• 대한토목학회논문집
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• 제11권4호
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• pp.103-112
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• 1991

본(本) 연구(硏究)는 일정균등(一定均等)한 열적(熱的) 특성(特性)을 가지고 있으며 상변화(相變化) 없는 등방(等方) 이질성(異質性)의 3차원(次元) 대수층계(帶水層系)의 열(熱)흐름과 정상상태(定常狀態)의 지하수(地下水)흐름을 모의발생(模擬發生)할 수 있는 유한차분(有限差分) 모형(模型)을 확립(確立)한 것이다. 이 모형(模型)은 대규모(大規模) 지하수(地下水) 흐름체계(體系)에서 폐기물(廢棄物)의 지하저류시(地下貯溜時) 지하수(地下水) 흐름과 발생(發生) 혹은 주입(注入)된 열(熱)의 흐름을 예측(豫測) 분석(分析)하기 위하여 확립(確立)된 것이다. 이러한 대수층계(帶水層系)의 지하수(地下水) 흐름에 작용(作用)하는 조건(條件)으로는 강우주입(降雨注入)으로 인한 수문학적(水文學的) 조건(條件)과 고정(固定)된 수리수두(水理水頭) 경계조건(境界條件) 등(等)이 포함(包含)되고, 열(熱)흐름에는 지열(地熱)의 흐름, 지표면(地表面)으로의 전도(傳導), 주입(注入)에 의한 이류(移流), 고정(固定) 수두경계(水頭境界)로 향(向)한 또는 고정수두경계(固定水頭境界)로 부터의 이류(移流) 등(等)이 포함(包含)된다. 본(本) 모형(模型)에서는 지하수(地下水)흐름과 열(熱)흐름 방정식(方程式)을 번갈아 푸는 교대반복과정(交代反復過程)을 사용(使用)하고, 두 방정식(方程式)의 계산(計算)에는 직접해법(直接解法)을 사용(使用)한다. 이동시간(移動時間)은 모형공간(模型空間)에서 입자추적(粒子追跡)으로 결정(決定)되며, 분할(分轄)된 구역내(區域內)의 지하수(地下水) 유속(流速)은 구역내(區域內)의 유속(流速)을 선형(線形)으로 보간(補間)하여 계산(計算)한다. 본(本) 모형(模型)을 경상북도(慶尙北道) 영일군(迎日郡) 송라면(松羅面) 지경리(地境里) 일대(一帶)의 지하수계(地下水系)에 적용(適用)하여 이 일대(一帶) 지하(地下) 암반층(岩盤層)의 수두분포(水頭分布), 유동로(流動路), 이동시간(移動時間) 및 지하수온분포(地下水溫分布)를 계산(計算)하여 지하수(地下水) 유동체계(流動體系)를 분석(分析)하였다.

• 한국환경과학회지
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• 제10권5호
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• pp.337-342
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• 2001

The Rondonia Boundary Layer Experiment (RBLE-II) was conceived to collect data the atmospheric boundary layer over two representative surface in the Amazon region of Brazil; tropical forest and a deforested, pasture area. The present study deals with the observations of atmospheric boundary layer growth and decay. Although the atmospheric boundary layer measurements made in RBLE-II were not made simultaneously over the two different surface types, some insights can be gained from analysing and comparing with their structure. The greater depth of the nocturnal boundary layer at the forest site may be due to influence of mechanical turbulence. The pasture site is aerodynamically smoother and so the downward turbulent diffusion will be much pasture than over the forest. The development of the convective boundary layer is stronger over the pasture than over the forest. The influence of the sensible heat flux is important but may be not enough to explain the difference completely. It seems that energy advection may occur from the wet and colder(forest) to the dry and warmer area(pasture), rapidly breaking up the nocturnal inversion. Such advection can explain the abrupt growth of the convective boundary layer at the pasture site during the early morning.

• 한국환경과학회지
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• 제10권5호
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• pp.329-336
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• 2001

Characgcteristics of nocturnal boundary layer(NBL) were analyzed by the upper-air observations data using with the airsonde and pilot balloons from 1994 to 1999 in Kyungpook province. The automate weather boundary layer can become stably stratified when the surface is cooler than the air. Stable nocturnal boundary layer height were estimated from the top of surface stable layer where the vertical gradient of temperature and mixing ratio tend to zero or negative. The depth of the stable nocturnal boundary layer depended largely on the thermal effect rather than the wind effect at nighttime. The NBL was more developed on the land than on the coastal region. The stability index (bulk Richardson number) showed that the NBL was stable when the wind was weak and the vertical gradient of the temperature was strong. The heat budget in the NBL was studied by considering the effect of the radiative and the cooled by both the longwave radiative flux and the divergence of the heat flux, while NBL under the cloudy sky the longwave radiative flux played a role of the warming. It was noted that the heat was not conserved in both cases. To complete the heat budget in the NBL the warming/cooling by advection and subsidence must be considered.

• 한국수산과학회지
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• 제36권5호
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• pp.535-540
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• 2003

Based on the monthly weather report of Korea Meteorological Administration (KMA) and daily sea surface temperature (SST) data from National Fisheries Research and Development Institute (NFRDl) (1991-2001), mean heat fluxes were estimated at the Gunsan harbor Net heat flux was transported from the air to the sea surface during March to early September, and it amounts to $125\;Wm^{-2}$ in average daily during May to June. During the middle of September to February, the transfer of net heat flux was conversed from the sea surface to the air with $-125\;Wm^{-2}$ in mininum value in October. Short wave radiation was ranged from 50 to $248\;Wm^{-2}$ showing maxima in April to June. Long wave radiation was ranged from 25 to $92\;Wm^{-2}$ with mininum value in June to July. Sensible heat flux denoting negative values in April to August was ranged from -30 to $72\;Wm^{-2}.$ Latent heat flux was ranged from 15 to $82\;Wm^{-2}$ with maxima in August to September. The phase of heat exchange was changed from cooling to heating in the end of February, and from heating to cooling In the beginning of September. The advective term of heat flux showed minima in April to June and maxima in November. The ratio of temperature variations was 1.37 in the sea surface process and the horizontal process by advection. This indicates that the main factor in variation of temperature at Gunsan harbor is the heat exchange process through the sea surface from the air.

• 한국지구과학회지
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• 제27권3호
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• pp.302-312
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• 2006

이 연구에서는 1979년부터 2004년까지 25년 동안에 극 진동의 강도가 한반도 겨울 한파에 미치는 영향을 대기순환과 열원을 분석하여 조사하였다. 북극 진동이 강할 때 한파의 발생 횟수는 약할 때 보다 약 14.3% 더 발생하는 것으로 나타났다. 월 발생 횟수에서도 양의 AO에서 1.05회/월, 음의 AO에서 1.33회/월로 나타나서 북극 진동이 강할 때가 약할 때 보다 약 26.6% 더 많았다. 이것은 북극 진동이 강한 특정 달에 한파가 자주 발생한다는 것을 의미한다. 또한 북극 진동이 강할 때가 약할 때보다 $0.6^{\circ}C$ 더 낮은 기온을 보였다. 북극 진동의 강약에 따른 열원의 차이를 고찰한 결과, 북극 진동이 강해졌을 때 한반도 주변의 기온은 이류항에 의한 냉각이 강화되어 더 낮아지지만, 열원항에 의한 상쇄 효과에 의해 기온 하강을 억제하는 것으로 나타났다. 그 결과 대기 순환의 유의한 차이에도 불구하고 음의 AO와양의 AO 사이에 기온 차이는 평균적으로 $0.6^{\circ}C$로 작게 나타난다.

• Ocean and Polar Research
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• 제25권2호
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• pp.201-211
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• 2003

Bottom simulating reflectors (BSR), representing the base of the gas hydrate stability field, are widespread on the South Shetland continental margin (SSM), Antarctic Peninsula. With the phase diagram fur the gas hydrate stability field, heat flow can be derived from the BSR depth beneath the seafloor determined on multichannel seismic profiles. The heat flow values in the study area range from $50mW/m^2$ to $85mW/m^2$, averaging to $65mW/m^2$. Small deviation from the average heat flow values suggests that heat flow regime of the study area is relatively stable. The landward decrease of heat flow from the South Shetland Trench to the continental shelf would be attributed to the landward thickening of the accretionary prism and the upward advection of heat associated with fluid expulsion. The continental slope 1500m to 3000m deep, where BSRs are most distinguished in the SSM, shows relatively large variation of heat flow possibly due to complex tectonic activities in the study area. The local high heat flow anomalies observed along the slope may be caused by heat transport mechanisms along a NW-SE trending large-scale fault.

• 한국신재생에너지학회:학술대회논문집
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• 한국신재생에너지학회 2006년도 추계학술대회
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• pp.40-43
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• 2006

Public demand for the heat pump system as a next generation energy equipment is increasing for its eco-friendly and cost-effective advantage. Many researches have been concentrated on how to calculate and develop its own efficiency, while the possible effect of the heat pump operation on the whole subsurface temperature distribution is relatively less considered, During the current study, subsurface temperature disturbance caused by seasonal surface temperature cycle in Busan area and general W-tube heat pump operation is simulated in 3-dimensional heterogeneous medium. It shows that subsurface deeper than 10m from the surface remains nearly unchanged throughout the 4 seasons and groundwater convect ion in highly permeable layer near the surface acts like a main path of heat plume from heat pump system, This implies the significance of detail descript ion in shallow sedimentary layer or highly permeable layer which plays an important role on the regional flow advection and heat transfer. Also, the effect of groundwater convection increases when the arrangement of the 2 injection pipes and 2 extract ion well is maintained parallel to groundwater flow. Therefore, more careful and detail investigation is required before installation and operation of heat pump system that it may not cause any possible change of microbial ecosystem in the shallow subsurface environment or 'contamination of temperature' for groundwater use as well as the loss of efficiency of the equipment itself. This can also help to design the optimized grouting system for heat pump.

• 대한조선학회논문집
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• 제50권6호
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• pp.450-457
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• 2013

For the design guide of a vessel operating in cold region, numerical analysis was carried out to evaluate the weather-tight door which installed the heating cables by using ANSYS 13.0 Transient Thermal. The numerical analysis was performed by considering Advection-Diffusion equation. This study based on the experimental results of 'A study on Anti-Icing Technique for Weather-Tight Door of Ice-Strengthened Vessels'(Jeong, et al., 2011a) in KIOST. For validation of the numerical analysis results, the cold chamber experimental data measured by the heat sensors in certain location of the weather-tight door was used. The external environmental temperature which varies from $5^{\circ}C$ to $-55^{\circ}C$ was considered in numerical analysis. Also three different heating cables which have the heat capacity of 33W/m, 45W/m and 66W/m were adapted for the design parameters to be the most efficient and guidelines for anti-icing design of the weather tight door.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2008년도 춘계학술대회논문집
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• pp.216-217
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• 2008

In recent years, scientific community has found renewed interest in hypersonic flight research. These hypersonic vehicles undergo severe aero-thermal environment during their flight regimes. During reentry and hypersonic flight of these vehicles through atmosphere real gas effects come into play. The analysis of such hypersonic flows is critical for proper aero-thermal design of these vehicles. The numerical simulation of hypersonic real gas flows is a very challenging task. The present work emphasizes numerical simulation of hypersonic flows with thermal non-equilibrium. Hyperbolic system of equations with stiff relaxation method are identified in recent literature as a novel method of predicting long time behaviour of systems such as gas at high temperature. In present work, Energy Relaxation Method (ERM) has been considered to simulate the real gas flows. Navier-Stokes equations A numerical scheme Advection Upstream Splitting Method (AUSM) has been selected. Navier-Stokes solver along with relaxation method has been used for the simulation of real flow over a circular cylinder. Pressure distribution and heat flux over the surface of cylinder has been compared with experiment results of Hannemann. Present heat flux results over the cylinder compared well with experiment. Thus, real gas effects in hypersonic flows can be modeled through energy relaxation method.

• Nuclear Engineering and Technology
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• 제48권4호
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• pp.915-924
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• 2016

After a severe accident to the nuclear reactor, the in-vessel retention strategy is a key way to prevent the leakage of radioactive material. Nanofluid is a steady suspension used to improve heat-transfer characteristics of working fluids, formed by adding solid particles with diameters below 100nm to the base fluids, and its thermal physical properties and heat-transfer characteristics are much different from the conventional working fluids. Thus, nanofluids with appropriate nanoparticle type and volume concentration can enhance the heat-transfer process. In this study, the moving particle semi-implicit method-meshless advection using flow-directional local grid method is used to simulate the bubble growth, departure, and sliding on the downward-facing heating surface in pure water and nanofluid (1.0 vol.% $Al_2O_3/H_2O$) flow boiling processes; additionally, the bubble critical departure angle and sliding characteristics and their influence are also investigated. The results indicate that the bubble in nanofluid departs from the heating surface more easily and the critical departure inclined angle of nanofluid is greater than that of pure water. In addition, the influence of nanofluid on bubble sliding is not significant compared with pure water.