• 제목/요약/키워드: Distributed Reaction Zone

검색결과 14건 처리시간 0.022초

평면전단층의 난류예혼합 화염의 구조에 관한 실험적 연구 (A study of turbulent premixed flame structure in a plane shear layer)

  • 이재득;최병륜
    • Journal of Advanced Marine Engineering and Technology
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    • 제13권4호
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    • pp.33-39
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    • 1989
  • A turbulent premixed flames of layer formed between burned hot gas and unburned mixture were investigated by means of schlieren photograph with fluctuations of temperature and ion current. The combustion intensity between burned hot gas and shear layer was higher than the intensity between unburned mixture and shear layer. A wrinkled laminar flame and flamelet were appeared at downstream to exist and distributed reaction zone was at upstream as a result of analyzed probability density functions of temperature fluctuation. The initial combustion intensity of reaction zone of eddy between burned hot gas and shear layer was higher than that of final, flowing downstream, and vice versa between unburned mixture and shear layer.

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이중분류버너화염의 미세구조에 관한 실험적 연구 (An experimental study on microstructure of doubled jet burner flame)

  • 장인갑;최경민;최병륜
    • 대한기계학회논문집B
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    • 제20권7호
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    • pp.2337-2346
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    • 1996
  • One of the most useful method for increasing combustion loading of premixed flame is to strengthen the turbulent intensity of unburned mixture. It produces an important information to a design of efficient combustion equipment that analysing microstructure of strong turbulence premixed flame. The flame structure and characteristics are depend on the turbulence of unburned mixture. Therefore, to strengthen the turbulent intensity of unburned mixture make flame scale small and accomplish efficient combustion. We measured the velocity of local flame front movements, local eddy radius and local reaction zone thickness quantitatively with increasing turbulent intensity of unburned mixture. We researched the microstructure of flame using ion currents that react sensitively in the reaction zone. Consequently, the velocity of local flame front movements is depend on the velocity of unburned mixture and local eddy scale is to be small with increasing turbulent intensity. But there is no change in local reaction zone thickness with turbulence.

영역분할조건평균법을 이용한 난류예혼합화염내 난류운동에너지 생성에 관한 연구 (Analysis of Flame Generated Turbulence for a Turbulent Premixed Flame with Zone Conditional Averaging)

  • 임용훈;허강열
    • 한국연소학회지
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    • 제8권4호
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    • pp.15-23
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    • 2003
  • The zone conditional two-fluid equations are derived and validated against DNS database of a premixed turbulent flame. The conditional statistics of major flow variables are investigated to understand the mechanism of flame generated turbulence. The flow field in burned zone shows substantially increased turbulent kinetic energy, which is highly anisotropic due to reaction kinematics across thin f1amelets. The transverse component may be larger than the axial component for a distributed pdf of the flamelet orientation angle, while the opposite occurs due to redistribution of turbulent kinetic energy and flamelet orientation normal to the flow at the end of a flame brush. The major source or sink terms of turbulent kinetic energy are the interfacial transfer by the mean reaction rate and the work terms by fluctuating pressure and velocity on a flame surface. Ad hoc modeling of some interfacial terms may be required for further application of the two-fluid model in turbulent combustion simulations.

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CMC 모델 기반 수치해석을 사용한 순산소 난류확산화염 구조 연구 (A Study on the Structure of Turbulent non-Premixed Oxy-fuel Flame Using CMC Model-based Simulation)

  • 김종수;;허강열;양원
    • 한국연소학회지
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    • 제13권1호
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    • pp.31-43
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    • 2008
  • Oxy-fuel flame has a significantly different structure from that of air-fuel flame because of its high temperature. This study is aimed to find out the difference of the oxy-fuel flame structure in order to understand reaction mechanism closely, which is crucial to design real-scale oxy-fuel combustion system. By examining pictures of counterflow flame and LIF images, we found that oxy-fuel flame had two-zone structure: fuel decomposition region and distributed CO oxidation region. In the oxy-fuel flame, OH radical was distributed intensely through the whole flame due to its higher flame temperature than crossover temperature. For showing those features of the oxy-fuel flame, 1 MW scale IFRF oxy-natural gas burner was simulated by conditional moment closure(CMC) model. Calculation results were compared with experimental data, and showed agreements in trend. In the simulated distributions of fuel decomposition/CO oxidation rates, CO oxidation region was also separated from fuel decomposition zone considerably, which showed the two-zone structure in the oxy-fuel flame.

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유선형 스텝에 의해 안정화된 예혼합화염의 구조와 연소특성에 관한 연구 ($\Pi$) (A Study on the Flame Structure and Combustion Charactexistics of a Premixed Flame Stabilized by a Streamline Step( $\Pi$))

  • 이재득;최병륜
    • 대한기계학회논문집
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    • 제14권6호
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    • pp.1661-1668
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    • 1990
  • 본 연구에서는 코히런트 와(渦)에 지배되는 난류 예혼합화염의 미세구조를 밝 히기 위해 슐리이렌사진과 온도, 이온전류의 3가지를 동시에 측정하고, 그 변동량을 통계처리, 분석하여, 미시적인 화염구조 모델을 제시하고자 한다.

미연혼합기의 난류특성과 이중분류버너화염의 연소특성에 관한 실험적 연구 (An experimental study on turbulence characteristics of mixture and combustion characteristics of doubled jet burner flames)

  • 최경민;장인갑;최병륜
    • 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.

미연혼합기의 난류특성과 화염 스케일에 관한 실험적 연구 (An experimental study on characteristics of mixture turbulence and flame scale)

  • 최병륜;장인갑;최경민
    • 대한기계학회논문집B
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    • 제20권3호
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    • pp.1040-1049
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    • 1996
  • The high loading combustion is accomplished by making the turbulent intensity strong and the scale small in the premixed combustor. The Da-mkoler number, which is decreased by short turbulent characteristic time or by long chemical reaction time, can make the distributed reaction flame. So we developed a doubled jet burner for high loading combustion. The doubled jet burner was designed to make the scale of the flame small by the effect of impingement and increasing shear stress with doubled jet. We investigated the turbulence characteristics of unburned mixture and visualized several flames with the typical schlieren photography. Then we studied the influence of several factors that related the scale of flame. Consequently, the doubled jet burner can make the eddy very small. And we can obtain the detail information of the flame scale through ADSF(the Average Distance between Successive Fringes) in the micro- schlieren photography. The ADSF is not a exact flame scale, but it has qualitative trend with increasing turbulent intensity. The ADSF is diminished remarkably with increasing turbulent intensity. The reason is that strong turbulent intensity makes the flame zone thick and flamelets numerous. We can confirm this fact by the signal analysis of ion currents.

확대유로내의 Bluff-Body 후류확산화염의 구조 및 특성 (1) (Structure and Characteristics of Diffusion Flame behind a Bluff-Body in a Divergent Flow(I))

  • 최병륜;이중성
    • 대한기계학회논문집
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    • 제19권5호
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    • pp.1269-1279
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    • 1995
  • An experimental study is carried out on turbulent diffusion flames stabilized by a circular cylinder in a divergent duct flow. A commercial grade gaseous propane is injected from two slits on the rod as fuel. Flame stability limits, as well as size and temperrature of recirculation zone, are measured by direct and schlieren photographs to clarify the characteristics and structure of diffusion flames and to assess the effect of various divergent angle of duct. The results of the present study are as follows. Temperature in the recirculation zone decreases with increasing divergent angle. The blow-off velocity in parallel duct is higher than that in divergent duct. Critical blow-off velocity is expected to be about 8-12 degree through blow-off velocity pattern. Regardless of divergent angles, the length of recirculation zone is nearly constant, and this length becomes longer with rod diameter. Pressure gradient has an effect on the eddy structure in shear layer behind the rod. With the increase of divergent angle, large scale eddies by dissipated energy in shear layer are split into small scale eddies, and the flame becomes a typical distributedreacting flame.

용탕단조에 의한 $Al_2O_3-SiO_2$ 단섬유 및 SiC whisker강화 알루미늄 합금기 복합재료의 제조 (Fabrication of Aluminum Alloy Composites Reinforced with SiC whisker an $Al_2O_3-SiO_2$ Short Fiber by Squeeze Casting)

  • 홍성길;윤중렬;최정철
    • 한국주조공학회지
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    • 제17권1호
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    • pp.28-35
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    • 1997
  • SiC whisker and $Al_2O_3-SiO_2$ short fiber reinforced AC8A, AC8B and AC8B(J) marix composites were fabricated by squeeze casting method. Preform deformation, change of reinforcement volumefraction and formation of macro-segregation in two composites were investigated by using micro Vickers hardness test, analysis of macro and micro structures with OM, SEM and EDAX. $Al_2O_3-SiO_2$ short fiber preform manufactured with 5% $SiO_2$ binder in this study was considerably deformed and cracked, nevertheless, the short fibers were distributed homogeneously in the composites. In SiC whisker reinforced composites, on the other hand, preform deforming and cracking were not occurred, however, macro segregation zone formed along the infiltration routes by interface reaction during infiltration of molten metal into the preform was observed at center-low area in the composites. The decrease of hardness in the macro segregation zone resulted from the depletion of Si and Mg atoms.

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Numerical analysis of NOx reduction for compact design in marine urea-SCR system

  • Choi, Cheolyong;Sung, Yonmo;Choi, Gyung Min;Kim, Duck Jool
    • International Journal of Naval Architecture and Ocean Engineering
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    • 제7권6호
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    • pp.1020-1033
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    • 2015
  • In order to design a compact urea selective catalytic reduction system, numerical simulation was conducted by computational fluid dynamics tool. A swirl type static mixer and a mixing chamber were considered as mixing units in the system. It had great influence on flow characteristics and urea decomposition into ammonia. The mixer caused flow recirculation and high level of turbulence intensity, and the chamber increased residence time of urea-water-solution injected. Because of those effects, reaction rates of urea decomposition were enhanced in the region. When those mixing units were combined, it showed the maximum because the recirculation zone was significantly developed. $NH_3$ conversion was maximized in the zone due to widely distributed turbulence intensity and high value of uniformity index. It caused improvement of $NO_x$ reduction efficiency of the system. It was possible to reduce 55% length of the chamber and connecting pipe without decrease of $NO_x$ reduction efficiency.