• 제목/요약/키워드: Interaction of Flames

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Flamelet 및 CMC 모델을 이용한 재순환 비예혼합 난류 화염장의 해석 (Flamelet and CMC Modeling for the Turbulent Recirculating Nonpremixed Flames)

  • 김군홍;강성모;김용모;김성구
    • 한국연소학회:학술대회논문집
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    • 한국연소학회 2004년도 제28회 KOSCO SYMPOSIUM 논문집
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    • pp.75-82
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    • 2004
  • The conditional moment closure(CMC) model has been implemented in context with the unstructured-grid finite-volume method which efficiently handle the physically and geometrically complex turbulent reacting flows. The validation cases include a turbulent nonpremixed $CO/H_2/N_2$ Jet flame and a turbulent nonpremixed $H_2/CO$ flame stabilized on an axisymmetric bluff-body burner. In terms of mean flame field, minor species and NO formation, numerical results has the overall agreement with expermental data. The detailed discussion has been made for the turbulence-chemistry interaction and NOx formation characteristics as well as the comparative performance for CMC and flamelet model.

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스월이 부분예혼합 상호작용화염의 화염날림 유속에 미치는 영향 (The Effect of Swirl on the Blowout Velocities of Partially Premixed Interacting Flames)

  • 이병준;최광덕
    • 한국연소학회지
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    • 제14권2호
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    • pp.26-31
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    • 2009
  • Adding small amounts of air to the fuel is used in many commercial combustors to avoid sooty flame. But partially premixed jet flame has lower blowout velocity, $u_{b.o}$, than nonpremixed one. Increasing blowout limit would be one of the key factors to develope highly intense compact combustion devices. Swirling flow enhances fuel and air mixing and induces a highly turbulent recirculation zone, which helps flame stabilization. It was known that NOx emission decreases with swirl on the proper range of swirl number. And it was shown that the flame interaction in multiple jets also increases $u_{b.o}$ owing to the internal recirculation and reduces NO emission. If the effects of swirl and flame interaction are combined together in partially premixed flame, both $u_{b.o}$ increasement and NOx emission reduction could be achieved. Blowout limits of partially premixed interacting propane flame in the swirling air coflow are investigated experimentally. The results show that the flame is not extinguished up to the experimental limits, 210 m/s, at the swirl number of 0.32 and $X_{F,o}$ = 0.46.

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덤프 연소기내의 와류-열방출의 관계에 대한 Damkohler 수의 영향 (Effect of Damkohler Number on Vortex-Heat Release Interaction in a Dump Combustor)

  • ;윤영빈;안규복
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2004년도 제23회 추계학술대회 논문집
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    • pp.137-140
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    • 2004
  • 주기적인 와류화염과 열방출 진동의 연관성에 대한 실험적인 연구가 수행되었다. 난류제트화염은 덤프 연소기에서 재순환 되는 뜨거운 생성물에 의해서 안정화되며, 큰 스케일의 주기적 와류가 음파에 의해서 제트화염에 부가되었다. 실제적인 연소기에서의 불안정 현상을 모사하기 위해 가진주파수와 실험변수들을 조절하였다. 본 연구의 목적은 원치 않는 열방출의 진동을 유도시키는 와류-열방출의 연관성을 분석하여, 연소불안정의 능동제어를 위해 사용될 수 있는 알맞은 연료분사 패턴을 조사하는 것이다. 주기적인 패턴을 측정할 수 있는 슐리렌 기법과 CH* chemiluminescence 기법이 사용되었으며, 실험결과는 와류 생성 사이클의 위상에 따라서 서로 비교되었다.

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액적배열연소의 상호간섭에 관한 실험적 연구 (An Experimental Study About Interaction of Droplet Array Combustion)

  • 김흥식;백승욱;박준성
    • 대한기계학회논문집B
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    • 제26권10호
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    • pp.1355-1363
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    • 2002
  • An experimental study was conducted to investigate the interaction phenomena of droplet array combustion in ambient environment. The droplet with 1 mm in diameter was supported from an optical fiber and ignited with a hot wire. Combustion lifetimes and burning rate constants were measured for fuel of nheptane according to parameters, which were junction and suspender spacings, and array configuration. Results show that the burning process considerably depends on the initial away configuration. The d$^2$-law is found to be correct when applied to both of the droplets in away and the single droplet. For separation distance of about 5mm, there exists a critical state. So the transition from a merged flame to separated flames occurs and burning velocity is much faster than before. Combustion lifetime of the lower droplet is shorter than that of the upper droplet in the two-dimensional arrays combustion. Burning rate constants of the droplets in arrays are smaller than that of the single droplet, while they become higher as separation distance increases. Combustion lifetimes of the droplets in arrays are longer than that of the single droplet and decrease as separation distance increase. It is concluded that the array configuration and the mergedness of the flame are the most important factors governing multi-droplet combustion.

와동과 상호작용하는 대향류 비예혼합화염의 비정상 응답특성 (Unsteady Response of Counterflow Nonpremixed Flames Interacting with a Vortex)

  • 오창보;박정;이창언
    • 한국연소학회지
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    • 제9권2호
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    • pp.10-17
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    • 2004
  • A two-dimensional direct numerical simulation is performed to investigate the flame structure of $CH_4/N_2-Air$ counterflow nonpremixed flame interacting with a single vortex. The detailed transport properties and a modified 16-step augmented reduced mechanism based on Miller and Bowman#s detailed reaction mechanism are adopted in this calculation. To quantify the strain on flame induced by a vortex, a scalar dissipation rate (SDR) is introduced. The results show that fuel-side and air-side vortex cause an unsteady extinction. In this case, the flame interacting with a vortex is extinguished at much larger SDR than steady flame. It is also found that air-side vortex extinguishes a flame more rapidly than fuel-side vortex. The unsteady effect induced by flame-vortex interaction does not lead to a transient OH overshoot of the maximum steady concentration observed in experiment, while $HO_2$ radical increases more than the maximum steady concentration with increasing SDR. In addition, it is seen that NO and $NO_2$ are not sensitive to the unsteady variation of SDR.

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와동과 상호작용하는 대향류 비예혼합화염의 비정상 응답특성 (Unsteady Response of Counterflow Nonpremixed Flames Interacting with a Votex)

  • 오창보;박정;이창언
    • 한국연소학회:학술대회논문집
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    • 한국연소학회 2002년도 제24회 KOSCO SYMPOSIUM 논문집
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    • pp.52-60
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    • 2002
  • A two-dimensional direct numerical simulation is performed to investigate the flame structure of $CH_4/N_2-Air$ counterflow nonpremixed flame interacting with a single vortex. The detailed transport properties and a modified 16-step augmented reduced mechanism based on Miller and Bowman's detailed reaction mechanism are adopted in this calculation. To quantify the strain on flame induced by a vortex, a scalar dissipation rate (SDR) is introduced. Results show that the fuel and air-side vortex cause an unsteady extinction. In this case, the flame interacting with a vortex is extinguished at much larger SDR than steady flame. It is also found that air-side vortex extinguishes a flame more rapidly than fuel-side vortex. The unsteady effect induced by flame-vortex interaction does not lead to a transient OH overshoot of the maximum steady concentration observed in experiment, while $HO_2$ radical increases more than the maximum steady concentration with increasing SDR. In addition, it is seen that NO and $NO_2$ are not sensitive to the unsteady variation of SDR.

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$C_2H_4$/Air 비예혼합 난류화염의 매연생성 모델링 (Numerical Modeling of Soot Formation in $C_2H_4$/Air Turbulent Non-premixed Flames)

  • 김태훈;우민호;김용모
    • 한국연소학회지
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    • 제15권4호
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    • pp.22-28
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    • 2010
  • The Direct Quadrature Method of Moments (DQMOM) has been presented for the solution of population balance equation in the wide range of the multi-phase flows. This method has the inherently interesting features which can be easily applied to the multi-inner variable equation. In addition, DQMOM is capable of easily coupling the gas phase with the discrete phases while it requires the relatively low computational cost. Soot inception, subsequent aggregation, surface growth and oxidation are described through a population balance model solved with the DQMOM for soot formation. This approach is also able to represent the evolution of the soot particle size distribution. The turbulence-chemistry interaction is represented by the laminar flamelet model together with the presumed PDF approach and the spherical harmonic P-1 approximation is adopted to account for the radiative heat transfer.

A Study of the Propagation of Turbulent Premixed Flame Using the Flame Surface Density Model in a Constant Volume Combustion Chamber

  • Lee, Sangsu;Kyungwon Yun;Nakwon Sung
    • Journal of Mechanical Science and Technology
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    • 제16권4호
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    • pp.564-571
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    • 2002
  • Three-dimensional numerical analysis of the turbulent premixed flame propagation in a constant volume combustion chamber is performed using the KIVA-3V code (Amsden et. al. 1997) by the flame surface density (FSD) model. A simple near-wall boundary condition is eaployed to describe the interaction between turbulent premixed flame and the wall. A mean stretch factor is introduced to include the stretch and curvature effects of turbulence. The results from the FSD model are compared with the experimental results of schlieren photos and pressure measurements. It is found that the burned mass rate and flame propagation by the FSD model are in reasonable agreement with the experimental results. The FSD combustion model proved to be effective for description of turbulent premixed flames.

수소화염과 상호작용하는 탄화수소화염의 연소특성 (Combustion Characteristics of a Hydrogen Flame Interacting with a Hydrocarbon Flame)

  • 오창보;이의주;최병일
    • 한국화재소방학회:학술대회논문집
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    • 한국화재소방학회 2008년도 추계학술논문발표회 논문집
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    • pp.17-20
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    • 2008
  • Numerical simulations were performed for the prediction of the flame structure of a hydrocarbon flame interacting with a hydrogen flame. Methane was used as a hydrocarbon fuel in this study. The interaction of two 1D premixed flames established in counterflow geometry was investigated. The temperature of the flame interacting with each other was much higher and the flame thickness was wider at a global strain of $1000\;s^{-1}$ than normal methane flame.

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Multi-environment PDF 모델을 이용한 MILD 연소과정 해석 (Multi-environment PDF Modeling for MILD Combustion Processes)

  • 지형근;전상태;김용모
    • 한국연소학회지
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    • 제22권4호
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    • pp.43-50
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    • 2017
  • In this study, the multi-environment probability density function(MEPDF) approach has been applied to numerically investigate Delft-Jet-in-Hot-Coflow(DJHC) turbulent flames under Moderate or Intense Low-oxygen Dilution (MILD) combustion condition. Computations are made for two different jet velocities(Re = 4100 and 8800). In terms of mean axial velocity, temperature, and turbulent kinetic energy, numerical results are in reasonably good agreements with experimental data even if there exist the noticeable deviations in downstream region. Based on numerical results, the detailed discussions are made for the essential features of the non-visible flame structure and MILD combustion processes.