• 태양에너지
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• 제9권1호
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• pp.62-69
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• 1989

This analysis is to investigate the influence of inflow angle when cooling air flows into PC (Printed Circuit) board channels. Flow between PC board channels with heat generating blocks is assumed laminar, incompressible, two-dimensional. Geometric parameters (block spacing (S), block height (H), block width (W) and channel height (L)) are held fixed. Inflow angle variations are $-10^{\circ},\;0^{\circ},\;10^{\circ}$, where uniform heat flux per unit axial length Q (W/m) from heated block surfaces is generated. The governing equations for velocity and temperature are solved by SIMPLE (Semi-Implicit Method Pressure for Linked Equation) algorithm. Nusselt number on each block surfaces is analyzed after a numerical calculation result. The result shows that the assumption on parallel inflow (inflow angle to channel, $0^{\circ}$) to PC board channels can be used without large error even when inflow' angle is varied.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2002년도 마이크로/바이오 가시화기술부문 학술강연회
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• pp.79-84
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• 2002

Most microfluidic devices such as heat sinks for cooling micro-chips, DNA chip, Lab-On-Chip, and micro pumps etc. have microchannels of various size. Therefore, the design of practical microfluidics demands detail information on flow structure inside the microchannels. However, detail velocity field measurements are rare and difficult to carry out. In addition, as the microfluidics expands, accurate understanding of microscale transport phenomena becomes very important. In this research, micro-PIV system was employed to measure the velocity fields of flow inside a micro-channel. We carried out PIV measurements for several microchannels with varying channels width, inlet and outlet shape, filters, CCD camera and ICCD camera, etc. For effective composition of micro-PIV system, first of all, it is essential to understand optics related with micro-imaging of particles and the particle dynamics encountered in micro-scale channel flows. In addition, it is necessary to find the optimal condition for given experimental environment and? micro-scale flow to be investigated. The problems encountered in measuring velocity field of micro-channel flows are discussed in this paper.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2006년도 PARALLEL CFD 2006
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• pp.395-397
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• 2006

Air interlacing serves to protect the yarn against damage, strengthens inter-filament compactness or cohesion, and ensures fabric consistency. The air interlacing nozzle is used to introduce intermittent nips to a filament yarn so as to improve its performance in textile processing. The effect of various interlacing nozzle geometries on the interlacing process was studied. The geometries of interlacing nozzles with single or multiple air inlets located across the width of yarn channels are investigated. The basis case is the yarn channel, with a perpendicular main air inlet in the middle. Other cases have main air inlets, slightly inclined double sub air inlets, The yarn channel cross sectional shapes are either semicircular or rectangular shapes. The compressed impinging jet from the main air inlet hole hits the opposing bottom wall of the yarn channel, is divided into two branches, joins with the compressed air coming out from sub air inlet at the bottom and creates two free jets at both ends of the yarn channel. The compressed air movement in the cross-section consists of two opposing directional vortices. The CFD-FASTRAN flow parallel solver was used to perform steady simulations of impinging jet flow inside of the interlace nozzles. The vortical structure and the flow pattern such as pressure contour, particle traces, velocity vector plots inside of interlace nozzle geometry are discussed in this pater.

• 사물인터넷융복합논문지
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• 제9권3호
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• pp.93-98
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• 2023

논문에서는 어닐링 시뮬레이션에 근거한 인공 뉴럴 네트워크를 구축한다. 미세 유동채널의 전기화학적 가공 파라미터와 채널 형태 간의 매핑은 샘플의 학습에 의하여 이루어진다. 스텐리스강 표면에 대한 미세 유동채널의 전기화학적 가공의 깊이와 넓이가 예측되고, 형성된 네트워크 모델을 입증하기 위한 NaNO3 해 내부의 펄스 전원공급기와 함께 유동채널의 실험이 진행된다. 결과적으로, "4-7-2" 구조를 갖는 인공 뉴럴 네트워크에 의한 어닐링 시뮬레이션으로 예측된 채널의 깊이와 넓이는 실험값에 매우 근접한다. 그 오차는 5.3% 미만이다. 예측된 데이터와 실험 데이터는 전기화학적 가공 과정에서의 에칭 규격이 전압 및 전류의 밀도와 매우 밀접한 관계가 있음을 보여준다. 전압이 5V보다 작을 때에는 채널 내에 "작은 섬"이 형성된다; 반면에 전압이 40V보다 클 때에는 채널의 측면 에칭이 비교적 크고 채널 사이의 "댐"은 사라지게 된다. 전압이 25V일 때 채널의 가공 형태는 최적이 된다.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2007년도 제29회 추계학술대회논문집
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• pp.367-370
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• 2007

Present study examines detonation wave propagation characteristics in annular channel. A normalized value of channel width to the annular radius was considered as a geometric parameter. A parametric study was carried out for a various regimes of detonation waves from weakly unstable to highly unstable detonation waves. Numerical approaches that used in the previous study of numerical requirements of the simulation of detonation wave propagations in 2D and 3D channel were used also for the present study with OpenMP parallization for multi-core SMP machines. The major effect of the curved geometry on the detonation wave propagation seems to be a flow compression effect, regardless of the detonation regimes. The flow compression behind the detonation wave by the curved geometry of the circular channel pushes the detonation wave front and results in the overdriven detonation waves with increased detonation speed beyond the Chapmann-Jouguet speed. This effect gets stronger as the normalized radius smaller, as expected. The effect seems to be negligible beyond the normalized radius of 10.

• 대한기계학회논문집B
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• 제25권9호
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• pp.1209-1218
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• 2001

The present paper proposes a new correlation for the flow boiling heat transfer coefficients in the low flow rate condition (Re(sub)LF$\leq$200) within horizontal rectangular channels with small gaps (heights). The gap between the upper and the lower plates of each channel ranges from 0.4 to 2mm while the channel width being fixed to 20mm. Refrigerant 113 was used as the test fluid. The mass flux ranges from 50 to 200kg/㎡s and the channel walls were uniformly heated with the heat flux range of 3-15kW/㎡. The quality range covers from 0.19 to 0.76 and the flow pattern is considered to be annular. The measured heat transfer coefficients increase with the mass flux and the local quality; however the effect of the heat flux appears to be minor. At the low mass flux condition, which is more likely with the smaller gap size, the heat transfer is primarily controlled by the liquid film thickness. The proposed F factor for the heat transfer coefficient in the range of Re(sub)LF$\leq$200 well represents the experimental data within the deviation of $\pm$20%. The Kandlikars flow boiling correlation covers the higher flow-rate range(Re(sub)LF>200) within the deviation of $\pm$20%.

• 설비공학논문집
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• 제13권4호
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• pp.304-311
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• 2001

An experimental study on the countercurrent two-phase flow in narrow rectangular channels has been performed. The void fraction and the pressure gradient were investigated using air and water in 760 mm long, 100 mm wide. vertical test sections with 2, 3 and 5 mm channel gaps. Tests were systematically performed with downward liquid superficial velocities and upward gas velocities covering 0 to 0.08 and 0 to 2.5 m/s ranges. respectively. the experimental results were compared with the previous correlations, which were mainly for round tubes, and the qualitative trends were found to be in good agreements. However the quantitative discrepancies were hardly neglected. as the superficial gas velocities increased, the void fraction increased and the pressure gradient decreased, where the effects of the liquid superficial velocities were infinitesimal. as the gap width of the rectangular channel increased the void fraction and the 2-phase frictional pressure gradient approached those values for the round tubes. Equi-periphery diameter, rather than the hydraulic diameter, seemed to be more effective in the analysis of two-phase flow behavior.

• 한국산림과학회지
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• 제79권3호
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• pp.269-277
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• 1990

황폐계류(荒廢溪流)에서 발생하고 있는 토사재해(土砂災害)의 방재대책(防災對策)을 수립할 경우 우선 검토되어야 할 것은 하상면(河床面)의 미지형변화(微地形變化)와 사방시설(砂防施設)에 의해 기대되는 하도고정(河道固定)을 예측하는 것이다. 이를 위해 실지계류(溪流)에서 발생되고 있는 하상미지형(河床微地形)의 특성과 사방시설(砂防施設)의 배치효과를 파악하고, 이어서 모형실험(模型實驗)에 의해 그 유효성을 확인하여 저(低)댐의 군적(群的)배치에 의한 하상미지형(河床微地形)의 변화에 대하여 검토하였다. 실험결과에서 저(低)댐의 군적(群的)배치가 하도고정(河道固定)에 미치는 영향은 국소세굴(局所洗掘) 방지, 유로폭(流路幅)과 퇴적역(堆積域)의 확대였다. 1. 저(低)댐 군(郡)의 배치(L'/L=1)에 의해 국소세굴(局所洗掘)을 일으키는 유수(流水)의 편류현상(偏流現象)에 대하여 댐이 유수(流水)와 토사(土砂)를 분리하여 퇴적(堆積)을 촉진시킴과 동시에 유하수(流下水)를 분산시켜 소유력(掃流力)을 감소시켰다. 따라서 횡단면변동량(橫斷面變動量)(F.A.)은 무시설(無施設)시에 비하여 약65%가 저감(低減)되었다. 2. 유로폭(流路幅)에 대한 저(低)댐군(郡)의 배치효과는 사방시설(砂防施設)의 시공구간장(施工區間長)에 비례하여 증가되었다. 전 구간에 사방시설(砂防施設)을 배치하였을 경우(L'/L=1)는 무시설(無施設)시 (L'/L=0)에 비해 1.53배 확보되었다. 3. 하도내(河道內)에 이종토사(移種土砂)가 퇴적(堆積)하기 위하여는 퇴적공간(堆積空間)이 필요하며, 퇴적토사(堆積土砂)가 안정하는 조건으로 소유력(掃流力)이 감소와 함께 퇴적역(堆積域)의 확보가 필요하다. 저(低)댐군(郡)의 배치에 의해 퇴적역(堆積域)은 약 2.10배 증가하였다.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.921-926
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• 2001

The link for the Superconducting Flux Flow Transistor (SFFT) which is based on the flux flow has been fabricated by the ICP etching methods. The channel width and the thickness of the SFFT were a 3 ${\mu}$m and about 300 nm, respectively. The superconducting characteristic of the link was measured by the x-ray diffraction and the E.D.S.. The SFFT etched by ICP showed an I-V characteristic like the three terminal transistor.

• 대한전기학회논문지:전기물성ㆍ응용부문C
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• 제53권4호
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• pp.231-236
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• 2004

A normally open thermopneumaticc-actuated microvalve has been fabricated and their properties are investigated. The advantages of the proposed microvalve are of the low cost fabrication process and the transparent optical property using polydimethylsiloxane (PDMS) and indium tin oxide (ITO) glass. The fabricated microvalves with in-channel configuration are easily integrated with other microfluidic devices on the same substrate. The fabrication process of thermopneumatic-actuated microvalvesusing PDMS is very simple and its performance is very suitable for a disposable lab-on-a-chip. The PDMS membrane deflection increases and the flow rates of the microchannel with microvalvels decrease as the applied power to the ITO heater increases. The powers at flow-off are dependent on the membrane thickness and the applied inlet pressure but are independent of the channel width of microvalves. The flow rate is well controlled by the switching function of ITO heater and the closing/opening times are around 20 sec and 25 sec, respectively.