• 한국분무공학회지
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• 제26권1호
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• pp.9-17
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• 2021

Six shear coaxial injectors with different recess length and taper angle were manufactured. Cold-flow tests on the injectors were performed at room temperature and pressure using water and air as simulants. By changing the water mass flow rate and air mass flow rate, spray images were taken under single-injection and bi-injection. Breakup length and spray angle were analyzed from instantaneous and averaged spray images using image processing techniques. For all the injectors, the breakup length generally decreased as the momentum flux ratio increased at the same gas mass flow rate. The injectors with 7.5° taper angle usually had the longest breakup length and the smallest spray angle. When the taper angle was 15° or more, it hardly affected breakup length and spray angle. The recess length did not influence breakup length but its effect on spray angle depended on the taper angle.

• 한국정밀공학회지
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• 제14권9호
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• pp.90-100
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• 1997

A full three-dimensional thermo-coupled rigid-viscoplastic finite element method and the currently developed microstructural evolution system which includes semi-empirical equations suggested by different research groups were used together to form an integrated system of process and micro- structure simulation of hot rolling. The distribution and time histroy of the momechanical variables such as temperature, strain, strain rate, and time during pass and between passes were obtained from the finite element analysis of multipass hot rolling processes. The distribution of metallurgical variables were calculated on the basis of instantaneous thermomechanical data. For the verification of this method the evolution of microstructure in plate rolling and shape rolling was simulated and their results were compared with the data available in the literature. Consequently, this approach makes it possible to describe the realistic evolution of microstructure by avoiding the use of erroneous average value and can be used in CAE of multipass hot rolling.

• 한국식품과학회지
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• 제24권4호
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• pp.335-340
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• 1992

무의 염절임 과정에서 일어나는 염의 확산과 관련하여 무의 조직 변화를 측정하고 시간의 함수와 관련된 기계적인 모델을 제시하였다. 침지 염용액의 농도와 침지 온도가 증가할수록 염의 확산은 더 잘 일어났으나 침지온도보다는 염용액의 농도에 의해서 더 많은 염의 확산에 영향을 미쳤다. 염장하지 않은 무는 높은 조직의 강도와 점탄성을 보였으나 온도와 소금농도를 증가시킴에 따라 초기 응력에 대한 조직의 강도 약화를 보여주었으며 응력완화의 정도도 빨라졌고 평형 상태에서 남아있는 탄성 고체의 양도 감소하였다. 또한 침지 용액의 농도와 온도가 증가할수록 무 조직의 점탄성 성분들도 낮아졌는데, 무의 조직변화도 염장 온도보다 염용액의 농도에 의해서 더 많은 영향을 받았다. $Ca^{2+}$과 $Mg^{2+}$이온을 첨가한 경우 점탄성 상수들은 더 큰 것으로 나타났으나 일정 변형에서의 응력의 완화는 더 빠르게 진행되었다. 일정 염농도, 일정 염장 농도와 비순수 소금을 사용했을 때 평형에 도달하기 전의 임의의 시간이 경과한 후에 무 조직의 최종 강도 변화를 점탄성 상수를 이용하여 예측하는 일반식을 제시하였다.

• 한국응용곤충학회지
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• 제34권3호
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• pp.234-242
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• 1995

멸구류 포식성 천적인 등검은황록장님노린재의 온도에 따른 벼멸구 알 공격능력과 기능반응의 변화를 20, 23, 26, 29, 32, $35^{\circ}C$ 등 6개 온도에서 검정하였다. 등검은 황록장님노린재는 산란된지 1일에서 4일된 이런시기의 벼멸구 알을 선호하였으며, 이중 3일된 벼멸구 알을 가장 선호하였다. 등검은황록장님노린재의 벼멸구 알에 대한 포식능력은 Holling의 제2형 기능반응의 Rogers(1972) 진정포식자 모형에 잘 부합되었다. 기능반응의 포식자 탐색율(a)은 $32^{\circ}C$까지는 온도가 높아짐에 따라 증가하는 경향이었으나 $35^{\circ}C$에서는 급격히 감소하였다. 그러나 처리시간(Th)은 온도가 높아짐에 따라 완만히 감소되었다. 등검은황록장님노린재의 벼멸구 알에 대한 온도별, 밀도별 공격위치의 선호성은 일반적으로 저밀도에서는 큰 차이가 없었으나 고밀도에서는 위쪽에 산란된 알을 더 선호하는 경향이었으며 특히 온도가 높아짐에따라 이러한 경향이 더욱 뚜렷이 나타났다.

• 대한기계학회논문집B
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• 제28권12호
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• pp.1557-1566
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• 2004

A flame extinction phenomenon is a typical unsteady process in combustion. Flame extinction is characterized by various physical phenomena, such as convection, diffusion, and the production of heat and mass. Flame extinction can be achieved by either increasing the strain rate or curvature, by diluting an inert gas or inhibitor, or by increasing the thermal or radiant energy loss. Though the extinction is an inherently transient process, steady and quasi-steady approaches have been used as useful tools for understanding the flame extinction phenomenon. Recently, unsteady characteristics of flames have been studied by many researchers, and various attempts have been made to understand unsteady flame behavior, by using various extinction processes. Representative parameters for describing flame, such as flame temperature, important species related to reactions, and chemi-luminescence of the flame have been used as criterions of flame extinction. In these works, verification of each parameter and establishing the proper criterions of the extinction has been very important. In this study, a time-dependent flame temperature and an OH radical concentration were measured using optical methods, and the instantaneous change of the flame luminosity was also measured using a high-speed ICCD (HICCD) camera. We compare the unsteady extinction points obtained by three different methods, and we discuss transient characteristics of maximum flame temperature and OH radical distribution near the extinction limit.

• Journal of Welding and Joining
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• 제11권3호
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• pp.34-47
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• 1993

용접에서 발생하는 열응력 및 잔류응력을 해석하기 위한 유한요소용 모델을 개발하였다. 여러 가 지 변수의 연구를 통하여 Ramp heat input function과 Lumped모델을 제시하였다. 용접부에 열입 력을 점차적으로 주기 위하여 Ramp heat input을 이용하였으며 Ramp input을 통하여 이차원 모 델에서의 이동열원의 영향을 고려하였고 실험치와 비교에서 최적 ramp시간을 결정하였다. 다층용 접에서는 용접 pass 에 비례하여 계산시간이 증가한다. 따라서 후판용접의 잔류응력계산에는 막 대한 계산시간이 필요하며 이를 줄이기 위하여 Lumped 모델을 개발하였다. 이 Lumped모델에서 는 각 용접층에 들어있는 용접 pass들을 하나의 lumped pass으로 이용하였으며 각 pass를 따로 계산한 모델 및 시험치와의 비교를 통하여 최적 lumped technique을 제시하였다. *****Finite element models were developed for thermal and residual stress analysis for the specific welding problems. They were used to evaluate the effectiveness of the various welding heat input models, such as ramp heat input function and lumped pass models. Through the parametric studies, thermal-mechanical modeling sensitivity to the ramp function and lumping techniques was determined by comparing the predicted results with experimental data. The kinetics for residual stress formation during welding can be developed by iteration of various proposed mechanisms in the parametric study. A ramp heat input function was developed to gradually apply the heat flux with variable amplitude to the model. This model was used to avoid numerical convergence problems due to an instantaneous increase in temperature near the fusion zone. Additionally, it enables the model to include the effect of a moving arc in a two-dimensional plane. The ramp function takes into account the variation in the out of plane energy flow in a 2-D model as the arc approaches, travels across, and departs from each plane under investigation. A lumped pass model was developed to reduce the computation cost in the analysis of multipass welds. Several weld passes were assumed as one lumped pass in this model. Recommendations were provided about ramp lumping techniques and the optimum number of weld passes that can be combined into a single thermal input.

• 한국산학기술학회논문지
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• 제21권2호
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• pp.511-520
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• 2020

지구온난화로 인해 하절기 폭염현상과 열대야가 강해짐에 따라, 도시공원 등 녹지공간의 열환경 개선에 대한 연구가 활발히 진행 중이다. 하지만, 녹지의 식재패턴과 바람의 세기로 인해 변화하는 도시 열환경 개선 연구는 아직까지 미흡한 실정이다. 본 연구는 공공 휴게 녹지공간의 온도분석 및 온도의 변화요인을 파악하는데 목적이 있다. 대상지로는 전남대학교 민주마루 앞 광장을 설정하였다. 대상지의 피복상태, 식재형태를 조사 후, 온도, 습도, 풍향, 풍속 등을 측정하여 요인들을 분석하였다. 측정기준은 기상청 기준 오후 2시에 전운량 30% 이하, 습도 90% 이하, 온도는 최고온도 30℃ 이상인 날로 지정하였다. 온도 실측은 크게 1차 실측과 2차 실측으로 구분하여 측정하였다. 1차 실험은 2018년 6월 1일부터 6월 21일까지 30도를 기준일로 6일간, 2차 실험은 2018년 7월 27일부터 8월 1일까지 35도를 기준으로 3일간 측정을 실시하였다. 온도분포에 가장 큰 영향을 미치는 요인은 증발산과 바람에 의한 열 이동으로 판단된다. 온도변화요인으로는 피복유형, 풍속/풍향, 식재유형 등이 있었다. 피복유형에서 목본 식재지는 저온역으로, 초지와 아스팔트 포장은 고온역으로 구분되었다. 풍속/풍향에서는 3.5m/s 이상의 바람이 불어올 때 남풍에서 1.2도, 서풍에서 0.7도, 북풍에서 0.4도, 동풍에서 0.5도씩 순간온도가 저감되었다. 식재유형에서는 녹지량이 많고, 바람의 영향을 많이 받는 형태일수록 온도가 저감되었다. 온도변화요인을 알아보기 위해 등온선을 작성하여, 풍향과 수목식재 위치 관계를 파악하였다.

• 대한기계학회논문집B
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• 제26권8호
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• pp.1095-1101
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• 2002

An experimental apparatus was prepared to investigate thermal and hydrodynamic characteristics of regenerator at cryogenic temperature under pulsating pressure condition. The regenerator was pressurized and depressurized by a compressor with various operating frequencies. Cold end of the regenerator was maintained around 100 K by means of a liquid nitrogen heat exchanger. Instantaneous gas temperature and mass flow rate were measured at both ends of the regenerator during the whole pressure cycle. Pulsating pressure drop across the regenerator was also measured to see if it could be predicted by a friction factor at steady flow condition. The operating frequency of pressure cycle was varied between 3 and 60 Hz, which are typical operating frequencies of Gifford-McMahon, pulse tube, and Stilting cryocoolers. First, the measured friction factor for typical wire screen mesh regenerator was nearly same as steady flow friction factor for maximum oscillating Reynolds number up to 100 at less than 9 Hz. For 60 Hz operations, however, the discrepancy between oscillating flow friction factor and steady flow one was noticeable if Reynolds number was higher than 50. Second, the ineffectiveness of regenerator was directly calculated from experimental data when the cold-end was maintained around 100 K and the warm-end around 293 K, which simulates an actual operating condition of cryogenic regenerator. Influence of the operating frequency on ineffectiveness was discussed at low frequency range.

• 대한기계학회논문집B
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• 제21권2호
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• pp.213-223
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• 1997

Premixed flame is better than diffusion flame to accomplish a high loading combustion. Since the turbulent characteristics of unburned mixture has a great influence on the flame structure, it is general that many researchers realize a high loading combustion with strengthening turbulent intensity of unburned mixture. Because turbulent premixed flame reacts efficiently on the condition of distributed reaction region, we made high turbulent premixed flame in the doubled impingement field. We investigated turbulent characteristics of unburned mixture with increasing shear force and visualized flames with direct and Schlieren photographs. And the combustion characteristics of flame was elucidated by instantaneous temperature measurement with a thermocouple, by ion currents with a micro electrostatic probe, by radical luminescence intensity and local equivalence ratio. Extremely strong turbulent of small scale is generated by impingement of mixture, and turbulent intensity of unburned mixture increased with the mean velocity. As a result of direct photographs, visible region of flame became longer due to increasing central direction flux. But as strengthed turbulent intensity, visible region of flame turned to shorter and reaction occurred efficiently. As strengthened turbulent intensity of mixture with increasing flux of central direction, maximum fluctuating temperature region moved to radial direction and fluctuation of temperature became lower. The reason is influx of central direction which caused flame zone to move toward radial direction, to maintain flame zone stable and to make flame scale smaller.

• 대한기계학회논문집B
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• 제29권2호
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• pp.169-179
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• 2005

Nucleate boiling experiments on heating surface of constant wall temperature were performed using R113 for almost saturated pool boiling conditions. A microscale heater array and Wheatstone bridge circuits were used to maintain a constant wall temperature condition of heating surface and to measure the heat flow rate with high temporal and spatial resolutions. Bubble images during the bubble growth were taken as 5000 frames per second using a high-speed CCD camera synchronized with the heat flow rate measurements. The bubble growth behavior was analyzed using the new dimensionless parameters for each growth regions to permit comparisons with previous experimental results at the same scale. We found that the new dimensionless parameters can describe the whole growth region as initial and later (thermal) respectively. The comparisons showed good agreement in the initial and thermal growth regions. In the initial growth region including surface tension controlled, transition and inertia controlled regions as divided by Robinson and Judd, the bubble growth rate showed that the bubble radius was proportional to $t^{2/3}$ regardless of working fluids and heating conditions. And in the thermal growth region as also called asymptotic region, the bubble showed a growth rate that was proportional to $t^{1/5}$, also. Those growth rates were slower than the growth rates proposed in previous analytical analyses. The required heat flow rate for the volume change of the observed bubble was estimated to be larger than the heat flow rate measured at the wall. Heat, which is different from the instantaneous heat supplied through the heating wall, can be estimated as being transferred through the interface between bubble and liquid even with saturated pool condition. This phenomenon under a saturated pool condition needs to be analyzed and the data from this study can supply the good experimental data with the precise boundary condition (constant wall temperature).