• 한국연소학회:학술대회논문집
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• 한국연소학회 제26회 KOSCO SYMPOSIUM 논문집
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• pp.201-207
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• 2003

Characteristic of turbulent nonpremixed interacting flames are investigated experimentally 8 or 9 nozzles are arranged in the shape of matrix or circle. When there is no center nozzle, flame is more stable than with center nozzle case. It is shown that these blowout limit enlargements are related with the recirculation of burnt gases. The interacting flame base was not located at the stoichiometric point. NO concentrations of interacting flame are smaller than that of single flame using same area nozzle.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2010년도 제35회 추계학술대회논문집
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• pp.369-374
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• 2010

본 연구에서는 가스 연료와 공기 혼합물 내 압력파에 의해 유도되는 화염 가속과 연소폭발천이 현상을 수치적 계산을 통하여 살펴본다. 실험에 기반을 둔 초기 조건 하에서 점성력, 열전단, 몰질량 확산, 그리고 화학 반응을 고려한 reactive compressible Navier-Stokes 방정식을 사용하여 계산을 수행하였다. 반복되는 압력파와 화염의 상호 작용에 의해 발생되는 화염의 Richtmyer-Meshkov (RM) 불안정성에 의해 증가된 화염면을 통하여 생기는 hot spot들에 의한 폭굉의 발생을 모델링하였다. 또한 압력파의 강도 변화에 따른 연소폭발천이 현상의 변화를 살펴보았다.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2011년도 제36회 춘계학술대회논문집
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• pp.457-462
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• 2011

본 연구에서는 에틸렌-공기 혼합물에서의 충격파에 의해 유도되는 화염폭발천이현상을 수치적 계산을 통하여 살펴본다. 연구에 사용된 모델은 점성력, 열전단, 몰질량 확산, 그리고 화학 반응을 고려한 Navier-Stokes 방정식으로 관 내부 유동을 해석하였다. 반복되는 압력파와 화염의 상호 작용에 의해 발생되는 화염의 불안정성에 의해 화염면이 증가하게 되는데 이를 통해 화학 반응률의 증가와 더불어 연소열의 상승하게 된다. 이러한 과정들이 반복되면서 발생할 수 있는 연소폭발천이 현상을 벽면 온도 조건의 변화(단열조건과 일정한 온도 조건)에 따라 어떻게 변화 되는지를 모델링하였다.

• 대한기계학회논문집B
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• 제22권12호
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• pp.1669-1680
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• 1998

A method is developed to include the effect of volume expansion in the description of the flame dynamics using G-equation. Line volume-source is used to represent the effect of the exothermic process of combustion with source strength assigned by the density difference between the burned and the unburned region. The present model provides good agreement with the experimental results. Including volume expansion, the flow field is adjusted to accommodate the increased volume flow rate which crossing the flame front and the result predicts the same behavior of measured velocity field qualitatively. The effect of increasing volume expansion does not change the initial growth rate of flame area but increase the residence time. Consequently this effect increases the maximum area of flame front. The flame propagation in varying flow field due to volume expansion provides a promising way to represent the wrinkled turbulent premixed flames in a numerically efficient manner.

• 한국자동차공학회논문집
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• 제14권6호
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• pp.171-178
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• 2006

The performance in the practical combustion system including reciprocating engines and gas turbine combustors is being much governed by turbulent reacting flow that is often analyzed by both a laminar flamelets concept and flame interaction. The characteristics of laminar flame interaction have been investigated numerically to provide basic understanding of wrinkled turbulent flames under concentration interaction resulting from inhomogeneity in fuel-air mixing, especially focused on the transition of flame characteristics such as diffusion flame, partially premixed diffusion flame, and triple-layer flame by the variation in the degree of premixedness. The extinction stretch rates to the premixedness have also been obtained in this paper. The boundary defining the regime of the existence of triple-layer flames as functions of both stretch rate and premixedness has been determined which agrees well with previously reported experiment measuring OH radical concentration peaks based on PLIF.

• 대한기계학회논문집
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• 제11권6호
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• pp.991-1000
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• 1987

본 연구에서는 과농-희박 연료장에서 화염들의 상호작용에 관하여 이론적 해 석 및 실험적 검증을 통해 연구하였고, 이 중 특히 두 개의 예혼합화염 사이에 확산화 염이 형성되어 세 개의 화염이 존재하는 영역을 고찰하였다.

• 한국가시화정보학회:학술대회논문집
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• 한국가시화정보학회 2007년도 추계학술대회
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• pp.149-154
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• 2007

This study examines the effect of acoustic excitation using forced coaxial air on the flame characteristics of turbulent hydrogen nonpremixed flames. A resonance frequency was selected to acoustically excite the coaxial air jet due to its ability to effectively amplify the acoustic amplitude and reduce flame length and NOx emissions. Acoustic excitation causes the flame length to decrease by 15 % and consequently, a 25 % reduction in EINOx is achieved, compared to a flame without acoustic excitation. Moreover, acoustic excitation induces periodical fluctuation of the coaxial air velocity, thus resulting in slight fluctuation of the fuel velocity. From phase-lock PIV and OH PLIF measurement, the local flow properties at the flame surface were investigated under acoustic forcing. During flame-vortex interaction in the near field region, the entrainment velocity and the flame surface area increased locally near the vortex. This increase in flame surface area and entrainment velocity is believed to be a crucial factor in reducing flame length and NOx emission in coaxial jet flames with acoustic excitation. Local flame extinction occurred frequently when subjected to an excessive strain rate, indicating that intense mass transfer of fuel and air occurs radially inward at the flame surface.

• 대한기계학회논문집B
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• 제36권3호
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• pp.315-324
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• 2012

본 연구는 가연성 기체로서 에틸렌-공기 혼합물로 채워져 있는 관에서 장애물과 굽은 관에 의한 지형적 효과에 따라 변화하는 충격파와 화염의 상호 작용, 화염 가속, 연소폭발천이 현상을 수치적으로 살펴보았다. 여기서 사용되는 모델은 지배방정식으로 Navier-Stokes 방정식과 경계조건 처리 방법으로 ghost fluid 기법을 사용하였으며 지형적 영향을 달리한 여러 모델링을 통하여 화염과 강한 충격파의 충돌에 의한 열점 생성과 화염 전파의 지연 혹은 가속 현상을 확인하였다. 추가적으로 평균 화학적 에너지 발생률이 대략 20 MJ/($g{\bullet}s$)에서 폭굉으로 천이한다는 사실을 확인하였다. 그리고 동일 위치 열점 생성에도 불구하고 폭굉의 발생 시기가 반응물의 부재와 화염면 전방의 온도와 압력 차에 의해 지연될 수 있음을 확인하였다.

• 대한기계학회논문집B
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• 제29권1호
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• pp.71-79
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• 2005

For the non-premixed interacting jet flames, it has been reported that if eight small nozzles are arranged along the circle of $40{\sim}72$ times the diameter of single jet, the flames are not extinguished even in 200m/s. In this research, experiments were extended to the partially premixed cases to reduce both flame temperature and NOx emission. Nine nozzles were used- eight was evenly located along the perimeter of the imaginary circle and one at the geometric centre. The space between nozzles, S, the equivalence ratio, ${\phi}$, the exit velocity and the role of the jet from the centre nozzle were considered. Normally, flame was lifted and flame base was located inside the imaginary circle made by the nozzle. As nozzles went away from each other, blowout velocity increased and then decreased. The maximum blowout velocity diminished with the addition of air to the fuel stream. When the fuel and/or oxidizer were not fed through the centre nozzle, the maximum blowout velocity obtained by varying S and ${\phi}$ was around 160m/s. Optimum nozzle separation distance at which peak blowout velocity obtained also decreased with ${\phi}$ decrease. Flame base became leaner as approaching to the blowout. It seemed that lots of air was supplied to the flame stabilizing region by the entrainment and partially premixing. To approve this idea and to enhance the blowout velocity, fuel was supplied to the centre region. With the small amount of fuel through the centre nozzle, partially premixed flame could be sustained till sonic velocities. It seemed that the stabilizing mechanism in partially premixed interacting flame was different from that of non-premixed case because one was stabilized by the fuel supply through the centre nozzle but the other destabilized.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2004년도 추계학술대회
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• pp.1365-1370
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• 2004

It has been reported that if eight small nozzles are arranged along the circle of 40 $^{\sim}$ 72 times the diameter of single nozzle, the propane non-premixed flames are not extinguished even in 200m/s, In this research, experiments were extended to the methane flame. Nine nozzles were used- eight was evenly located along the perimeter of the imaginary circle and one at the geometric center. The space between nozzles, s, the exit velocity and the role of the jet from the center nozzle were considered. On the contrary to the propane non-premixed case, the maximum blowout velocity for the methane diffusion flame was achieved when small amount of fuel is supplied through the center nozzle and s/d equals around 21. In the laminar region, the flame attached at the center nozzle anchored the outer lifted flames.