• 수산해양기술연구
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• 제19권1호
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• pp.40-45
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• 1983

전자식전발분사노즐로 급속압축장치 내에서 실현한 축대칭 자유분무.화염에 고속도 사진의 화상해석을 적용하여 다음과 같은 결론을 얻었다. 1. 고속도 사진의 화상해석에 의해 구한 디이젤분무의 축방향의 연료농도분포는 분무의 선단부를 제외하면 준정상이론에 의한 분포와 정성적으로 일치한다. 2. 화염중심축방향의 그을음 농도는 연과의 농도가 비교적 낮은 분무의 선단부에서 높은 농도를 나타내며, 그 농도는 거의 분사종료시에 최대로 되어, 그 후 시간경과에 따라 저하한다. 3. 양파모델을 축대칭 분무.화염에 적용하여 분무.화염내부의 반경방향의 그을음 농도와 연료농도분포를 비교해 보면 그을음 농도의 가장 높은 부분은 연료농도가 가장 높은 중심부보다 화염반경의 2/3의 위치에서 최대로 되었다

• 한국자동차공학회논문집
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• 제11권5호
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• pp.60-69
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• 2003

The simplified two-color method is proposed which can estimate the temperature distribution and the soot density of the whole flame with the image analysis of the high-speed photographs. The factors influenced on its processing were examined, for example, the selection of the wave length, the kind of films, the preparation of the calibration curve between the radiance of flame and the luminance temperature. The simplified two-color method reported in this paper can be used as a tool for the improvement of the combustion process in direct injection diesel engine.

• 수산해양기술연구
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• 제31권4호
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• pp.372-378
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• 1995

건착망의 침강 운동특성을 구명하기 위한 기초연구로서 그물감의 재료가 다른 세 종류의 건착망을 수중 총중량(60g)이 동일하게 되도록 발돌의 양을 조절하여 제작하고, 침강특성을 해석하였다. 실험에 사용한 건착망은 그물실의 직경 및 발의 길이가 같은 폴리프로피렌계(밀도 0.91g/$cm^3$) 및 폴리에스터계(밀도 1.38g/$cm^3$)의 매듭 없는 그물감을 사용하여, 뜸줄의 길이를 420cm, 그물의 폭을 86cm가 되도록 제작하고, 이 그물들을 각각 PP, PA 및 PES 그물이라고 하였다. 회유수조의 수로상에 투망장치를 설치해서 정지상태의 수중에 투망하고, 측면에 설치한 비디오 카메라를 이용하여 촬영 녹화하였다. 그리고, 그물에 표시한 측정점의 좌표를 화상해석장치로 읽고 실험치를 구하였다. 여기에는, 건착망의 수직방향의 침강운동을 나타내는 미분방정식을 구하고 Runge-Kutta-Gill법에 의한 연립 미분방정식 해법을 이용하여 수치해석을 행하였으며, 그 결과는 다음과 같다. 1. 그물 아랫자락의 침강속도는 PP 그물이 가장 빠르고, PA 및 PES 그물 순으로 늦게 나타났다. 2. 그물감의 저항계수 $K_D$는 계산결과 $K_D=0.061({\frac{\rho}{{\rho}_w}})^4$의 관계식으로 나타낼 수 있었다. 3. 그물다발의 저항계수 $C_R$은 계산결과 $C_R=0.91({\frac{\rho}{{\rho}_w}}$의 관계식으로 나타낼 수 있었다. 4. 건착망 투망후 경과시간에 따른 그물 아랫자락의 도달수심에 대한 실험치와 계산치는 매우 잘 일치하여 meas.=0.99cal.의 관계였다.

• 대한기계학회논문집
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• 제19권6호
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• pp.1382-1390
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• 1995

Electronic Speckle Pattern Interferometry (ESPI) with a CW laser, a video system and an image processor was utilized to measure the in-plane displacement. Unlike traditional strain gauges or Moire method. ESPI method measure the in-plane displacement on real time with out any surface preparation on surface attachment. The specimen has a crack of 10*0.1 mm in the middle of plate and strain gauge was also attached on that surface to compare with ESPI method. This study reveled the ESPI method to measure the displacement and distribution of strain in the specimen. It was shown in tensile tests that the measurement by ESPI method was comparable with strain gauge.

• 한국통신학회논문지
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• 제17권5호
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• pp.433-441
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• 1992

기본 주파수가 155.5.Mbit/s 인 새로운 동기식통신망에서 비동기화상신호를 다중화하여 전송하기 위하여 스타핑동기방식이 사용될 것이다. 본 연구에서는 스타핑장치의 시스템파라메터에 따라 발생될 지터의 실효치와 전력스펙트럼을 수치 해석적으로 구하였다. 분석 결과 실제 발생되는 지터는 지금까지 생각되어오던 이상적인 지터 보다 그 크기가 더 큰 것이 밝혀졌다.

• 한국분무공학회지
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• 제1권4호
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• pp.32-39
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• 1996

Fuel spray in the MPI gasoline injector and its atomization characteristics are investigated with both macroscopic and microscopic visualization systems. The Bosch injector is inserted into an air-assist spray adapter which is designed to be fabricated and assembled easily. particle motion analysis system is used to measure the SMD of injector, where the assistant air pressure is varied from 0.0 to 1.5bar with fuel pressure 2.8bar. Droplet size decreased with higher air pressure and fine fuel spray with below $60{\mu}m$ of SMD is acquired at the assistant air pressure over 0.5bar.

• 한국분무공학회지
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• 제3권4호
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• pp.16-24
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• 1998

The fuel injection type, in the gasoline engines of atomization of fuel droplet and its distribution hae influenced directly on the decision of engine performance and harmful emission. In this paper, atomization characteristics of fuel spray is investigated with microscopic visualization system. Particle motion analysis system is used to measure the SMD from fuel spray of air-assisted injector by initial factors such as temperature of ambient air and air-assisted pressure. As air-assist pressure and ambientair temperature increase, the SMD is decreased, and its variation is more stable.

• 대한기계학회논문집
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• 제14권5호
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• pp.1222-1233
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• 1990

본 연구에서는 급속압축장치에서 실현된 단발분무하염내의 매연을 레이저음영 사진법에 의하여 가시화하고, 화염내의 매연농도의 시간적, 공간적분포를 조사한다. 또 전보에서 측정된 비증발분무내의 당량비분포와 비교검토하여 디젤화염내의 매연 생 성기구를 고찰하고, 분위기조건에 따른 착화지연이 매연생성에 미치는 영향 및 매연생 성과 열발생율과의 관계를 밝힌다.

• 한국분무공학회지
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• 제3권4호
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• pp.58-64
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• 1998

In the gasoline engine of fuel injection type, atomization of fuel droplet and its distribution has directly influenced the performance of engine and harmful emission. To investigate atomization characteristics of fuel spray, in this paper fuel spray of air-assisted injector is observed at the various initial conditions of ambient air temperature and air assisted pressure. Behavior of fuel spray is photographed with microscopic visualization system. The SMD of fuel droplet is measured with PMAS (Particle Motion Analysis System). The effect of air-assisted pressure and temperature of ambient air resulted in the decrement of SMD and its variation. Finally, It was found that It was found that from spray angle at the two-hole injector had measured $20{\pm}4$ degree the result of photographs by shadow graphy. The mean diameter of suns decreased and the of droplets increased with increasing the temperature in the spray fields by the results of PMAS measurement. It was found that the characteristics of sprays became finer by increasing the temperature of spray fields about 373K without the delivery of air-assistance.

• 한국분무공학회지
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• 제13권4호
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• pp.212-219
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• 2008

To develop the twin-fluid atomizer having the excellent performance of painting, the spray characteristics of how a wide area can be painted efficiently by one time spraying were studied in this paper. Spray phenomena are affected by the many factors determining the spray field such as the spraying pressure of gas, the spraying pressure and viscosity of liquid paints, the opening duration of needle valve, the design dimension of nozzle, and so on. As the results of experiments, these factors affecting on spray characteristics were suggested as followings; 1) The optimum spraying pressure of gas was $0.015{\sim}0.02\;kPa$, and the appropriate spraying pressure of liquid paint was 0.01kPa, In these situations, the setting up pressures must be compensated as much as the losing amount of pressure because a decompression occurred when operating valves. 2) The duration of opening the needle valve must be sustained for $1{\sim}2$ seconds to inject gas after spraying the liquid paint. This operating of the needle valve was necessary to avoid the affect on the changing of liquid column length, and to prevent the droplet deposit at the initial time of spraying. 3) The spray tip penetration was gained form the experimental equation, and the effective spraying angle was $85^{\circ}{\pm}5^{\circ}$ just at he appropriate spraying pressure of gas. The distribution of the area sprayed had the variation in $350{\pm}50\;mm$ because of the spraying pressure of gas, the its distance from the spray tip, and the lift of the needle valve.