• Journal of the Optical Society of Korea
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• 제13권2호
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• pp.267-271
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• 2009

The aim of this study is to evaluate wavelength dependence for laser-assisted lipolysis using a mathematical simulation. In this study, a Monte Carlo simulation was performed to simulate light transport in fat and dermal tissue with 3 different laser wavelengths (${\lambda}\;=\;1064\;nm$, 1320 nm, and 1444 nm) that are currently used in clinic settings for laser-assisted lipolysis. The relative rates of heat generation versus penetration depth showed that the greatest amount of heat generation was seen in the tissues at ${\lambda}\;=\;1444\;nm$. This Monte Carlo simulation may help lend insight into the thermal events occurring inside the fat and dermal tissue during laser-assisted lipolysis.

• 한국자동차공학회논문집
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• 제5권6호
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• pp.167-174
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• 1997

The penetration depth and the size distribution of the droplets of fuel sprays are important in the operation of spark-ignition MPI engines. A fluorescence/scattering image technique for droplet sizing was applied to measure th edroplet size distribution in non-evaporating gasoline sprays. The fluorescence and scattering lights were imaged simultaneously by the two-dimensional visualization system composed of a laser sheet, a doubling prism, optical filters, and a CCD camera. Quantitative droplet size distributions were extracted from evaluating the ratio of the two light densities. The mean droplet size measured by the fluorescence/scattering technique was compared with the result obtained by the enlarged photographs of droplets. The fluorescence/scattering image technique also gives the useful information of the characteristics of droplet impingement in a inclined wall.

• 한국레이저가공학회지
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• 제8권3호
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• pp.11-19
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• 2005

In automotive industry, light weight vehicle is one of issues because of the air pollution and the protection of environment. Therefore, automotive manufacturers have tried to adopt light materials such as aluminum alloy to production line. Aluminum welding using laser has some advantages high energy density and high productivity. It is very important to understand weld characteristic according to welding condition in order to determine the possibility of application to car body. In this study, Nd:YAG laser welding of 5182 aluminum alloy with filler wire AA5356 was carried out through experimental design according to wire feed rate, laser power and welding speed. Weld bead shape in terms of cross section photo, bead with, height of reinforcement and penetration depth and mechanical property in terms of tensile strength and formability was investigated. Analysis of variation (ANOVA) was performed to know the effect of weld parameter for weldability, laser power was statistically most significance factor of three variables.

• 한국태양에너지학회 논문집
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• 제24권2호
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• pp.39-50
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• 2004

One of the challenge for successful daylighting design might be to capture sunlighting that varies in both intensity and position and to deliver the luminous flux into the inner space as deep as possible. Conventional glazing apertures allow daylight in the outer 3.5m of a perimeter spaces. More advanced daylighting technologies can extend this daylighting depth by reflecting sunlight further from the windows within a deep floor area. For this purpose, this study developed light shelves based on performance evaluation with a mock-up model that constructed recently and measured under real sky condition. All these daylighting devices have a customized geometry developed from the solar path at a given latitude and utilize unique reflecting finishing to maximize the amount of redirection and diffusion of the daylight. This paper tells that the best daylighting penetration typically can be expected from using light-colored sloped external shelves.

• 수산해양기술연구
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• 제18권2호
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• pp.61-67
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• 1982

한국 남해에서의 해수의 광학적 성질을 조사하기 위하여, 1980년 7월에 부산에서 제주도에 이르는 10개 관측점에서 투명도, 수색, 태양광의 4가지색(Clear ; 400~720nm, Red ; 600~700nm, Green ; 475~600nm, Blue ; 400~475nm)에 대한 해수의 표면조도 및 수중조도 등을 조사한 결과를 요약하면 다음과 같다. 1. 본 조사해역의 평균투명도는 17.1m (13~25m) 였고, 평균수색은 3.9 (3~5)였다. 2. 해수의 평균흡수계수는 적색광이 0.119 (0.069~0.154), 백색광이 0.102 (0.066~0.137), 청색광이 0.095 (0.056~0.129), 녹색광이 0.091 (0.054~0.123) 순으로 적게 나타났다. 3. 해수의 흡수계수 k와 투명도 D와의 관계는 적색광이 k=2.01/D, 백색광이 k=1.71/D, 청색광이 k=1.60/D, 녹색광이 k=1.52/D 순으로 적게 나타났다. 4. 태양광선의 표면광에 대한 평균 해중 투과율은 녹색광(수심 5m층에서 60.9%, 15m층에서 24.51%, 30m층에서 7.11%, 50m층에서 1.56%), 청색광(수심 5m층에서 59.4%, 15m층에서 22.92%, 30m층에서 6.09%, 50m층에서 1.29%), 백색광(수심 5m층에서 57.3%, 15m층에서 20.82%, 30m층에서 5.16%, 50m층에서 0.94%), 적색광(수심 5m층에서 52.2%, 15m층에서 15.99%, 30m층에서 2.99%, 50m층에서 0.39%)의 순으로 적게 나타났다.

• 한국수산과학회지
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• 제13권3호
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• pp.95-101
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• 1980

1977년 5월 부터 8월 사이와 11월에서 12월까지의 6개월간 매월 한국 남해안의 활멸치어장을 중심으로 한 7채 관측점에서 투명도, 수색, 태양고도, 태양광선에 대한 해수의 표면조도 및 수심별 해중조도 등을 조사한 결과를 요약하면 다음과 같다. 1. 본 조사해역의 평균투명도는 $8.4m(2.6\~16m)$였고, 월별 평균투명도는 8월(11.4m), 6월(9.1m), 7월(9m), 5월(7.9m), 12월(6.7m), 11월(6.3m)순으로 낮게 나타났다. 2. 평균수색은 $4.8(3\~10)$이였고, 월별 평균수색은 8월(4.1), 6월과 7월(4.6), 5월(4.7), 11월(5.3), 12월(5.6) 순으로 낮게 나타났다. 3. 해수의 평균흡수계수는 $0.21(0.066～0.619)$이였고, 월별 평균흡수계수는 11월(0.25), 5윌(0.23), 7월과 12월(0.22), 5월(0.16), 6월(0.15)순으로 적게 나타났다. 4. 해수의 흡수계수 k와 투명과 D와의 관계는 k=1.70/D로 나타났다. 5. 태양광선의 평균해중투적률은 수심 1m층에서 표면광의 $69.38\%(25.45\~88.1\%)$, 5층에서는 $30.35\%(4.38\~59.46\%)$, 10m층에서는 $12.53\%(0.75\~33.51\%)$, 15층에서는 $5.7\%(0.18\~20.27\%)$의 투과율을 보였다. .6 투명도층에서의 탱양광선의 평균투과율은 표면광의 $16.18\%(6.96\~23.48\%)$로 나타났다.

• 수산해양기술연구
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• 제17권2호
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• pp.53-58
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• 1981

제주도 북서해역에서의 해수의 광학적 성질을 조사하기 위하여, 1980년 7월에 제주도에서 소흑산도에 이르는 7개 관측점에서 투명도, 수색, 태양광의 4가지색(Clear; 400~720nm, Red; 600~700nm, Green; 475~600nm, Blue; 400~475nm)에 대한 해수의 표면조도 및 수중조도 등을 조사한 결과를 요약하면 다음과 같다. 1. 본 조사해역의 평균투명도는 16.1m(11~19m)였고, 평균수색은 4.3(3~5)였다. 2. 해수의 평균흡수계수는 적색광이 0.135(0.106~0.184), 백색광이 0.106(0.084~0.152), 청색광이 0.097(0.073~0.136), 녹색광이 0.089(0.069~0.130)순으로 적게 나타났다. 3. 해수의 흡수계수 k와 투명도 D와의 관계는 적색광이 k=2.12/D, 백색광이 k=1.66/D, 청색광이 k=1.15/D, 녹색광이 k=1.38/D 순으로 작게 나타났다. 4. 태양광선의 표면광에 대한 평균해중투과율은 녹색광(수심 5m층에서 62.29%, 15m층에서 26.43%, 30m층에서 7.74%, 50m층에서 1.56%), 청색광(수심 5m층에서 59.29%, 15m층에서 23.43%, 30m층에서 6.10%, 50m층에서 1.08%), 백색광(수심 5m층에서 56.57%, 15m층에서 20.54%, 30m층에서 4.60%, 50m층에서 0.68%), 적색광(수심 5m층에서 50.14%, 10m층에서 14.29%, 30m층에서 2.37%, 50m층에서 0.23%)의 순으로 적게 나타났다. 5. 투명도층에서의 태양광의 평균해중투과율은 녹색광이 표면광의 24.3%(20~25.8%), 청색광이 21.21%(17.3~24%), 백색광이 18.29%(15.5~20%), 적색광이 12.4%(10.3~15%)의 순으로 적게 나타났다.

• 공업화학
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• 제21권4호
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• pp.401-404
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• 2010

GDC (Gadolinium doped ceria) 펠렛에 120 keV 및 5 MeV 에너지의 양성자 또는 제논 이온을 주입하였으며, 그 영향을 UV-vis 분광계, SEM 및 XRD를 이용하여 측정하였다. GDC 펠렛은 cubic fluorite 구조를 갖는 조밀한 소결체였으며, 갈색이었던 펠렛이 이온빔을 조사한 후 옅은 검은색을 띠기 시작하였으며, fluence가 증가함에 따라 색도 짙어졌다. XRD 패턴은 이온의 에너지 및 X선의 투과 깊이와 밀접한 관계가 있었으며, 120 keV의 양성자 빔을 조사한 표면 바로 아래층은 이온의 주입으로 결정 구조는 유지한 채 격자 상수가 증가하였다는 것을 관찰하였다.

• 한국세라믹학회지
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• 제33권2호
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• pp.242-250
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• 1996

Glasses of Na2O-Al2O3-SiO2 system were prepared and ion-exchange characteristics change of properties and bactericidal effects by Na+↔Ag+ ion exchange were studied. Parent glasses with three compositions of varying Na2O in the 20~30 wt% were ion-exchanged in the molten salt of 2 mol% AgNO3+98 mol% NaNO3 at 320~36$0^{\circ}C$ for 15~16min. Amount of ion exchange and penetration depth of Ag+ ion increased with Na2O content in the parent glass ion exchange temperature and time. After ion exchange densities and Vickers hardness of the glasses increased and the glasses showed yellow-brown color and as amount of ion exchange increased the color turned deep because partial reduction and agglomeration of Ag+ into Ag0 results in absorption of visible light. After ion exchange chemical durability of the glass to wter was enhanced compara-bly that weight loss and change of surface of the glass were not found for the leaching test in 5$0^{\circ}C$ K.I water for 240hrs. Bactericidal effect of ion exchanged glass on Staphylococcus aureus and E. coli was determined by microorganism test and bactericidal effect increased with amount of ion exchange and incubation time.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2005년도 춘계학술대회 논문집 디스플레이 광소자 분야
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• pp.92-95
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• 2005

The silver photodoping effect in amorphous AsGeSeS chalcogenide thin films for holographic recording has been investigated using a HeNe laser ($\lambda$=632.8 nm). The chalcogenide films prepared in this work were thinner in comparison with the penetration depth of recording light ($d_p$=1.66 mm). The variation of the diffraction efficiency $(\eta)$ in amorphous chalcogende films exhibits a tendency, independently of the Ag photodoping. That is, n increases relatively rapidly at the beginning of the recording process, reaches the maximum $({\eta}_{max})$ and slowly decreases. In addition, the value of ${\eta}_{max}$ depends strongly on chalcogenide film thickness(d) and its peak among the films with d = 40, 80, 150, 300, and 633 nm is observed at d = 150 nm (approximately 1/2n), where n is refractive index of the chalcogenide (n=2.0). The ${\eta}$ is largely enhanced by Ag photodoping into the chalcogenides. In particular, the value of hmax in a bilayer of 10-nm-thick Ag/150-nm-thick AsGeSeS film is about 1.6%, which corresponds to ~20 times in comparison with that of the AsGeSeS film (without Ag).