• 한국자동차공학회논문집
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• 제12권6호
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• pp.103-110
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• 2004

The major trend in global automotive market is changing drastically in the way that a vehicle FECPS(Front End Cooling Pack System) is designed and manufactured as an assembly part. The system can encompass many functions, be assembled into a vehicle as a module, and reduce the production cost as well as time. The FECPS consists of an impact beam, an aluminum condenser and a radiator, a carrier and a cooling fan with a BLDC motor. In order to predict the performance of a FECPS accurately, it is essential to properly model the air flow field through various heat exchangers, such as a condenser or a radiator. In this study, the flow field of the system is measured by a PIV(Particle Image Velocimetry) system. The result is compared with that measured with multi-channel anemometer.

• 한국기계기술학회지
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• 제13권1호
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• pp.105-112
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• 2011

Increasing needs for light weight and high safety in modern automobiles induced the wide application of high strength steels in automotive body structures- The main difficulty in the forming of sheet metal parts with high strength steel is the large amount of springback including sidewall curl and twist in channel shaped member parts- Among these shape defects, twist occurs frequently and requires numerous reworks on the dies to compensate the shape deviation- But until now, it seems to be no effective method to reduce the twist in the forming processes- In this study, a new forming process to reduce the twist deformation during the forming of automotive structural member was suggested- This method consists of forming and restriking of embosses on the sidewall around the stretch flanging area of the part- and was applied in the forming process design of an automotive front side inner member with high strength steel- To evaluate the effectiveness of the method, springback analysis using $Pamstampa^{tm}$ was done- Through the analysis results, the suggested method was proven to be effective in twist reduction of channel shaped parts with stretch flanging area.

• Nuclear Engineering and Technology
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• 제53권6호
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• pp.1786-1795
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• 2021

Printed Circuit Heat Exchanger (PCHE) is a widely used heat exchanger in the supercritical carbon dioxide (sCO₂) Brayton cycle because it can work under high temperature and pressure, and has been a hot topic in Next Generation Nuclear Plant (NGNP) projects for use as recuperators and condensers. Most previous studies focused on channel structures or shapes. However, no clear advancement has so far been seen in the allover size of the PCHE. In this paper, we proposed an optimal size of the PCHE with a fixed volume. Two boundary conditions of PCHE were simulated, respectively. When the volume of PCHE was fixed, the heat transfer rate and pressure loss were picked as the optimization objectives. The Pareto front was obtained by the Multi-objective optimization procedure. We got the optimized number of PCHE channels under two different boundary conditions from the Pareto front. The comprehensive performance can be increased by 5.3% while holding in the same volume. The numerical results from this study can be used to improve the design of PCHE with straight channels.

• 한국정보통신학회논문지
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• 제17권11호
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• pp.2621-2626
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• 2013

비대칭 이중게이트 MOSFET의 전위분포에 대하여 고찰하였으며 이를 위하여 포아송방정식의 해석학적 해를 구하였다. 대칭 DGMOSFET는 3단자 소자로서 상하단의 게이트단자가 상호 연결되어 있어 상하단 동일한 제어능력을 가지고 있으나 비대칭 DGMOSFET 소자는 4단자 소자로서 상하단 게이트단자의 전류제어능력을 각각 설정할 수 있다는 장점이 있다. 전위분포를 구할 때 포아송방정식을 이용하였으며 도핑분포함수에 가우시안 함수를 적용함으로써 보다 실험값에 근사하게 해석하였다. 비대칭 이중게이트 MOSFET의 게이트 단자전압 및 게이트 산화막 두께 그리고 채널도핑의 변화에 따라 전위분포의 변화를 관찰하였다. 비대칭 DGMOSFET의 전위분포를 관찰한 결과, 게이트단자 전압 및 게이트 산화막 두께 등에 따라 전위분포는 크게 변화하는 것을 알 수 있었다. 특히 게이트 산화막 두께가 증가하는 단자에서 전위분포의 변화가 더욱 크게 나타나고 있었으며 채널도핑이 증가하면 드레인 측보다 소스 측 전위분포가 크게 변화하는 것을 알 수 있었다.

• Korean Chemical Engineering Research
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• 제58권1호
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• pp.122-126
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• 2020

본 연구에서는 폴리디메틸실록산(PDMS)과 모세관-미세몰딩(MIMIC) 기술을 활용하여 마이크로패턴 채널 시스템을 제작하고, 단일 세포 수준에서 극성화 패턴으로 형성되는 분자 신호를 고해상도 세포 이미징을 통해 분석하였다. 이 과정에서 혈소판유래성장인자(PDGF)가 처리된 세포에서는 세포 이동에 중요한 세 종류의 신호인 포스포이노시티드 3-인산화효소(PI3K), Rac 및 액틴(Actin) 신호가 선두(front)영역에서 후미(rear)영역에 비해 강하게 활성화 하는 데 반해, 마이오신 경쇄(MLC) 신호는 비특이적 경향성을 보여주었다. 본 연구 결과는 향후 마이크로패턴의 미세환경에서 세포 극성화 신호와 세포 이동과의 상관 관계를 연구하는 데 중요한 도움이 될 것으로 사료된다.

• 한국정보통신학회:학술대회논문집
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• 한국정보통신학회 2013년도 추계학술대회
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• pp.691-694
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• 2013

비대칭 이중게이트 MOSFET의 전위분포에 대하여 고찰하였으며 이를 위하여 포아송방정식의 해석학적 해를 구하였다. 대칭 DGMOSFET는 3단자 소자로서 상하단의 게이트단자가 상호 연결되어 있어 상하단 동일한 제어능력을 가지고 있으나 비대칭 DGMOSFET 소자는 4단자 소자로서 상하단 게이트단자의 전류제어능력을 각각 설정할 수 있다는 장점이 있다. 전위분포를 구할 때 포아송방정식을 이용하였으며 전하분포함수에 가우시안 함수를 적용함으로써 보다 실험값에 근사하게 해석하였다. 비대칭 이중게이트 MOSFET의 게이트 단자전압 및 게이트 산화막 두께 그리고 채널도핑의 변화에 따라 전위분포의 변화를 관찰하였다. 비대칭 DGMOSFET의 전위분포를 관찰한 결과, 게이트단자 전압 및 게이트 산화막 두께 등에 따라 전위분포는 크게 변화하는 것을 알 수 있었다. 특히 게이트 산화막 두께가 증가하는 단자에서 전위분포의 변화가 더욱 크게 나타나고 있었으며 채널도핑이 증가하면 드레인 측보다 소스 측 전위분포가 크게 변화하는 것을 알 수 있었다.

• 한국전산유체공학회지
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• 제12권3호
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• pp.41-46
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• 2007

Dynamic behavior of immiscible gas bubble attached to the wall in channel flow plays very important role in many engineering applications. Special attention has been paid to micro direct methanol fuel cell(${\mu}$DMFC) where surface tension becomes dominant factor with minor gravitational effect due to its reduced size. Therefore, displacement of $CO_2$ bubble generating on a cathode side in ${\mu}$DMFC can be very difficult and efficient removal of $CO_2$ bubbles will affect the overall machine performance considerably. We have focused our efforts on studying the dynamic behavior of immiscible bubble attached to the one side of the wall on 2D rectangular channel subject to external shear flow. We used Level Contour Reconstruction Method(LCRM) which is the simplified version of front tracking method to track the bubble interface motion. Effects of Reynolds number, Weber number, advancing/receding contact angle and property ratio on bubble detachment characteristic has been numerically identified.

• JSTS:Journal of Semiconductor Technology and Science
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• 제15권2호
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• pp.286-291
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• 2015

For highly scalable NAND flash memory applications, a compact ($4F^2/cell$) nonvolatile memory architecture is proposed and investigated via three-dimensional device simulations. The back-channel program/erase is conducted independently from the front-channel read operation as information is stored in the form of charge at the backside of the channel, and hence, read disturbance is avoided. The memory cell structure is essentially equivalent to that of the fully-depleted transistor, which allows a high cell read current and a steep subthreshold slope, to enable lower voltage operation in comparison with conventional NAND flash devices. To minimize memory cell disturbance during programming, a charge depletion method using appropriate biasing of a buried back-gate line that runs parallel to the bit line is introduced. This design is a new candidate for scaling NAND flash memory to sub-20 nm lateral dimensions.

• Journal of Mechanical Science and Technology
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• 제20권8호
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• pp.1240-1247
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• 2006

Large eddy simulation of turbulent premixed flame in turbulent channel flow is studied by using G-equation. A flamelet model for the premixed flame is combined with a dynamic subgrid combustion model for the filtered propagation flame speed. The objective of this work is to investigate the validity of the dynamic subgrid G-equation model to a complex turbulent premixed flame. The effect of model parameters of the dynamic sub grid G-equation on the turbulent flame speed is investigated. In order to consider quenching of laminar flames on the wall, wall-quenching damping function is employed in this calculation. In the present study, a constant density turbulent channel flow is used. The calculation results are evaluated by comparing with the DNS results of Bruneaux et al.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2006년도 추계학술대회 논문집
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• pp.36-41
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• 2006

Reverse flow (i.e. flow in the direction opposite to the free stream) inside a channel occurs when an obstruction is placed at certain positions near the near to the channel, placed in another wider channel. In this paper the reverse flow in a duct (diameter D) with an obstruction at the front (which is a disc), is investigated using PIV. The gap g between the obstruction and the entry to the duct is systematically varied and it is found that maximum reverse flow occurs at a g/D value of 0.5. The flow is stagnant around g/D of 1.25 and forward flow occurs for g/D values of 1.5 and above.