• Journal of Mechanical Science and Technology
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• 제16권2호
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• pp.270-278
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• 2002

In order to reduce the exhaust emissions of a spark ignition engine, it is important not only to improve the catalyst conversion efficiency, but also to directly reduce the engine-out exhaust emissions during a cold starting of the engine and warm up periods. The purpose of this study is to evaluate feasibility of a glow plug for an early fuel evaporator. In order to promote atomization, gasoline is injected on the glow plug with room temperature(20$\^{C}$) and high temperature(250$\^{C}$). To analyze the spray behavior characteristics, a PMAS is used to measure the SMD and the dropsize distribution of an impinging spray and a free spray. Results show that the evaporation rate of the impinging spray on the high temperature surface of the glow plug was higher than that of the free spray on the room temperature surface.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2008년도 추계학술대회A
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• pp.1869-1873
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• 2008

In this work, to make it possible to generate glow discharge in atmospheric pressure condition with relatively high and wide electric field, micro channel reactor is proposed. Si DRIE and Cr deposition by Ebeam evaporation is used to make channel and bottom electrode layer. Upper electrode is made from ITO glass to visualize discharge within micro channel. Fabricated reactor is verified by generating uniform glow plasma with N2 / He gases each as working fluid. The range of gas electric field to generate glow plasma is from about 200 V/cm and upper limit is not observed in tested condition of up to 150 kV/cm. This data shows that micro channel plasma reactor is more versatile. Indirect estimation of electron temperature in this reactor can be inferred that the electron temperature within glow discharge in micro reactor lies $0{\sim}2eV$. This research demonstrates that the reactor is appropriate in application that needs to maintain low temperature condition during chemical process.

• Nuclear Engineering and Technology
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• 제6권1호
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• pp.3-8
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• 1974

천연 녹주석의 방사선조사에 의한 효과를 없애기 위한 열처리방법을 연구하였다. Glow곡선분석에서 최적열처리시간과 온도는 145$0^{\circ}C$에서 1시간이었고, 녹주석을 다시 사용할 시에는 145$0^{\circ}C$에서 1시간동안 열처리를 다시 할 필요는 없고 55$0^{\circ}C$에서 1시간만 열처리를 하면 된다. 145$0^{\circ}C$에서 열처리된 녹주석시료를 $^{60}$Co감마선으로 100R 조사한 후 glow곡선을 그려보니 $65^{\circ}C$와 20$0^{\circ}C$에서 glow peaks를 발견하였다. $65^{\circ}C$ glow peak는 곧 없어졌으나 20$0^{\circ}C$ glow peak는 매우 안정하였다. 따라서 열형광방사선측정에는 20$0^{\circ}C$ glow peak를 이용하여 $^{60}$Co감마선을 측정할 수 있다.

• Preventive Nutrition and Food Science
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• 제6권1호
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• pp.23-28
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• 2001

A study was carried out to establish a detection method of irradiated shellfish through thermoluminescence (TL). The TL intensity of first glow curves for irradiated bloody, freshwater, and short-neck shellfish increased from control until 5 kGy and increased slightly room 5 kGy until 10 kGy. Maximum TL temperatures of all irradiated samples tested were below 23$0^{\circ}C$, within temperature interval of 150~25$0^{\circ}C$ recommended for evaluation. Since just in control, glow curve ratios of G3 and G4 calculated from re-irradiated (1 kGy) bloody, freshwater and shortneck were over 0.5, detection in control was possible. However, as glow curve ratios after three months were below 0.5, detection by glow curve ratios after three months was impossible. Gl, which calculated from unirradiated samples, exhibited below 0.1, they were classified as unirradiated. In all samples, all the irradiated shellfish could be classified correctly as irradiated by hemaximum TL temperatures and shape of the second glow curve because those were shown in a lower temperature region than those of the first glow curve.

• 한국자동차공학회논문집
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• 제10권1호
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• pp.84-92
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• 2002

On the cold start of LPG engine, as the engine temperature has not reached its equilibrium temperature, liquid LPG could not be changed perfectly gaseous LPG, although it was passed to the vaporizer. Liquid and gas mixed fuel could influence starting ability and exhaust emission characteristics of LPG engine. In this study, the vaporization characteristic of liquid LPG was investigated with a conventional vaporizer and the vaporizer with heat source(glow plug) installed at preheated chamber inlet, by using the visualization methods and engine test. According to visualization result, even if the engine coolant temperature was $14^{\circ}C$, liquid fuel was supplied to primary chamber over 25 seconds without vaporizing from preheated chamber in such a conventional vaporizer. However, the vaporizer with heat source do not correspond with that, scarcely had been trim on glow plug when LPG began to vaporize. The effectiveness of heat source could be verified by application to the conventional LPG engine.

• 한국방사선학회논문지
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• 제8권4호
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• pp.181-187
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• 2014

본 연구는 방사선 치료 영역의 선량 측정을 위하여 상용화된 열형광선량계의 가열 온도에 따른 형광 곡선의 특성을 분석하였다. 본 연구에 사용된 열형광선량계는 LiF:Mg${\cdot}$Ti, LiF:Mg${\cdot}$Cu${\cdot}$P, $CaF_2$:Dy, $CaF_2$:Mn(Thermo Fisher Scientific Inc., USA)이었다. 선원과 고체 팬텀 표면(RW3 slab, IBA Dosimetry, Germany)간 거리를 100cm로 하여 기준점 깊이에서 6MV, 15MV X선과 6MeV, 12MeV 전자선을 각각 100MU 조사하였다. 방사선 조사 후 열형광 판독기(Hashaw 3500, Thermo Fisher Scientific Inc., USA)를 사용하여 $50^{\circ}C$에서 $260^{\circ}C$까지 $15^{\circ}C/sec$의 가온율로 가열하여 형광 곡선을 분석하였다. 트랩 준위에 포획된 전자가 정공과 결합하면서 빛을 방출하는 형광 피크(glow peak)는 2개 또는 3개의 피크가 나타났으며 방사선 조사 후 TLD의 온도를 일정하게 증가시켰을 때 최대 형광 피크를 나타내는 형광 온도의 경우 각각의 에너지에 따라 $LiF:Mg{\cdot}Ti$ 선량계는 $185.5{\pm}1.3^{\circ}C$, $LiF:Mg{\cdot}Ti$ 선량계는 $135.0{\pm}5.1^{\circ}C$, $CaF_2$:Dy 선량계는 $144.0{\pm}1.6^{\circ}C$, $CaF_2$:Mn 선량계는 $294.3{\pm}3.8^{\circ}C$ 근처에서 최대 형광 피크를 각각 나타났다. 방사선 조사 후 포획 전자의 형광 방출 확률은 가열 온도에 의존하게 되므로 방사선 치료 영역의 선량 측정에서 방사선 조사 후 열형광선량계에 일정한 가온율을 적용함으로써 고유한 물리적 특성에 따른 측정 정확도를 향상시킬 수 있을 것으로 판단되었다.

• 센서학회지
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• 제8권5호
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• pp.388-393
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• 1999

회토류 원소인 Eu로 활성화한 $CaSO_4:Eu$ TLD를 제작하였으며, 트랩 매개변수 등의 물리적 특성을 조사하였다. 제작한 $CaSO_4:Eu$ TLD는 활성제 Eu의 농도를 0.5 moi%로 하고, $600^{\circ}C$에서 2시간 동안 열처리하였을 때 최대의 열형광 강도를 나타내었으며, glow 곡선은 2개의 glow peak로 구성되었다. 두 glow peak를 분리하여 초기 상승법, peak 형상법, 가온율법, 최소자승법에 의한 glow 곡선의 fitting 방법 등을 사용하여 glow 곡선을 분석하였다. 두 glow peak의 활성화에너지는 각각 1.00 eV, 1.09 eV이고, 진동수인자는 각각 $7.04{\times}10^{11}\;s^{-1}$과 $5.12{\times}10^{11}\;s^{-1}$였으며, 1.11과, 1.33의 발광차수를 갖는 것으로 평가되었다.

• 한국안광학회지
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• 제6권1호
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• pp.149-153
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• 2001

LiF:Mg, Cu, Na, Si TL 물질의 열자극발광을 온도대 파장대 발광강도의 3차원으로 측정하여 분석하였다. 온도대 발광강도곡선(glow curve)은 각 온도에서 파장별 발광강도데이터를 적분하여 구성하였고, 이를 분석하여 트랩에 관계되는 여러가지 파라미터들을 결정하였다. 발광곡선의 분석은 일반차 모델의 TL 강도 표현식을 기본함수로 하여 컴퓨터화된 발광곡선 분해(Computerized Glow Curve Deconvolution: CGCD)기법을 이용하였고, 그 결과 LiF:Mg, Cu, Na, Si TL 물질의 열자극발광곡선은 정점온도 333 K, 374 K 426 K, 466 K, 483 K 그리고 516 K를 갖는 6개의 개별적인 발광곡선들로 구성되어 있음을 확인하였다. 주 피크(main peak)인 456 K 발광곡선에 대하여 활성화에너지는 2.06 eV, 발광차수는 1.05로 밝혀졌다. 발광스펙트럼 분석결과 LiF:Mg, Cu, Na, Si TL 물질은 3개의 재결합준위 1.80 eV, 2.88 eV 그리고 3.27 eV를 가지는 것으로 판명되었다. 이 중 약 2.88 eV 준위가 지배적이고 다음으로 3.27eV 준위에서 발광이 일어나며 1.80 eV 준위는 극히 미약하나 분명한 존재를 확인하였다.

• 한국염색가공학회지
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• 제26권3호
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• pp.201-208
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• 2014

The high value-added functionality for synthetic fiber can be considered through a plasma enhanced treatment. In this study, PET(Polyethyleneterephthalate) was treated with a glow plasma and corona treatment. Surface characteristics of treated fabric were investigated using electron scanning microscopy(SEM), contact angle, X-ray photoelectron spectroscopy(XPS), tensile and adhesion strength. It was found that the contact angle showed $85.5^{\circ}$ for untreated fabric, $0^{\circ}$ for plasma and corona treatment at the condition of 200W for 7min. By XPS analysis, atomic ratio of O 1s/C 1s was increased from 0.27 to 0.43 by glow plasma and 0.27 to 0.41 by corona treatment at 200W for 7min, respectively. Glow plasma and corona treatment did not significantly change the tensile strength of PET fabric. Adhesion strength showed a substantial enhancement for the surface treated with the glow plasma, while corona treatment was adversely affected.

• 대한전기학회논문지
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• 제43권3호
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• pp.478-484
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• 1994

Facing target dc sputtering system developed by Hoshi et al. has simple configuration and high deposition rate under moderate substrate temperature in the range of pressure 5x10S0-4T - 1x10S0-2T torr. In this system, magnetic field should be applied perpendicular to the target surface in order to confine high energy secondary electrons between two targets. Because of this magnetic field, the glow discharge characteristics are very different from dc planar diode system showing some unstable discharge region. In this paper, the glow discharge characteristics of this system have been studied under the condition of Ti targets with Ar-NS12T(10%) as working gas. It is found that this system has stable discharge region under the discharge current density of 15-30(mA/cmS02T). The plasma density and electron temperature are in the range of 10S010Y - 10S011T(CMS0-3T) and 2.5-5(eV), respectively.