• Proceeding of EDISON Challenge
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• 2016.03a
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• pp.625-627
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• 2016

본 논문은 EDISON CFD의 전처리기, eMEGA를 이용하여 격자를 생성하고, 2차원 정렬 격자 기반 비압축성 해석자를 이용하여 유동해석을 진행한 뒤 후처리기, eDAVA를 통해 유동선을 그려 블라인드 장착에 따른 실내 공기 순환에 대한 연구 내용을 담고 있다. 본 연구는 시중에 판매중인 사생활 보호용 블라인드를 포함, 여러 블라인드의 장착 여부에 따라 실내 내부 공기 순환의 양상을 확인하고 실제로 블라인드 장착 시 실내환기에 어떤 영향을 주는지 유동 선을 통해 확인해 보았다. 블라인드 미장착시, 실내 전체적으로 공기가 고루 순환되는 모습을 보였으며, 블라인드 장착 시 대체로 블라인드 형태에 따라 유동이 이동하는 것을 볼 수 있었다. 본 연구는 사생활 보호와 환기 효율성의 관점에서의 소비자 선택권에 영향을 미치는 효과를 가져 올 것으로 보인다.

• Transactions of the Korean Society of Mechanical Engineers
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• v.11 no.1
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• pp.160-169
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• 1987

Numerical simulation of the flow of upper convected Maxwell fluid through planar 4:1 contraction has been performed using type dependent difference apprximation of vorticity equation. For creeping flow assumption, the numerical convergence has been achieved up to much higher values of elasticity parameter than those obtained by conventional finite difference method. For non-vanishing Reynolds number flow, it is shown that the corner vortices disappear, which is in good qualitative agreement with extant experimental results. In doing so, spatial distributions of stream function, vorticity and stresses are considered in relation to change of type of vorticity.

• Proceedings of the Korea Contents Association Conference
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• 2007.11a
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• pp.530-534
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• 2007

Flow visualization is one of visualization techniques and it means a visual expression of vector data using 2D or 3D graphics. It aims for human to easily understand a special feature of the vector data. Flow visualization can be classified into various criterions such as visualization technique, data dimension, type of the flow, and so on. Visualization technique can be categorized into direct method, integration method and derived data based method. Data dimension can be divided into 2D, 2.5D and 3D. Type of flow data may be classified into steady and unsteady. In this paper, various LIC based flow visualization methods will be introduced which is one of representative integration based techniques. Those methods will be categorized with more detailed criterions such as dimension and type of flows.

• Composites Research
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• v.34 no.4
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• pp.249-256
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• 2021

In this paper, the densification of a carbon/carbon composite during a chemical vapor infiltration (CVI) process is studied using a chemo-mechanical model. The multi-physics numerical model, developed in the previous research, couples computational fluid dynamics and major chemical reactions in the reactor. The model is especially utilized to study the effect of flow behavior around the preform on the densification. Four different types of "flow-guide" structures are placed to alter the gas flow around the preform. It is shown that the flow pattern and speed around the preform can be controlled by the guide structures. The process simulations demonstrate that the average density and/or density distribution of the preform can be improved by controlling the gas flow around the perform. In this study, a full industrial-scale reactor and process parameter were used.

• Proceedings of the Korea Water Resources Association Conference
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• 2007.05a
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• pp.503-507
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• 2007

지하수 유동 모델에 반영되는 유역의 수리지질학적, 수문학적 특징들은 지하수 유동 특성에 주요한 영향을 미칠 수 있는 현장 특성들이다. 상기 특징들을 최대한 반영하기 위하여 438개의 관정자료를 토대로 갑천 유역(유역 면적 $648.3km^2$)의 대수층 구조 특성을 분석하고, 24개의 하천 자료를 이용하여 지하수 유동 모델을 구축하였다. 그리고 검 보정된 준분포형 유출모형(SWAT)의 22개 소유역의 지하수 함양량 결과를 3차원 지하수 유동 모델(MODFLOW)과 연계하여 갑천 유역의 광역 지하수 유동 특성을 평가하였다. 모의된 지하수위와 86개 지하수 관측정의 지하수위 비교에서 결정계수는 0.9918, 유역 전체의 물교환량의 상대오차율이 약 0.57%로 갑천 유역의 지하수 유동 특성을 잘 반영하였다. 갑천 유역의 지하수는 지형 및 대수층 특성과 하천의 영향에 의하여 전반적으로 유역 남쪽에서 북쪽으로 유동하는데 산지 지역에 존재하는 하천들은 손실과 이득 하천의 형태를 반복하는 반면, 갑천 중 하류 부분과 갑천-유등천 합류 부근은 이득하천의 형태를 보이고 있다. 그리고 소유역별 지하수 물교환량 분석한 결과, 상기 지역을 포함하는 소유역의 하천 공급원이 해당 유역의 지하수 함양량보다 지하수 유동 체계에 따라 인근 소유역에서 공급되는 지하수 유입량 비율이 훨씬 높은 것으로 분석되었다. 반면 유등천 중 상류 지역의 소유역을 제외한 산지 지역의 경우는 하천 공급원이 지하수 유동 체계에 의한 유입량보다 해당 유역 내에서 공급되는 지하수 함양량 비율이 높은 것으로 분석되었다. 따라서 지표수와 지하수의 상호작용 및 하천 유출에 지하수 유동 특성이 주요한 영향을 미치는 것으로 평가되었다.ens 4.4% (2.19)로 나타났다. 4. 全모기類의 月別 捕獲個體數에 對한 百分率은 다음과 같다. 5月 : 0.1% (1981年), 0.0% (1982年); 6月 : 3.5%, 1.3%; 7月 : 50.0%, 33.9%; 8月 : 37.1%, 52.1%; 9月 : 8.8%, 11.9%; 10月 : 0.5%, 0.8%; 11月 : 0.1%. 5. 모기類의 出現은 1981年과 1982年 모두 5月初로서 共通性을 지니고 있으나 增加勢를 보이는 것은 다르게 나타났다. 즉, 1981年은 6月 첫째 週이고 1982年은 前年度보다 3週 앞당겨진 5月 둘째 週였다. 6. 發生最大 peak는 1981年이 7月 다섯째 週이고, 1982年은 2週가 늦은 8月 둘째 週였다. 7. Culex (Culex) pipiens pallens의 最大發生 peak는 1981年度에 7月 다섯째 週, 1982年度는 2週 앞당겨진 7月 셋째 週였다. 8. Culex (Culex) tritaeniorhynchus summoro년의 最大發生 peak는 1981年, 1982年 모두 8月 둘째 週였다. 9. Anopheles (Anopheles) sinensis의 最大發生 peak는 1981年에 7月 다섯째 週, 1982年은 2週 앞당겨진 7月 셋째 週였다. 10. 重要 3種의 最大 peak를 比城하면 Culex (Culex) pipiens pallens와 Anopheles (Anopheles) sinensis는 1981年과 1982年 모두 最大 peak時期가 同一하였으며, Culex (Culex) tritaeniorhynchus summoro년는 2年間 모두 8月둘째 週에 나타났다.osterior to manubrium and anterio

• Proceedings of the Korean Nuclear Society Conference
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• 1999.05a
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• pp.299-299
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• 1999

• Journal of the Korean Society of Marine Environment & Safety
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• v.12 no.4 s.27
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• pp.261-266
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• 2006

In this study, a scaled model chamber was built to investigate ventilation characteristics of the hood room in LNG carrier. Experimental study was performed in model by visualization equipment with laser apparatus. Four different kinds of measuring area were selected as experimental condition Instant simultaneous velocity vectors at whole field were measured by 2-D PIV system and its software adopting two-frame grey-level cross correlation algorithm. The flow pattern reveals the large scale counter-clockwise forced-vortex rotation at center area.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.10 no.3
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• pp.177-184
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• 2000

The effect of the buyancy and thermocapillarity for differnent aspect ratio of flow field on melt motion and mass transfer has been numerically investigated in magnetic Czochralski crystal growth of silicon. During the process of crystal growth, the melt depth of crucible reduces so the aspect ratio of flow field also reduces. Therefore the shape of magnetic field of the flow field changes and the flow pattern also changes significantly. Together with the melt flow which forms the Marangoni convection (or thermocapillary flow) that comes from the inside the flow field, a flow circulation is observed near the corner close both to the crucible wall and the free surface. Due to this circulation, buoyancy effect has been turned out to be local rather than global. As the aspect ratio decreases, the radial component of the magnetic field prevails compared with the axial component in the flow field. Under the influence of this magnetic field, the melt flow and the temperature distribution in a meridional plane tend to depend on the radial position. As the aspect ratio decreases, the temperature gradient near the edge of the crystal decreases yielding smaller thermocapillarity, and the oxygen concentration near the crystal and the oxygen incorporation rate also decrease.

• Journal of the Korean Society for Aeronautical & Space Sciences
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• v.43 no.2
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• pp.109-117
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• 2015

Aircraft needs an inlet duct to supply the airflow to engine face. A fighter aircraft that requires low radar observability has to hide the engine face in the fuselage to reduce the Radar Cross Section(RCS). Therefore, the flow path of the inlet duct is changed into S-shape. The performance of the aircraft engine is known to be influenced by the shape and the centerline curvature of the S-Duct. In this study, CFD analysis of the RAE M 2129 S-Duct has been performed to investigate the influence of aspect ratio of inlet geometry. The performance of the S-Duct is evaluated in terms of the distortion coefficient. To simulate the flow under adverse pressure gradient better, $k-{\omega}SST$ turbulence model is employed. The computational results are validated with the ARA experimental data. The secondary flow and the flow separation are observed for all computational cases, while the semi-circular geometry has been found to produce the best results.

• Journal of the Korean Society for Nondestructive Testing
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• v.31 no.5
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• pp.479-486
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• 2011

In image-based CFD modeling of carotid bifurcation hemodynamics, it is often not possible (or at least not convenient) to impose measured velocity profiles at the common carotid artery inlet. Instead, fully-developed velocity profiles are usually imposed based on measured flow rates. However, some studies reported a pronounced influence of inflow boundary conditions that were based on actual velocity profiles measured by magnetic resonance imaging which showing the unusual presence of a high velocity band in the middle of the vessel during early diastole inconsistent with a Dean-type velocity profile. We demonstrated that those velocity profiles were induced by the presence of modest secondary curvature of the inlet and set about to test whether such more "realistic" velocity profiles might indeed have a more pronounced influence on the carotid bifurcation hemodynamics. We found that inlet boundary condition with axisymmetric fully-developed velocity profile(Womersley flow) is reasonable as long as sufficient CCA inlet length of realistic geometry is applied.