• 한국분무공학회지
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• 제14권3호
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• pp.131-138
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• 2009

In the present study, spread-recoil behavior of a drop of shear-thinning liquid (xanthan solution) on a dry wall (polished stainless-steel plate) was examined and compared with that of Newtonian liquid (glycerin solution). Nine different kinds of xanthan and glycerin solutions were tested, including three pairs of xanthan and glycerin solutions, each having the same viscosity in low shear rate region ($10^{-2}-10^0\;l/s$). The drop behavior was visualized and recorded using a CCD camera. The maximum diameter and the spreading velocity of the xanthan drops turned out to be significantly larger and the time to reach their final shape was much shorter compared to the cases with the glycerin solutions, due to the smaller viscous dissipation resulted from lower viscosity in the higher shear rate region (>$10^0\;l/s$). As a result, the maximum diameters were measured to be larger than the predicted values based on the model proposed for Newtonian liquids, and the deviation was more pronounced with the solution with the larger viscosity variation. Consequently, viscosity variation with the shear rate was found to be a dominant factor governing the spread-recoil behavior of shear-thinning drops.

• 대한안전경영과학회지
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• 제17권4호
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• pp.397-401
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• 2015

In this study, analysed the characteristics of power drop and surface damage in solar cell through high temperature and humidity test in the 3 case of EVA(ethylene vinyl acetate) and 2 case ribbon thickness. The solar cells were tested during the 500hr in $85^{\circ}C$ temperature and 85% relative humidity conditions, that excerpted standard of PV Module(KS C IEC-61215). Through the EL(Electroluminescence) shots, specimen's surface have partialy damaged. Before and after high humidity and high temperature test, ribbon thickness $200{\mu}m$ EVA1 case power drop rate was 8.463%, EVA2 case was 6.667%, EVA3 case was 6.373%. In the ribbon thickness $250{\mu}m$ EVA1 case power drop rate was 6.521%, EVA2 case was 8.517%, EVA3 case was 6.019%. EVA3 case was the lowest power and FF(fill factor) drop rate at the 2 case of ribbon thickness, because EVA3 is laerger than EVA1 and EVA2 in thickness, elongation and tensile strength.

• 설비공학논문집
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• 제19권9호
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• pp.622-629
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• 2007

Compact semi-center type automotive air handling system(AHS) is developed in this study and it's performance is compared with the conventional 3-pieces type air hand-ling system. The pressure drop is measured at component level and system level, and air flow rate and air distribution of discharge air through each ducts from air handling system are measured. System level characteristics of pressure drop at face and windshield discharge mode and air flow rate are investigated, and also temperature control linearities are tested. The volume of the air handling system package is reduced about 20%. And air flow rate increase about 5 to 20% compared to the conventional 3-pieces type air handling system at each discharge mode with significantly improved air pressure drop both component and system level. Also, air distribution and temperature controllability meet to evaluation criteria.

• Journal of Mechanical Science and Technology
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• 제19권6호
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• pp.1338-1346
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• 2005

Effects of thermal contact resistance between heater and susceptor, susceptor and graphite board in a MOCVD reactor on temperature distribution and film growth rate were analyzed. One-dimensional thermal resistance model considering thermal contact resistance and heat transfer area was made up at first to find the temperature drop at the surface of graphite board. This one-dimensional model predicted the temperature drop of 18K at the board surface. Temperature distribution of a reactor wall from the three-dimensional computational fluid dynamics analysis including the gap at the wafer position showed the temperature drop of 20K. Film growth rates of InP and GaAs were predicted using computational fluid dynamics technique with chemical reaction model. Temperature distribution from the three-dimensional heat transfer calculation was used as a thermal boundary condition to the film growth rate simulations. Temperature drop due to the thermal contact resistance affected to the GaAs film growth a little but not to the InP film growth.

• 대한설비공학회:학술대회논문집
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• 대한설비공학회 2008년도 하계학술발표대회 논문집
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• pp.440-445
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• 2008

The present study was investigated the effect of the driving condition on the performance of a louver fin and tube type heat exchanger under frosting condition. Heat transfer rate and pressure drop by frost were experimentally investigated. Effects of the wet blub temperature and the shape of a fin on heat transfer performances has been also investigated. The key parameters were fin type(louver and corrugate fin) and the wet blub temperature of air (0.5, 1.0, $1.5^{\circ}C$). The heat transfer performance of the louver fin and tube type heat exchanger was higher by 0.89% than the corrugate fin type. As the wet blub temperature of air were increased, the heat transfer rate, pressure drop and mass of frost of three test models(Type A, B, C) were increased. Especially, the maximum heat transfer rate and maximum pressure drop were shown for the louver fin and tube type heat exchanger. As a experimental result, the enhancement factor(EF) of louver fin and tube type heat exchanger was $0.2{\sim}0.4$ due to the high pressure drop.

• 설비공학논문집
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• 제21권2호
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• pp.79-86
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• 2009

The present study was investigates the effect of the parameters on the frost formation and heat transfer performance such as fin shape, air temperature and air velocity. Heat transfer rate and pressure drop by frost were experimentally investigated. Effect of the wet blub temperature and air velocity on the heat transfer performance has been also investigated. The heat transfer performance of the louver fin and tube type heat exchanger was higher by maximum of 0.85% than the corrugate fin type at the air temperature of $2.0/1.5^{\circ}C$. As the wet blub temperature of air were increased, the heat transfer rate, pressure drop and mass of frost of three test models were increased. Especially, the maximum heat transfer rate and maximum pressure drop were shown for the Type B louver fin heat exchanger. As an experimental result, the enhancement factor(EF) of louver fin and tube type heat exchanger was only $0.2{\sim}0.4$ due to the high pressure drop.

• Tribology and Lubricants
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• 제38권5호
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• pp.213-221
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• 2022

This paper presents performance measurements of pressure drop and leakage flow rate of test flat seals with asymmetric inclined grooves. This study aims to reveal the influence of groove shapes, often machined in radial film riding-face seals, in forming a hydrodynamic wedge on leakage performance. A test facility was developed, and test seals were manufactured to study the effects of the inlet pressure level, ratio of inlet to outlet pressure, seal groove length, and seal groove height on the steady-state pressure drop and leakage performance. A series of tests were conducted, and the test data were compared to the predictions from a simple and efficient mathematical model using a one-dimensional Reynolds equation. The test results revealed that an increase in the inlet pressure increased the pressure drop through the test seals. The leakage flow rate increased significantly as the inlet pressure and ratio of the inlet to outlet pressure increased. The groove shape also affects seal performance. An increase in the groove length and height resulted in an evident increase in the leakage flow rate. The simple model predictions underestimated the leakage flow rates but showed good agreement with the trend in the measurements for all test operating conditions and changes in the groove shape.

• 한국가스학회지
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• 제28권2호
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• pp.47-55
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• 2024

한국에는 2030년까지 100여 기의 액화수소 탱크가 도입될 것으로 전망된다. 액화수소는 -253 ℃ 상태로 진공단열구조 탱크에 저장되기 때문에 단열에 문제가 생기면 탱크가 파열되는 대재해의 가능성이 상존한다. 그래서 법령에서는 최후의 보루로 PRV를 설치하도록 규정하고 있다. 주의할 것은 액화수소의 경우 배관의 압력강하를 무시하고 용량을 잘못 계산하면 무용지물이 된다는 것이다. CGA S-1.3에서는 PRV 입·출구 압력강하율을 각각 3% 미만 및 10% 미만으로 하도록 하고 있다. 그러나 배관의 압력강하량과 유량 사이에 상호 의존성이 있어 이들 값을 단번에 계산하는 것이 불가능하다. 그래서 본 연구에서는 매트랩/시뮬링크를 이용하여 PRV시스템의 압력강하율을 계산하는 시뮬레이터를 개발하고, 설계 요소에 대한 압력강하율의 민감도를 평가하였다.

• 한국컴퓨터산업학회논문지
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• 제3권1호
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• pp.95-104
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• 2002

본 논문은 ATM(Asynchronous Transfer Mode) 서비스 분류 중 UBR(Unspecified Bit Rate)과 ABR(Available Bit Rate)상에서의 인터넷 TCP/IP(Transmission Control Protocol-Internet Protocol) 트래픽에 관한 연구이다. 퍼지 논리 예측은 트래픽 처리량의 효율성과 공정성을 개선하는 데 사용된다. 본 논문에서는 TCP/IP에서 셀 제거 방식에 기반한 UBR 서비스 버퍼 방식으로 퍼지 논리를 사용하였다. 이는 퍼지 논리 선택적 셀 제거 방식이라고 부른다. 이 방식의 주요 특징은 스위치의 차후 예측 버퍼 상태에 따라서 동적으로 새로 들어오는 패킷을 수락할 것인지 제거할 것인지를 결정한다는 것이다. 이는 제거 인수의 산출을 위해 퍼지 논리 예측의 사용으로 수행된다. 패킷 제거 결정은 이러한 제거 인수와 예측 초기값에 의해 결정된다. 시뮬레이션을 수행하여 제안된 방식이 TCP/IP의 효율성과 공정성 측면에서 현저하게 개선된 것을 알 수 있다. ABR 서비스에서 TCP/IP를 연구하기 위하여 퍼지 논리 ABR 서비스 버퍼 관리 방식을 이전의 연구로부터 근접하거나 정확한 공정율 계산 ER(Explicit cell Rate) 스위치 알고리즘에 적용하였다. 그리하여 기존의 방식과 퍼지 논리 제어 방식의 성능을 비교하였다. 시뮬레이션 결과는 TCP 패킷 손실율이 0이고, 퍼지 논리 제어 방식이 최대한의 효과를 내며 작은 버퍼 크기로 완벽한 공정성을 갖는 것을 보여준다. 퍼지 논리 제어 방식은 VBR 트래픽과 혼용되었었을 때 낮은 셀 손실을 갖고 보다 높은 효율성을 보여준다.

• 한국운동역학회지
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• 제22권4호
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• pp.379-386
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• 2012

The aim of this study was to investigate and identify the differences in lower extremity energy dissipation strategies between drop-landing and countermovement-jump maneuvers. Fourteen recreational athletes(Age : $23.3{\pm}2.1years$, Height : $172.3{\pm}4.0cm$, Weight : $69.2{\pm}4.7kg$) were recruited and instructed to perform drop-landing from 45 cm height and countermovement-jump from 45 cm to 20 cm height. The landing phase was taken as the time between initial contact and peak knee flexion. A motion-capture system consisting of eight infra-red cameras was employed to collect kinematics data at a sampling rate of 200 Hz and a force-plate was used to collect GRF data at a sampling rate of 2000 Hz. Paired t-test was performed to determine the difference in kinematics and kinetics variables between each task. During the countermovement-jump task, all of lower extremity joint ROM and the hip joint eccentric moment were decreased and the ankle joint plantarflexion moment was increased than drop-landing task. In the eccentric work during countermovement-jump task, the ankle joint displayed greater while knee and hip joint showed lesser than drop-landing. Therefore, the knee joint acted as the key energy dissipater during drop-landing while the ankle joint contributed the most energy dissipation during countermovement-jump. Our findings collectively indicated that different energy dissipation strategies were adopted for drop-landing and countermovement-jump.