• 한국자동차공학회논문집
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• 제14권2호
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• pp.100-106
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• 2006

The behavior of spray impinging on the inclined constant temperature flat plate was experimentally investigated. To clarify the wall effect of a high pressure DISI injector, a relative angle of the inclined wall to a spray axis was varied. Spray penetration along the wall was observed optically and it was compared with that of a Fan spray type and Swirl type spray. To evaluate various spray motion quantitatively, a spray path penetration which describe the development of a spray tip along the wall was newly introduced. To observe the structure of an impinging spray, it was visualized by a controlled stroboscope light and its visualized image was captured on an CCD camera. Using the digital image of impinging spray $H_x$ and $R_x$ was extracted to clarify the structure of impinging spray. The main parameter of the relative position of the wall was the inclined angle which was defined as the angle was varied from $0^{\circ}$ (vertical impingement) to $60^{\circ}$ at the same condition.

• 한국추진공학회지
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• 제14권5호
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• pp.24-31
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• 2010

충돌형 분사기가 장착된 모델 연소실에서 연소장 수치 해석을 이용하여 연소 안정성을 평가하였다. 충돌형 분사기로는 F(fuel)-O(oxidizer)-O-F형 분사기를 채택하였다. 본 연구에서는 연료와 산화제의 제트 혼합과정이 지배적이라는 가정하에 순간 화학 반응 모델을 채택하여 수치해석을 수행하였다. 선행 연구를 통해 제안된 방법론을 토대로 모델 연소실 형상이 설계되고 연소실 작동 조건이 결정되었다. 본 연구에서 제시한 방법을 토대로 얻은 연소 안정성 경계는 공기 분사 음향 실험과 연소 실험결과와 정성적으로 잘 일치하였다. 연료와 산화제의 분사와 혼합이 연소 불안정 유발에 지배적인 경우, 본 연구에서 제안된 수치해석 기법을 이용하여 효과적으로 분사기의 연소 안정성을 평가할 수 있다.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2003년도 제21회 추계학술대회 논문집
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• pp.195-203
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• 2003

실물형 Unlike 충돌형 triplet 분사기인 F-O-F형과 O-F-O형의 분무특성 및 혼합특성을 실험적으로 알아보았다. 각각의 분사기에 대해 산화제와 연료의 운동량비의 변화에 따라 분무형상과 케로신/물을 이용한 혼합효율을 측정하였다. 분무형상은 Stroboscope와 CCD camera를 이용한 직접사진기법으로, 혼합효율은 Mechanical Patternator를 이용하였다. O-F-O형 분사기가 미립화 특성이 우수함을 알 수 있었고, 운동량비가 증가함에 따라 혼합효율이 급격히 감소함을 알 수 있었다.

• 한국분무공학회지
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• 제7권1호
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• pp.21-28
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• 2002

The mixing of propellant and its mass distribution of unlike-doublet impinging injector, which is known to affect the combustion efficiency significantly, have been studied using PLIF(Planar Laser Induced Fluorescence). The results show that fuel jet penetrates considerably into the oxidizer jet at impinging point as variation of momentum ratio. and then stream flows inclined because of variation of momentum ratio. Consequently, the mixing efficiency shows that maximum efficiency is at MR=3. after MR=3, mining efficiency decreases slightly.

• International Journal of Automotive Technology
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• 제7권5호
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• pp.585-593
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• 2006

The effect of the shape of the side wall on vaporization and fuel mixture were investigated for the impinging spray of a direct injection(DI) gasoline engine under a variety of conditions using the LIEF technique. The characteristics of the impinging spray were investigated under various configurations of piston cavities. To simulate the effect of piston cavity configurations and injection timing in an actual DI gasoline engine, the parameters were horizontal distance from the spray axis to side wall and vertical distance from nozzle tip to impingement plate. Prior to investigating the side wall effect, experiments on free and impinging sprays for flat plates were conducted and these results were compared with those of the side wall impinging spray. For each condition, the impingement plate was located at three different vertical distances(Z=46.7, 58.4, and 70 mm) below the injector tip and the rectangular side wall was installed at three different radial distances(R=15, 20, and 25 mm) from the spray axis. Radial propagation velocity from spray axis along impinging plate became higher with increasing ambient temperature. When the ambient pressure was increased, propagation speed reduced. High ambient pressures tended to prevent the impinging spray from the propagating radially and kept the fuel concentration higher near the spray axis. Regardless of ambient pressure and temperature fully developed vortices were generated near the side wall with nearly identical distributions, however there were discrepancies in the early development process. A relationship between the impingement distance(Z) and the distance from the side wall to the spray axis(R) was demonstrated in this study when R=20 and 25 mm and Z=46.7 and 58.4 mm. Fuel recirculation was achieved by adequate side wall distance. Fuel mixture stratification, an adequate piston cavity with a shorter impingement distance from the injector tip to the piston head should be required in the central direct injection system.

• 한국자동차공학회논문집
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• 제9권5호
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• pp.54-61
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• 2001

It is reported that during the cold starting, especially in gasoline engine, the engine response and the effect of HC emission can be improved by prompting atomization and reducing the quantity of fuel adhered to the range of injector tip, inlet port, and inlet valve. The purposes of this study are to promote atomization of fuel before air-fuel mixture in the inlet port. In order to achieve its goal, the glow plug is to evaluate the feasibility of for the early fuel evaporator and the spray behavior characteristics of gasoline, injected on the surface of glow plug with room temperature(2$0^{\circ}C$) and high temperature(25$0^{\circ}C$) is to examine. Particle motion analysis system(PMAS) was used to measure the SMD and the dropsize distribution of impinging spray and free spray. The results of this experiment, evaporation rate of impinging spray was higher than that of free spray, and the higher evaporation rate win, the smaller peak dropsize was. Especially, during early spray SMD of impinging spray was still smaller than that of fee spray.

• Journal of Mechanical Science and Technology
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• 제20권6호
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• pp.874-881
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• 2006

Combustion stability characteristics in actual full-scale combustion chamber of a rocket engine are investigated by experimental tests with the model (sub-scale) chamber. The present hot-fire tests adopt the combustion chamber with three configurations of triplet impinging-jet injectors such as F-O-O-F, F-O-F, and O-F-O configurations. Combustion stability bound-aries are obtained and presented by the parameters of combustion-chamber pressure and mixture (oxidizer/fuel) ratio. From the experimental tests, two instability regions are observed and the pressure oscillations have the similar patterns irrespective of injector configuration. But, the O-F-O injector configuration shows broader upper-instability region than the other configurations. To verify the instability mechanism for the lower and upper instability regions, air-purge acoustic test is conducted and the photograph or the flames is taken. As a result, it is found that the pressure oscillations in the two regions can be characterized by the first impinging point of hydraulic jets and pre-blowout combustion, respectively.

• 한국추진공학회지
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• 제17권5호
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• pp.86-94
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• 2013

로켓의 연소불안정과 관련되어 분사기의 동특성을 연구하는 일은 중요하다. 와류형 분사기의 동특성에 대해서는 많은 연구가 이루어졌지만 충돌형 분사기의 동특성에 대해서는 알려진 바가 거의 없다. 따라서 본 연구에서는 충돌형 분사기의 동특성을 규명하기 위해 이에 관한 실험을 수행하였으며 동적거동을 생성시키기 위해 특별히 제작된 압력섭동기(mechanical pulsator)가 사용되었다. 가진주파수와 매니폴드 압력의 여러 조건 하에서 게인(gain)과 위상차(phase difference)를 분석하였고 주파수는 5, 10, 15 Hz의 낮은 영역에 맞춰졌다. 제트 속도를 결정하기 위한 방법에 대해 논의하였으며 실험과정 중에 나타난 특정현상이 클라이스트론(Klystron) 효과와 관련이 있는 것으로 판단되어 이에 대해 고려하였다.

• 한국추진공학회지
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• 제5권3호
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• pp.41-51
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• 2001

Split-triplet(F-O-O-F)형의 분사기 요소를 장착한 KSR-III 액체 로켓엔진의 성능과 연소장을 고찰하기 위해 수치해석을 수행하였다. 방사형 분사기 배열의 액체 로켓엔진의 수치해석 검증을 위해 2차원 축대칭과 3차원 계산을 수행하여 연소시험 결과와 비교하였다. 2차원 축대칭 계산과 3차원 해석을 통하여 성능 측면에서 오차가 약 3∼5% 정도의 정확도를 유지하며 예측하는 것을 볼 수 있었다. 3차원 해석에서는 연소장을 해석하여 분사기 면의 온도 분포가 연소 시험결과와 정성적으로 일치하는 것을 볼 수 있었다. 또한 충돌각의 감소와 분사기 배열의 직교-방사형으로 변경이 방사형 분사기배열의 국부적인 고온 영역을 감소시키며 성능에도 영향을 미치는 것을 볼 수 있었다. 이러한 해석을 통하여 분사기 배열과 충돌각 선정이 액체 로켓엔진의 성능과 연소장에 영향을 미치는 중요한 요인이 됨을 알 수 있었다.

• 한국분무공학회지
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• 제5권1호
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• pp.41-48
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• 2000

In this research, the velocity distribution of the liquid sheet formed by two impinging jets at low velocities are measured using LDV. The spatial distribution of the sheet velocity as well as the effects of impinging anlge and jet velocity on the sheet velocity are examined. The sheet velocity is highest along the sheet axis and it decreases with the increase of the azimuthal angle. With the increase of the impinging angle, the average sheet velocity is decreased due to the increased impact momentum. The average sheet velocity is proportional to the jet velocity but it is always higher than the jet velocity. This result is against the fact that the sheet velocity can be assumed to be equal to the jet velocity in the previous researches.