat transfer resistance. Nusselt and Sherwood numbers on Teflon (FEP) coated surface and bare stainless steel surface are discussed in detail with the contact angles of the condensate.

• Journal of Power System Engineering
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• v.13 no.6
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• pp.13-21
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• 2009

This basic study is required to examine spray or jet behavior depending on fuel phase. In this study, analyses of diesel fuel(n-Tridecane, $C_{13}H_{28}$) spray and natural gas fuel(Methane, $CH_4$) jet under high temperature and pressure are performed by a general-purpose program, ANSYS CFX release 11.0, and the results of these are compared with experimental results of diesel fuel spray using the exciplex fluorescence method. The simulation results of diesel spray is analyzed by using the combination of Large-Eddy Simulation(LES) and Lagrangian Particle Tracking(LPT) and of a natural gas jet is analyzed by using Multi-Component Model(MCM). There are two study variables considered, that is, ambient pressure and injection pressure. In a macroscopic analysis, the higher ambient pressure is, the shorter spray or jet tip penetration is at each time after start of injection. And the higher injection pressure is, the longer spray or jet tip penetration is at each time after start of injection. When liquid fuel is injected, droplets of the fuel need some time to evaporate. However, when natural gas fuel is injected, the fuel does not need time to evaporate. Gas fuel consists of minute particles. Therefore, the gas fuel is mixed with the ambient gas more quickly at the initial time of injection than the liquid fuel is done. The experimental results also validate the usefulness of this analysis.

• Journal of the Korean Ceramic Society
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• v.39 no.3
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• pp.272-277
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• 2002

Aluminum nitride (AlN) powders and whiskers were synthesized by a modified carbothermal reduction and nitridation where a ($NH_4)[Al(ethylenediaminetetraacetate)]{\cdot}2H_2O$ complex is used as precursor. The AlN powders were obtained by calcining the complex without mixing any carbon source under a flow of nitrogen in the temperature range 1200∼1500$^{\circ}$C and then burning out the residual carbon. The nitridation process was investigated by $^{27}Al$ magic-angle spinning (MAS) unclear magnetic resonance, infrared spectroscopy and X-ray diffraction. The complex is pyrolyzed, converted to ${\rho}$- and ${\gamma}$- alumina and then nitridated to AlN without ${\gamma}-{\alpha}$ alumina transition. The morphology of ${\gamma}$-alumina, when it was converted to AlN, was retained, strongly indicating that ${\gamma}$-alumina is converted to AlN through solid-state $AlO_xN_y$, not through gaseous intermediates such as aluminum and aluminaum suboxides. AlN whiskers were obtained, when a (0001) sapphire was used as a catalyst.

• Transactions of the Korean Society of Mechanical Engineers B
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• v.36 no.10
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• pp.989-999
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• 2012

An ejector is a fluid transportation device that operates based on the principle that a high-pressure fluid is spouted through a driving pipe and the pressure of a low-pressure fluid is increased through exchange of momentum with a low-pressure gas. Steam-steam ejectors have been widely used for suction, mixture, and dehydration. They can be easily used in places where fluid moves and expenses are reasonable. In addition, such ejectors are a semi-permanent fluid device that requires little maintenance. In this study, we present an optimized design by analyzing what cannot be obtained through experiments in order to improve the device performance, analyze general contents of a flow by acquiring exact test data on specific and interpretative areas using more advanced experimental techniques, and identify the flow characteristics of a branch pipe by examining the validity of experiments using computer hydrodynamics simulations.

• Applied Chemistry for Engineering
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• v.7 no.5
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• pp.992-998
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• 1996

The $La_{0.8}Ca_{0.2}CoO_3$ prepared by a citrate process was shown to have higher oxygen reduction current density and specific activity than $LaCoO_3$, $La_{0.6}Ca_{0.4}CoO_3$. In the cyclic voltammogram, an oxygen desorption peak of a $La_{0.8}Ca_{0.2}CoO_3$+carbon electrode was larger than that of a only carbon electrode. $La_{0.8}Ca_{0.2}CoO_3$ sintered at $900^{\circ}C$ for 5 hours was shown high oxygen reduction current density because of the particle size distribution and sintering effect.

• 한국신재생에너지학회:학술대회논문집
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• 2011.05a
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• pp.146.1-146.1
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• 2011

석탄가스화복합발전(IGCC)공정에서 가스화기를 거쳐 생성된 합성가스로부터 $CO_2$를 효과적으로 분리/회수하기 위해 가스 고형화법을 제안하였다. 가스 하이드레이트 형성과정에서의 반응특성을 살펴보기 위하여 반응시간에 따른 가스소모량과 기상의 $CO_2$ 조성 변화를 측정하였다. 순수계와 촉진제 첨가계 (TBAB (10, 40 wt%), TBAF (10, 34 wt%), THF (4, 19 wt%))에 대하여 하이드레이트 생성 후의 기상과 하이드레이트상의 $CO_2$ 조성을 측정하였으며, 그 결과 하이드레이트 형성법에 의해 고농도의 $CO_2$가 하이드레이트상에 포집되는 것을 확인하였다. 가스 소모량 측정실험에서는 THF 19.1 wt%를 첨가하였을 때 가장 큰 소모량을 보였으며, TBAF 10 wt%를 첨가하였을 때 가장 적은 가스소모량을 보였다. $CO_2$ 조성 변화 실험에서는 가스 소모량 실험과 마찬가지로 THF 19.1 wt%를 첨가하였을 때 가장 큰 조성변화를 보였다. 이는 THF의 첨가로 인하여 가스 하이드레이트로의 전환율 증가로 많은 양의 $CO_2$ 기체가 하이드레이트 상에 포집되었음을 나타낸다. 속도론적인 측면에서는 모든 실험조건에서 하이드레이트 형성반응이 1시간 이내에 대부분 종결되는 것을 볼 수 있었다. 또한 $^1H$-NMR을 통하여 혼합가스 하이드레이트의 구조적인 분석을 진행하였다. 본 실험에서 얻어진 결과는 가스 하이드레이트 형성법을 이용한 합성가스 분리 공정 개발에 중요한 기초자료가 될 것으로 사료된다.

• Analytical Science and Technology
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• v.5 no.4
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• pp.425-431
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• 1992

The concentration and determination of trace phosphate ion was studied by $La(OH)_3$ coprecipitaiton. Phosphate ions in 1.0L samples were coprecipitated with lanthanium hydroxide at pH 9.5 adjusted with ammonia solution. The precipitates were floated with the aid of mixed surfactant(1:8 sodium oleate/sodium dodecyl sulfate) and nitrogen gas bubbles. The floated precipitate was collected in suction flask from the solution. The precipitate were washed with dil. ammonia solution and dissolved in sulfuric acid. The phosphate ion in the concentrated solution was finally determinated by UV/VIS spectrophotometry using the molybdenium blue method. The proposed method could be applied to the determination of phosphate ion in tap water and river water.

• Journal of Korean Society of Environmental Engineers
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• v.27 no.6
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• pp.614-619
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• 2005

The activated carbon fibers of different surface area and pore structures were modified by carbon deposition from the pyrolysis of benzene, in an attempt to obtain carbon molecular sieves of high adsorption capacity and selectivity for the separation of $CO_2/CH_4$ gas mixtures. The ACFs molecular sieves prepared from different temperature and time were tested by the static adsorption of $CO_2$ and $CH_4$ gas, and their pore structures were characterized by the $N_2$ adsorption isotherms. We are able to prepare ACF molecular sieve with good selectivity for $CO_2/CH_4$ separation and showing acceptable adsorption capacities from the change of porosity by carbon deposition of pyrolyzed benzene.