• 한국식품영양학회지
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• 제29권5호
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• pp.670-676
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• 2016

서기 530년부터 1950년까지의 고조리서 32권에 수록된 장 만드는 방법 중 메주 만드는 방법을 언급한 225가지 중 재료의 가열방법, 메주의 형태, 메주를 띄우는데 사용하는 용기, 덮개 및 깔개를 분석하였다. 그 결과 전통 메주의 콩이나 전분질의 가열 방법은 찌기 57가지, 삶기 58가지, 볶아 삶기 21가지, 밥짓기 2가지의 순으로 나타났다. 메주의 형태는 알 41가지, 구형 27가지, 덩어리 22가지, 칼자루형 8가지, 납작형 6가지, 쪼가리형 4가지, 구멍형 1가지, 사각형 1가지의 순으로 나타났다. 고추장 메주 72가지 중 콩 가열 방법은 삶기 9가지, 찌기 6가지의 순이었고, 전분질의 가열방법은 떡찌기 19가지, 밥 짓기 11가지, 익반죽 삶기 5가지의 순으로 나타났다. 콩메주 띄우는 용기는, 가마니 섬 섶 49가지, 독 5가지, 둥구미 멱서리 14가지, 온돌 11가지, 소쿠리 채반 광주리 7가지, 독 5가지, 흙도랑 4가지, 시루 오쟁이 3가지, 바가지 2가지, 시루 2가지, 용수 1가지의 순으로 나타났다. 메주 띄우기용 덮개나 깔개는 짚 36가지, 닥나무잎 17가지, 멍석 거적 자리 15가지, 쑥 14가지, 솔잎 11가지, 콩잎 10가지, 도꼬마리잎 6가지, 북나무잎 6가지, 보릿짚 6가지, 뽕잎 6가지, 가랑잎 5가지, 띠풀 5가지, 삿자리 4가지, 헝겊 3가지, 개오동나무잎 2가지, 갈잎 1가지의 순으로 나타났다. 매달기는 5가지 밖에 없었다.

• 한국해양학회지:바다
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• 제10권1호
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• pp.100-112
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• 2005

갯벌의 온도구조와 열적 특성변화를 조사하기 위해 서해안 공소만 갯벌조간대에서 고도가 다른 3개 지점을 설정하여 40 cm깊이까지 계절별로 1개월간의 온도관측을 수행하였다. 표층에서 평균온도는 하계에 아래층보다 높고 동계에는 낮아져 표층가열과 냉각에 의한 온도구조와 변화 형태를 보여주었으며 표준편차는 아래층으로 갈수록 감소하였다. 주기성이 뚜렷한 일사량과 조위 변화가 주로 단기적 온도변화를 야기하였고, 간헐적으로는 강우와 강한 풍속도 영향을 주었다. 시계열분석에 의하면 24시간, 12시간 그리고 8시간 주기 성분에 강한 에너지 첨두(peak)를 보였으며, 24시간 주기성분이 가장 큰 에너지를 보였다. 24시간 주기 성분은 일사량변화, 12시간 주기는 반일주조 조위변화 그리고 8시간 주기성분은 일사량과 조위변화의 상호작용에 의한 온도파동으로 해석되었다. EOF분석에서 제 1모드와 제 2모드가 수직온도구조 변화의 96%를 차지하였다 제 1모드는 갯벌 표층에서의 가열과 냉각에 의한 현상으로, 제 2모드는 갯벌내부의 열 전파과정에서 발생하는 지연효과로 해석되었다. 교차스펙트럼 분석에서 24시간 주기성분 온도파동에 의한 열전달위상은 깊이에 따라 선형적으로 증가하는 평균위상 차이를 보였고, 표층에서 10 cm, 20 cm, 40 cm 깊이까지의 위상 차이에 의한 지연시간은 각각 3.2시간, 6.5시간 9.8시간이었다. 일차원적 열확산모델에서 산출된 24시간 주기성분 온도파동의 수직 확산계수는 깊이와 계절에 걸쳐 평균하였을 때 중부조간대 정점에서는 $0.70{\times}10^{-6}m^2/s$, 하부조간대 정점에서는 $0.57{\times}10^{-6}m^2/s$의 값을 보였다. 깊이 평균된 확산계수는 봄철에 크고 여름철에 작았고, 계절 평균된 확산계수는 2cm부터 10cm깊이까지 증가하고 10cin부터 40cm깊이까지는 감소하는 수직구조를 보였다. 평균 열확산계수를 사용하여 구한 온도전파 확산속도는 2 cm 깊이로부터 10 cm, 20cm, 40cm까지 각각 $8.75{\times}10^{-4}cm/s,\;3.8{\times}10{-4}cm/s,\;1.7{\times}10^{-4}cm/s$정도의 값이 되어 표층에서 깊어질수록 작아졌다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2003년도 춘계학술대회
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• pp.1966-1971
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• 2003

Matching inviscid and boundary layer methods are developed for hypersonic flow with thick boundray layer. The new equations match all the boundary layer properties with a variation in the inviscid solution near the edge, except for the normal velocity. Computational comparison are performed for incompressible and compressible flows over a flat plate. Results from the present method are compared with Navier-Stokes solutions. The present results are in good agreement with Navier-Stokes solutions. They show that the new technique can provide improved heating rates and skin friction predictions for preliminary design of vehicles where shear layers and entropy layer swallowing are important.

• 한국군사과학기술학회지
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• 제7권3호
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• pp.165-173
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• 2004

Matching inviscid and boundary layer methods are developed for analysis of hypersonic flow with thick boundary layer. The new equations match all the boundary layer properties with a variation in the inviscid solution near the edge, except for the normal velocity. Computational comparison are peformed for incompressible and compressible flows over a flat plate. Results from the present method are compared with Wavier-Stokes solutions. The present results are in good agreement with Wavier-Stokes solutions. They show that the new technique can provide improved predictions of heating rates and skin friction predictions for preliminary design of vehicles where shear layers and entropy layer swallowing are importantfor for preliminary design.

• Journal of Welding and Joining
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• 제15권6호
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• pp.32-40
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• 1997

Solid state diffusion bonding is the joining process performed by creep and diffusion, which is accelerated by heating below melting temperature and proper pressing, in vacuum or shielding gas atmosphere. By this process we can obtain sufficient joint which can't be expected from the fusion welding. For Ti-6Al-4V alloy, the optimum solid state diffusion bonding condition and mechanical properties of the joint were found, and micro void morphology at bond interface was observed by SEM. The results of tensile test showed sufficient joint, whose mechanical properties are similar to that of base metal. 850$^{\circ}$C, 3MPa is considered as the optimum bonding condition. Void morphology at interface is long and flat at the initial stage. As the percentage of bonded area increases, however, small and round voids are found. Variation of void shape can be explained as follows. As for the void shrinkage mechanism, at the initial stage, power law creep is the dominant, but diffusion mechanism is dominant when the percentage of bonded area is increased.

• 한국태양에너지학회 논문집
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• 제23권4호
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• pp.55-61
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• 2003

Heat transfer characteristics for an air jet vertically impinging on a flat plate with a set of hybrid rods was investigated numerically using the RNG k-$\varepsilon$turbulent model. A commercial finite-volume code FLUENT is used. The rods had cross sections of half circular and rectangular shapes. The heating surface was heated with a constant heat flux value of $1020W/m^2$. Parameters investigated were the jet Reynolds number, nozzle -to-plate spacing, the rod pitch and rod-to-plate clearance. The local and average Nusselt number were found to be dependent on the rod pitch and the clearance because installing rods disturbed the flow. Higher convective heat transfer rate occurred in the whole plate as well as in the wall jet region.

• 한국분말재료학회지
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• 제6권1호
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• pp.75-80
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• 1999

The formation of $n-TiO_2$ powder by oxidation of Ti-ethoxied vapor in a flat flame burner reactor maintained under 20 torr has been studied. The produced powder were characterized in terms of crystal structure, chemical composition by XRD and TEM. The results showed that the powder consisted of loose agglomerated anatase and rutile particles and their size were about 10 nm and 20 nm, respectively. In the course of synthesis, changes of the flame color were happened to each condition during heating up the bubbler. The flame color transition phenomena reveled that a critical precursor delivery rate was needed for the powder formation (obtainable powder yield). The critical precursor delivery rate was estimated by a simple function of the bubbler temperature and the carrier gas flow rate. The critical precursor delivery rate was reviewed as an important variable of the nanopowder synthesis.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2006년도 춘계학술대회
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• pp.593-596
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• 2006

This paper introduces various natural energy systems installed at the Eco-Science Center in Geumsan near Taejon. The center, especially, features different solar energy systems to harvest the solar energy to its full extent. Such passive schemes as direct gain and at lacked sun space are applied along with active solar ingredients using flat plate and double skin solar collectors. Space and water heating depends very little on the conventional means. Also a number of photovoltaic modules deployed within its premise supplies power to drive a water pump for the biotop. Combined with other natural energy utilizing systems, the solar energy systems make an exemplary model of a self sustainable public facility which is the first of its kind in Korea.

• 설비공학논문집
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• 제12권3호
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• pp.277-283
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• 2000

The heat transfer characteristics for air jet vertically impinging on a flat plate which had a set of hybrid rod were investigated experimentally. The rod had a cross section made with a half of circular cross section and that of rectangular and was installed in front of the plate. The heating surface was given constant heat flux value of 1020 W/$m^2^{\circ]C$ and the problem parameters investigated were jet Reynolds number, nozzle-to-plate spacing and the rod size. The local and local average Nusselt number characteristics were found to be dependent on the rod size because the flow was disturbed by installing the rod. Higher convective heat transfer rate occurred in the whole plate as well as in the stagnation region.

• 한국태양에너지학회 논문집
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• 제21권3호
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• pp.61-68
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• 2001

This study represents numerical analysis on the thermal and fluid flow of the air layer in a solar collector. The boundary conditions was assumed that the top and bottom wall of the air layer have a heating and cooling surface, respectively, and this calculation model have a solid body with a cooling temperature of $20^{\circ}C$. As the results of simulations, the magnitudes of the velocity vectors and isotherms are increased proportionally to the tilt angles. As the tilt angle is increased, the mean Nusselt numbers are increased and the maximum value of the mean Nusselt number was appeared at tilt angle $\theta=75^{\circ}$.