• 제목/요약/키워드: 분무 화염

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APU 가스터빈엔진 압력식 스월인젝터의 분무특성 (Spray Characteristics of the Pressure Swirl Injector for the APU Gas Turbine Engine)

  • 최채홍;최성만;임병준
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2007년도 제29회 추계학술대회논문집
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    • pp.359-364
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    • 2007
  • APU 가스터빈엔진의 연료분무특성을 연구하였다. 지상 및 고도 작동조건에 대한 연료분무특성 실험을 수행하여 APU 엔진의 실화 가능성을 검토하였다. 분무실험은 4개의 작동조건에 대하여 수행되었으며 각 조건은 지상 무부하 및 통합부하 조건과 고도 20,000 feet 무부하 및 통합부하에 대한 실험을 수행하였다. 분무특성은 PDPA를 이용한 입자의 크기 및 속도 측정과 레이저 빔을 이용한 가시화를 수행하였다. 연구결과 20,000 feet 무부하의 경우 입자의 크기가 100 ${\mu}m$정도이며 분무속도가 10 m/s로 낮아 화염안정성을 위한 개선이 필요할 것으로 판단된다.

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이류체 노즐형 화염 반응기에 의한 실리카 나노분말 제조 (Controlled synthesis of silica nanoparticles by a two-fluid nozzle flame reactor)

  • 장한권;장희동;장원철
    • 한국자원리싸이클링학회:학술대회논문집
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    • 한국자원리싸이클링학회 2005년도 추계정기총회 및 제26회 학술발표대회 고분자리싸이클링기술 특별심포지엄
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    • pp.308-313
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    • 2005
  • 실리콘 잉고트의 절단공정에서 발생하는 폐실리콘 슬러지는 실리콘과 실리콘카바이드 등의 유가자원이 함유되어 있으며, 이 중 실리콘 분말은 실리콘 화합물인 알콕시실란 등을 제조하는데 원료로 사용이 가능하다. 본 연구에서는 폐실리콘 슬러지로부터 분리, 합성된 사에 톡시실란(TEOS)을 원료로 이용하여 실리카 나노분말을 합성하였다. TEOS 원료물질을 외부 혼합형 이류체 노즐을 이용하여 미세액적으로 분무하고 화염 속으로 도입시키고 화염열분해 반응을 진행시켜 실리카 나노분말을 합성하였다. 합성된 실리카 나노입자의 특성은 투과형 전자현미경 및 BET에 의하여 입자형상 및 평균 입자크기가 분석되었다. 주요 공정변수인 분산공기의 압력, 반응가스의 조성을 변화시켜 실험한 결과 평균크기가 $9{\sim}68nm$인 실리카 나노분말을 제조하였다.

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예혼합 분무화염내의 이중적 액적 연소속도에 관한 관찰 (Observation on Double-droplet Combustion Speed in Premixed Spray Flame)

  • 이치우;심한섭
    • 한국자동차공학회논문집
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    • 제12권6호
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    • pp.119-126
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    • 2004
  • In order to elucidate the modes of double-droplet combustion speed in premixed spray flame, the difference between flame propagation speed and droplet cluster disappearance speed are experimentally investigated using a premixed spray burner system, It was confirmed that flame speed concerned with premixed-mode combustion in the spray flame was approximately 2.0 m/s in average while mean disappearance speed of droplet clusters, which were dominated by diffusion-mode combustion in downstream of the flame, was evaluated as much as 0.45 m/s. It was clarified that both characteristics of premixed-mode and diffusion-mode combustion in spray flames are of much difference in nature, even though both speed, which are supposed to depend on local properties of the spray itself and flow conditions surrounding droplet clusters, are scattered in experiments.

초음파에 의해 무화된 케로신 분무연소에서의 OH 라디칼 및 CH 라디칼 자발광 특성 (OH-and CH-Radical Chemiluminescence Characteristics in the Spray Combustion of Ultransonically Atomized Kerosene)

  • 김민철;김정수
    • 한국추진공학회지
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    • 제22권1호
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    • pp.72-79
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    • 2018
  • 초음파 진동자에 의해 미립화된 케로신 분무연소의 OH 라디칼과 CH 라디칼의 자발광 특성을 고찰하기 위한 실험이 수행되었다. ICCD 카메라를 이용하여 분무화염의 자발광 강도를 측정하였으며, 연소 시 소모된 연료량은 정밀유량측정법으로 계측하였다. 그 결과, 연료소모율은 수송기체인 공기 공급유량에 선형적으로 증가하였으며, 분무연소의 특징인 전형적인 그룹 연소가 관찰되었다. OH 라디칼과 CH 라디칼을 분석한 결과, 분사방향으로의 유량 증가에 따라 라디칼 방사강도의 최댓값은 감소하고 그 위치는 후류로 이동하여 반응대의 폭은 증가하였다.

2유체 분사노즐을 이용한 분무 및 연소특성에 관한 실험적 연구 (An Experimental Study on the Characteristic of Sprays and Spray Flames by Twin-Fluid Atomizer)

  • 백민수;오상헌
    • 대한기계학회논문집
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    • 제19권2호
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    • pp.548-558
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    • 1995
  • An experimental investigation has been conducted to study the spray and combustion characteristics using the air-assisted twin fluid atomizer. Axial mean and fluctuating velocity components as well as drop-size distributions in non-reaction spray were measured with a nonintrusive phase doppler technique. Droplet number density distributions were also visualized using high speed CCD camera. Locations of spray and flame boundaries are obtained by direct photographic method. It is confirmed that at the fixed fuel flow rate, the increase of the atomizing air flow causes improvements on both spray and combustion characteristics under stable flame conditions. Internal group combustion modes where flame is located inside the spray boundary are observed to exist in the upstream region of higher droplet number density.

디젤엔진조건에서 DME분무의 연소특성 해석 (Parametric Study of DME Spray Combustion Characteristics in the Diesel-like Condition)

  • 배준경;강성모;김용모
    • 한국분무공학회지
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    • 제14권4호
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    • pp.163-170
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    • 2009
  • The present study has numerically investigates the vaporization, auto-ignition and combustion processes in the high-pressure and high-temperature conditions encountered in the diesel engine. In the present study, in order to understand the overall spray combustion characteristics of DME fuel as well as to identify the distinctive differences of DME combustion processes compared to conventional hydrocarbon liquid fuels, the sequence of the comparative analysis has been systematically made for DME and n-Heptane liquid fuels. Computations for DME fuel are made for two cases including constant fuel mass flow rate condition and fixed heat release rate. Based on numerical results, the discussions are made for the detailed combustion processes of DME and n-Heptane spray.

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연료 종류 및 당량비에 따른 Flame Spray 화염장의 열-유동 특성 연구 (Thermal and Flow Characteristics of Fluid with Fuel Type and Equivalence Ratio in Flame Spray Process)

  • 이재빈;김대윤;신동환;이성혁
    • 한국분무공학회지
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    • 제18권4호
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    • pp.202-208
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    • 2013
  • The present study aims to investigate the flow characteristics with respect to fuel type and equivalence ratio in the flame spray coating process. The flame spray flow is characterized by much complex phenomena including combustion, turbulent flows, and combined heat transfer. The present study numerically simulated the flam spray process and examined the gas dynamics involving combustion, gas temperature and velocity distributions in flame spray process by using commercial computational fluid dynamics (CFD) code of FLUENT (ver. 13.0). In particular, we studied the effect of fuel type and equivalence ratio on thermal and flow characteristics which could substantially affect the coating performance. From the results, it was found that the gas temperature distributions were varied with different fuels because of reaction times were different according to the fuel type. The equivalence ratio also could change the spatial flame distribution and the characteristics of coated layer on the substrate.

스파크점화직분식 CNG의 점화성 및 연소화염 특성에 대한 연구 (An Experimental Study on the Ignition Probability and Combustion Flame Characteristics of Spark-Ignited Direct-Injection CNG)

  • 황성일;정성식;염정국;전병열;이진현
    • 한국분무공학회지
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    • 제21권1호
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    • pp.37-46
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    • 2016
  • For the SI engines, at only full load, the pumping loss has a negligible effect, while at part load conditions, the pumping loss increases. To avoid the pumping loss, the spark-ignited engines are designed to inject gasoline directly into the combustion chamber. In the spark-ignited direct-injection engines, ignition probability is important for successful combustion and the flame propagation characteristics are also different from that of pre-mixed combustion. In this paper, a visualization experiment system is designed to study the ignition probability and combustion flame characteristics of spark-ignited direct-injection CNG fuel. The visualization system is composed of a combustion chamber, fuel supply system, air supply system, electronic control system and data acquisition system. It is found that ambient pressure, ambient temperature and ambient air flow velocity are important parameters which affect the ignition probability of CNG-air mixture and flame propagation characteristics and the injected CNG fuel can be ignited directly by a spark-plug under proper ambient conditions. For all cases of successful ignition, the flame propagation images were digitally recorded with an intensified CCD camera and the flame propagation characteristics were analyzed.

가솔린 기관(機關)의 혼합기(混合氣) 성분(成分)이 출력(出力)에 미치는 영향(影響) (점화지연(点火遲延) 및 연소(燃燒) 기간(期間)에 미치는 영향(影響)) (The Effect of Mixture Component in a Gasoline Engine on Output (The Effect of Ignition Delay and Combustion Period))

  • 송재익
    • 한국분무공학회지
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    • 제3권1호
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    • pp.19-26
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    • 1998
  • The effect of mixture component makes a nelay time and a long total combustion period $\tau_{p\;max}$. The flame propagation delay $\tau_{df}$ was determined by the record of current ion. The pressure release delay $\tau_{dp}$ and $\tau_{p\;max}$ were determined by the indicated pressure diagram in constant volume of the combustion chamber. The results are as follows: 1) The ignition delay $\tau_t$ time takes the minimum value around $\Phi=1.15$. 2) $\tau_{df}$ and $\tau_t$ time increased according to the increases of the concentrated dilution gases, because the adiabatic flame temperature decreased due to the increases of the heat capacity. But dilution gases have little effect on flame nucleus formation delay 3) The relation between $\tau_t$ time and reciprocal laminar burning velocity is almost linear. 4) The increase of the propagation length is accompanied with increased ratio of the $\tau_{df},\;\tau_{dp},\;\tau_{t},\;\tau_{p\;max}$.

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