• 한국마린엔지니어링학회:학술대회논문집
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• 한국마린엔지니어링학회 2001년도 춘계학술대회 논문집
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• pp.75-90
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• 2001

For the purpose of helping development of a GDI(Gasoline Direct Injection) engine, the in-cylinder phenomena, such as the spray behaviors and fuel distributions, unburned fuel, and flame characteristics were investigated in a single cylinder GDI engine. The GDI engine was equipped with a swirl type electronic injector and SCV(Swirl Control Valve). PLIF(Planar Laser Induced Fluorescence) system with KrF Excimer laser was used for the measurements of the fuel distributions. The effects of the injector specifications, such as the spray cone angle and the offset angle on the fuel distributions and combustion characteristics were investigated. As a result, it was found that the injected fuel spray collided with the bottom of the bowl and moved upward along the exhaust side wall of the piston bowl. This fuel vapor played a important role in the instance of spark ignition. The injector specifications has a great influence on the flame characteristics.

• 방사성폐기물학회지
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• 제9권4호
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• pp.207-217
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• 2011

UV-Vis 분광광도법과 시간분해 레이저 유도 형광분광법(TRLFS)을 이용하여 흄산의 모사 리간드로 사용한 2,6-Dihydroxybenzoate(DHB)와 U(VI)의 착물형성반응을 조사하였다. U(VI)-DHB 착물 고유의 전하이동 흡수 스펙트럼을 분석한 결과, 착물형성반응은 우라늄-리간드 비가 1:1 또는 1:2 착물을 형성하는 이중 평형반응이며, 산도에 따라 착물종의 분포가 변한다는 것을 밝혔다. 계산된 착물형성상수 (log $K_1$ and log $K_2$)는 $12.4{\pm}0.1$과 $11.4{\pm}0.1$이다. 이에 더하여, TRLFS 방법으로 조사한 결과, DHB는 U(VI) 화학종들의 형광 소광제(quencher)로서 역할을 한다는 것을 확인하였다. 특히, 확인된 U(VI) 화학종 모두(${UO_2}^{2+}$, $(UO_2)_2{(OH)_2}^{2+}$과 $(UO_2)_3(OH)_5{^+})$에서 정적 (static) 및 동적 (dynamic) 소광작용이 공존하는 것으로 관찰되었다. 시간분해 형광 스펙트럼으로부터 리간드 농도에 따른 U(VI) 화학종의 형광세기와 형광수명을 측정하였으며, Stern-Volmer 식을 이용하여 분석하였다. 결정된 정적소광계수(KS)는 ${UO_2}^{2+}$, $(UO_2)_2{(OH)_2}^{2+}$ 과 $(UO_2)_3(OH)_5+$에 대하여 각각 $4.2{\pm}0.1$, $4.3{\pm}0.1$ 과 $4.34{\pm}0.08$이다. Stern-Volmer 식을 이용한 분석 결과, 단일 또는 이중 배위자 구조(mono- and bi-dentate)의 U(VI)-DHB 착물이 모두 정적소광효과에 관여하는 바닥상태 착물임을 확인하였다.

• 대한기계학회논문집B
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• 제26권7호
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• pp.1039-1046
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• 2002

Co-flow axisymmetric laminar premixed flame of methane was used to study the influence of air temperature and $N_2$ addition on the flame structure, temperature field and emission characteristics. OH 2-D images and temperatures along the centerline were measured experimentally by PLIF and CARS techniques respectively to observe the influences of dilution and thermal effects of $N_2$ in the gas mixture. Also, the concentration of NOx was measured at each condition by gas analyser to see the suppression effect of N2 addition on NOx emissions. It was found that OH concentrations distribute widely as air temperature goes higher, while the effect of $N_2$ addition is not significant. But $N_2$ addition highly contributes to the flame front and NOx emissions which was argued to be due to the reduction of flame temperature. In accordance with experimental study, numerical simulation using CHEMKlN code was carried out to compare the temperature results with those acquired by CARS measurement, and we could find that there is good agreement between those results.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제38회 동계학술대회 초록집
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• pp.412-412
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• 2010

플라즈마는 미세 전기 소자 제작에 있어 박막의 증착, 식각, 세정등 여러 가지 공정에서 널리 사용되고 있다. 미세 소자의 선폭의 감소와 높은 생산성을 위한 웨이퍼 면적의 대형화가 진행됨에 따라 플라즈마의 균일도는 공정 수율 향상의 관점에서 중요한 요소로 그것의 계측과 공정 중 실시간 감시에 필요성이 부각되고 있다. 플라즈마에 존재하는 라디칼의 밀도, 이온의 밀도, 전자 온도 등의 웨이퍼 상에서의 공간 분포와 공정 결과물과의 상관관계에 대한 연구는 현재까지 다양하게 진행 되었으며 특히, 라디칼의 공간 분포가 공정 결과물의 균일도와 큰 상관 관계가 있는 것으로 알려져 있다. 라디칼의 농도 분포를 계측은 레이저 유도 형광법, 발광 분광법, 흡수 분광법 등을 통하여 이루어져 왔으며, 특히 발광 분광법의 경우 계측의 민감성, 편의성등을 이유로 가장 널리 사용되고 있다. 그러나 현재 까지 진행된 발광 분광법을 이용한 라디칼의 공간 분포 계측은 그 자체로 공간 분포를 계측하는 것이 아닌 플라즈마 밀도의 축 대칭성을 가정하여 Abel inversion을 적용하거나, 광섬유를 플라즈마에 직접 삽입하는 방식을 사용하기 때문에 실제 반도체 제작공정을 비롯한 미세소자 공정 플라즈마의 라디칼 밀도 분포를 실시간, 비 접촉 방식으로 계측 하는데 한계가 있다. 본 연구에서는 반도체 공정 플라즈마의 밀도 균일성 분석을 위한 공간 분해 발광 분광기를 제안한다. 기존의 발광 분광법과 비교하여 공간 분해능 향상을 위하여 직렬로 설치된 다수의 렌즈, 개구, 그리고 핀홀을 이용하였다. 공간 분해 발광 분광기의 공간 분해능을 계산하였으며, 실험을 통하여 검증 하였다. 또, HDP CVD를 이용한 $SiO_2$ 박막 증착 공정에서 산소 라디칼의 농도와 증착된 박막의 두께 분포의 상관 관계를 계측 함으로써 공간 분해 발광 분광기의 플라즈마 공정 적용 가능성 입증 하였다.

• 방사성폐기물학회지
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• 제5권3호
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• pp.189-197
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• 2007

레이저유도파열검출 기술을 이용하여 우라늄(VI) 가수분해물의 용해도를 측정하였다. 측정 용액의 우라늄 농도 범위는 $2{\times}10^{-4}{\sim}4{\times}10^{-6}\;M$, pH 범위는 $3.8{\times}7.0$, 그리고 이온 강도는 0.1 M $NaClO_4$이며, 온도는 $25.0{\pm}0.1^{\circ}C$로 유지하였다. 문헌에 제시된 가수분해 상수와 specific ion interaction theory(SIT)를 이용하여 이온 강도 I=0 일 때의 용해도 곱 (solubility product) 상수 ${\log}K^{\circ}_{sp}=-22.85{\pm}0.23$를 구하였다. 동일한 시료에 대해 흡수 및 형광 스펙트럼을 측정하여 가수분해 화학종의 존재를 확인하였다. $2{\times}10^{-4}\;M$ 우라늄 농도에서 용액 중에 존재하는 주요 가수분해 화학종은 $(UO_2)_2(OH)_2^{2+}$와 $(UO_2)_3(OH)_5^+$임을 보였다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2007년도 춘계학술대회B
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• pp.2585-2590
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• 2007

In this paper, a technique of simultaneously measuring the velocity and the temperature in micro-scale flow is proposed. This method uses particle tracking velocimetry (PTV) for measuring the velocity and laser induced fluorescence (LIF) for measuring the temperature. To measure the accurate velocity and temperature, images for PTV and for LIF are separated by using two light sources and a shutter which is synchronized with a camera. By using only one camera, measurement system can be simplified and the error from complicate optical system can be minimized. Error analyses regarding the concentrations of fluorescent dye and particle and the light source fluctuation are also conducted. It is found that the error of the temperature and the velocity highly depends on the concentration of fluorescent particles which are used for PTV. This technique is applied to the simultaneous measurement of the velocity and the temperature in the electrokinetic flow. It is found that the velocity and temperature vary with the electric field strength and the concentration of electrolyte.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집D
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• pp.54-59
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• 2001

OH radical concentration have been measured in a methane-air partially premixed flames using PLIF. Excitation lines were selected $Q_{1}(6)$ branch, (1,0) band. The system is consisted of Nd:YAG laser, dye laser and frequency doubler to make pump beam for OH radical. On the direct photographs, flame height increases as fuel flow rate and equivalence ratio increase. And on the PLIF images, OH radical is distributed from premixed flame front to nonpremixed flame front through the flame structure with all equivalence ratio. OH overall concentrations increase with equivalence ratio. At the stoichiometric equivalence ratio, the peak of OH radical concentration exists strongly near the inner cone. As equivalence ratio is changed to richer, OH radical distribution goes thinly and the peak is increased as longitudinal direction. As the flow goes to the downstream, OH radical concentration decreases and broadens, because OH radical reacts with another species after OH formation at the initial oxidization. This phenomenon resembles radial distribution. At the l00cc fuel flowrate, the radial peak of OH radical exists from x/R=l.0 to 1.5.

• 한국자동차공학회논문집
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• 제14권6호
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• pp.171-178
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• 2006

The performance in the practical combustion system including reciprocating engines and gas turbine combustors is being much governed by turbulent reacting flow that is often analyzed by both a laminar flamelets concept and flame interaction. The characteristics of laminar flame interaction have been investigated numerically to provide basic understanding of wrinkled turbulent flames under concentration interaction resulting from inhomogeneity in fuel-air mixing, especially focused on the transition of flame characteristics such as diffusion flame, partially premixed diffusion flame, and triple-layer flame by the variation in the degree of premixedness. The extinction stretch rates to the premixedness have also been obtained in this paper. The boundary defining the regime of the existence of triple-layer flames as functions of both stretch rate and premixedness has been determined which agrees well with previously reported experiment measuring OH radical concentration peaks based on PLIF.

• 한국분무공학회지
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• 제4권2호
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• pp.19-32
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• 1999

The present study investigated the forms and behaviors of fuel during intake and compression process, and the initial flame stability in a lean burn engine modified as a single cylinder engine equipped with quartz windows for visualization. PLIF(Planar Laser Induced Fluorescence) method with KrF Excimer laser was used for measuring the fuel distributions. The principal design concept of the lean burn nin in this study is the axial stratification in the fuel distribution via fuel injection during intake process and different shapes of intake ports; helical and straight. The experiments showed that fuel flowed in as a vapor state in the early part of intake process and lots of this mixture mated down along the intake valve side cylinder wall, but in the latter part, a lot of fuel flowed in as a liquid state and this fuel stayed in the upper part of cylinder, after that the dense fuel cloud moved upward in the early of part compression process. It became clear that the fuel flowed in via straight port had a important role in the axial fuel stratification.

• 대한기계학회논문집B
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• 제27권1호
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• pp.32-38
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• 2003

Staged combustion, such as air- and fuel-staging, is a relatively well-known technique fur reduction of NOx emission and used in combination with other techniques nowadays. However, the design variables are still selected depending upon operating conditions. There are many variables tested to investigate the NOx emission characteristics fur changing of fuel or air velocity, swirl intensity, and staging ratio of air and fuel in multi-staged burner. In air-staging case, the fuel-rich condition of the primary combustion zone is very helpful to reduce NOx emission and its range is known to be restricted by the increase of carbon monoxide. However, in many cases carbon monoxide level is not too high to be restricted operating condition. So we tried to expand the equivalence ratio range to the richer condition in the primary combustion zone and certificate the function of each burner component and its contribution to the overall NOx production.