• 한국자동차공학회논문집
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• 제11권4호
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• pp.29-36
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• 2003

A cylindrical constant volume combustion chamber was used to investigate the flow characteristics at spark plug and the combustion characteristics of inhomogeneous charge methane-air mixture under several parameters. The flow characteristics such as mean velocity and turbulence intensity was analyzed by hot wire anemometer. Combustion pressure development measured by piezoelectric pressure transducer was used to investigate the effect of initial charge pressure, excess air ratio and ignition times on combustion pressure and combustion duration. Mean velocity and turbulence intensity had the maximum value at 200 or 300ms and then decreased to beneath 0.05m/s gradually at 3 seconds. Second mixture is accompanied by an increase in the combustion rate, and that the higher the mass which is added in the second stage injection, the faster the burn rate.

• International Journal of Automotive Technology
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• 제6권2호
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• pp.79-85
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• 2005

This work is to investigate the surface heat flux and combustion characteristics of premixed propane mixture in a constant volume chamber. The experiment of heat flux and combustion characteristics of premixed propane mixture are performed with various equivalence ratio and initial pressure conditions. Based on the experimental results, it is found that the maximum instantaneous temperature is increased with the increase of initial pressure in the chamber. There are significant differences in the burning velocity of premixed propane mixture at different measuring points in the constant volume combustion chamber. A]so, the trends of temperature difference at each measuring points are similar to the burning velocity in the combustion chamber. It is concluded that the total heat loss during the combustion period is affected by the equivalence ratio and the initial condition of fuel-air mixture.

• 한국소음진동공학회:학술대회논문집
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• 한국소음진동공학회 2004년도 추계학술대회논문집
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• pp.972-975
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• 2004

In order to reduce the noise of BLDC motor, a systematic optimization procedure for rotor structure is presented. The noise index is defined as the sum of volume velocity of FE-model that are calculated at the dominant frequencies during dehydration process, which is based on the principle of radiation simple volume source. Then, the five design variables are selected to represent the shape and layout or rotor structure. This discrete design optimization problem for minimizing the noise index is solved by 3-level orthogonal array based effect analysis. Finally, the response surface method (RSM) combined optimization approach is employed for more refining the approximate optimum.

• 한국음향학회:학술대회논문집
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• 한국음향학회 1994년도 FIFTH WESTERN PACIFIC REGIONAL ACOUSTICS CONFERENCE SEOUL KOREA
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• pp.770-774
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• 1994

The volume of an acoustic source is important in determining various acoustic parameters. One of the suggested techniques is the internal pressure method incorporating a loudspeaker attached to a chamber wall and a microphone inserted into the cavity. Although the method is easy to handle with a very simple measurement setup, the coupling effects between the dynamic system of the loudspeaker and acoustic field, and the effects of higher order modes introduced by the discontinuities in the acoustic field, and the effects of higher order modes introduced by the discontinuities in the acoustic field should be considered for precise result. In this study, higher order modes due to the discontinuities of loudspeaker and microphone boundaries are included and the electro-acoustic coupling effects are compensated for by using the results of two cylinders with different lengths. The volume velocity of a loudspeaker thus obtained agrees very with that measured by laser sensor.

• Nuclear Engineering and Technology
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• 제54권12호
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• pp.4620-4624
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• 2022

Several cadmium zinc telluride (CZT) crystals were fabricated into radiation detectors using methods that included slicing, dicing, lapping, polishing, and chemical etching. A wet passivation with sodium hypochlorite (NaOCl) was then carried out on the Br-etched detectors. The Te-rich layer on the CZT surface was successfully compensated to the Te oxide layer, which was analyzed with X-ray photoelectron spectroscopy data of both a Br-etched crystal and a passivated CZT crystals. We confirmed that passivation with NaOCl improved the transport property by analyzing the mobility-lifetime product and surface recombination velocity. The electrical and spectroscopic properties of large volume detectors were compared before and after passivation, and then the detectors were observed for a month. Both bar and quasi-hemispherical detectors show an enhancement in performance after passivation. Thus, we could identify the effect of NaOCl passivation on large volume CZT detectors.

• 대한기계학회논문집B
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• 제29권6호
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• pp.671-686
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• 2005

The transient nature and complex geometries of two-phase gas-liquid flows cause fundamental difficulties when measuring flow velocity using an electromagnetic flowmeter. Recently, a current-sensing flowmeter was introduced to obtain measurements with high temporal resolution (Ahn et al.). In this study, current-sensing flowmeter theory was applied to measure the fast velocity transients in slug flows. The velocity fields of axisymmetric gas-liquid slug flow in a vertical pipe were obtained using Volume-of-Fluid (VOF) method, and the virtual potential distributions for the electrodes of finite size were also computed using the finite volume method for simulating slug flow. The output signal prediction for slug flow was carried out from the velocity and virtual potential (or weight function) fields. The flowmeter was numerically calibrated to obtain the cross-sectional liquid mean velocity at an electrode plane from the predicted output signal. Two calibration parameters are proposed for this procedure: a flow pattern coefficient and a localization parameter. The flow pattern coefficient was defined by the ratio of the liquid resistance between the electrodes for two-phase flow with respect to that for single-phase flow, and the localization parameter was introduced to avoid errors in the flowmeter readings caused by liquid acceleration or deceleration around the electrodes. These parameters were also calculated from the computed velocity and virtual potential fields. The results can be used to obtain the liquid mean velocity from the slug flow signal measured by a current-sensing flowmeter.

• 한국수자원학회논문집
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• 제54권11호
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• pp.933-942
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• 2021

홍수시 하천의 유속을 효율적이고 안전하게 측정할 수 있는 방법의 하나로 제시된 것이 표면 영상유속측정법이다. 표면영상유속측정법에는 영상분석 기법에 따라 다양한 종류가 있으나, 이 중에서도 최근 일정시간 동안의 유속의 시간평균을 한 번에 산정할 수 있는 시공간영상 유속계측법이 하천의 표면유속 측정에 대한 연구가 활발히 진행되고 있다. 시공간영상 유속계측법은 일정 시간 동안의 시공간 영상을 한 번에 분석하기 때문에, 유속산정 시간을 획기적으로 줄일 수 있는 장점이 있다. 그러나 시공간영상 유속계측법은 주흐름방향을 정확히 알지 못하면 오차를 유발할 수 있다. 본 연구는 표면영상을 시간적으로 누적한 시공간체적을 구성하고, 이 시공간체적에서 시간축 방향으로 최대값 영상을 만든 뒤 이를 고속푸리에변환하여 주흐름방향을 탐색하는 새로운 기법을 제안하였다. 이 방법은 공간영상에서 주흐름방향을 찾는 첫단계와 주흐름방향의 시공간영상에서 유속의 크기를 산정하는 두번째 단계로 구성되어 있다. 첫번째 단계에서 찾아낸 주흐름방향으로 시공간영상을 작성하고, 이 시공간영상의 고속푸리에변환을 이용하여 유속을 산정하였다. 제안된 방법은 주흐름방향을 정확하게 추정하여 시공간영상을 생성하고 분석하므로, 기존 방법들이 취약했던 이차원 흐름에 대해서도 신속하고 정확한 유속분석이 가능하다. 개발된 방법을 공동흐름에 대한 인공영상에 적용한 결과 비교적 정확하게 2차원 유속분포 측정이 가능한 것으로 나타났다.

• 한국의학물리학회지:의학물리
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• 제24권4호
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• pp.243-252
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• 2013

본 연구는 표적이 규칙적으로 움직일 때 생기는 4DCT 영상의 모션 아티팩트(motion artifact) 관련된 원인들인 partial volume effect (PVE), partial projection effect (PPE), 각각의 프레임의 시작점 사이에 불일치(MMimph)의 원인들은 조사 및 분석을 목적으로 했다. 본 기관에서 제작된 흉부팬텀과 아크릴의 두개의 원기둥팬텀(반지름: 2 cm, 길이: 0.5 cm/ 반지름: 2 cm, 길이: 10 cm)이 규칙적인 움직이는 동안 CT을 이용하여 4D 영상을 획득했다. 촬영은 자동시작과 각각의 프레임의 시작점을 일치시키기 위해 매뉴얼로 두 가지 방법으로 시작하였다. 첫번째 실험에서는 CT 캔트리 rotation time은 5초와 8초가 이용되었다. 각 프레임은 다른 위상으로 시작되었다. 두번째 실험에서는 각 프레임에서 같은 위상으로 시작되게 하기 위해 매뉴얼로 시작했다. 세번째 실험에서는 원기둥팬텀을 2초와 6초를 주기로 움직였다. 각각의 4DCT의 영상에서 표적의 부피를 구했다. 영상으로부터 구한 표적의 부피와 표적의 실제 부피와 비교를 통해 관계를 분석했다. 흉부팬텀 실험에서는 CT의 갠트리 속도가 팬텀의 움직임보다 빠를수록 PVE와 PPE의 영향이 적어짐에 따라 영상에서 얻은 표적부피는 실제에 근접했다. 각각의 프레임의 시작점이 일치할수록 움직임의 속도와 표적의 부피와 상관관계가 높았다. 원기둥팬텀에서는 흉부팬텀의 경우와 같이 갠트리 속도가 팬텀의 움직임보다 빠를수록 영상으로부터 구한 표적부피는 실제 표적부피에 근접했다. 특히 한 slice의 두께가 2.5 mm을 고려 할 때 axial방향의 PVE, PPE, 각각의 프레임의 시작점이 일치가 되는 상태를 시뮬레이션한 길이 10 cm의 원기둥팬텀 실험에서는 영상에서 얻은 표적부피는 표적이 정지되었을 때 영상에서 얻은 부피와 거의 일치했다. 팬텀이 느리게 움직일수록, CT 갠트리의 rotation 시간이 짧을수록 영상에서 얻은 표적부피는 실제 부피에 근접했다. CT 촬영 시 각각의 프레임의 시작점이 같을수록 표적의 속도와 영상에서 의한 표적의 부피는 상관관계가 높게 나타났다. CT 갠트리의 rotation 속도를 팬텀의 움직임보다 빠르게 하고, CT 촬영시 각의 프레임의 시작점을 일치시킬수록 실제의 팬텀부피에 근접하리라고 예상된다.

• 대한기계학회논문집B
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• 제21권2호
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• pp.195-201
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• 1997

Static and non-static flame methods were used to measure the laminar burning velocity of methane, ethane and natural gas. The flame slot angle and velocity of unburned gas mixture were determined by Schlieren method and LDV, respectively, for static flame. The diameter of nozzle was selected as 11 mm. The experimental results containing the stretch effect showed that the maximum burning velocities were 41.5 for natural gas, 40.8 for methane and 43.4 cm/sec for ethane on equivalence ratio of 1.1. Constant volume combustion chamber was also used for non-static flame. The propagation process of flame front was visualized by high speed camera during constant pressure. The maximum burning velocity of natural gas was determined as 42.1 cm/sec on equivalence ratio of 1.15.

• 대한기계학회논문집B
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• 제27권4호
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• pp.476-483
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• 2003

A mathematical model is presented to predict the two-phase flow and heat transfer phenomena of the evaporating extended meniscus region in a micro-channel. The pressure difference at the liquid-vapor interface can be obtained by the augmented Laplace-Young equation. The correlative equations for film thickness, pressure, and velocity in the meniscus region are derived by applying the mass, momentum, and energy equations into the control volume. The results show that increasing the heat flux and the liquid inlet velocity cause the length and liquid film thickness of the extended meniscus region to decrease. The variation, however, of the heat flux and liquid inlet velocity has no effect on the profile of film thickness. The majority of heat is transferred through the thin film region that is a very small region in the extended meniscus region. It is also found that the vapor velocity increases gradually in the meniscus region. However, it increases sharply at the junction of the meniscus and thin film regions.