• 한국연소학회:학술대회논문집
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• 대한연소학회 2003년도 제27회 KOSCO SYMPOSIUM 논문집
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• pp.159-165
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• 2003

This paper describes numerical efforts to characterize the flame-holding and air-fuel mixing process of model SCRamjet engine combustor, where a hydrogen jet injected into a supersonic cross flow and in a cavity. Combustion phenomena in a model SCRamjet engine, which has been experimentally studied at University of Queensland and Australian National University using a free-piston shock tunnel, was observed around separation region of upstream of the normal injector and inside of cavity. The results show that the separation region and cavity generates several recirculation zones, which increase the fuel-air mixing. Self ignition occurs in the separation-freestream and cavity-freestream interface.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2007년도 제28회 춘계학술대회논문집
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• pp.295-298
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• 2007

본 연구에서는 초음속 공동유동장에서 발생하는 압력변동을 저감하기 위한 피동제어방법의 유용성을 실험 및 수치해석적으로 조사하였다. 피동제어방법으로 사각 공동내 상류 벽면에 sub-cavity를 설치하였다. 공동내 하류벽면에 센서를 설치하여 압력변동 값을 실험적으로 측정하였으며, 측정된 압력변동값을 FFT변환하여 주파수 분석을 하였다. 수치계적으로는 공동내 압력변동 특성을 살펴보기 위해 3차원 비정상 Navier-Stokes 방정식에 유한체적법을 적용하여 유동장을 모사하였으며, 유동의 난류상태량들은 LES 방법을 사용하여 계산하였다. 본 연구에서 얻어진 결과는 다음과 같다. 공동유동에서 진동 특성은 공동 하류벽면에서 발생하는 압력진동에 의존한다. 특히 leading tip 두께와 sub-cavity 크기가 진동 저감효과에 주요 인자이다.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2002년도 학술대회지
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• pp.755-758
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• 2002

The physical phenomena of rectangular open cavity are numerically investigated in this paper Two-dimensional cavity problems with laminar boundary layers in upstream are simulated by using the compressible Wavier-Stokes equations. The high-order and high-resolution numerical schemes are used for the evaluation of spatial derivatives and the time integration. Cross-correlation is used to analyze the characteristics of wave propagation along time and spatial. Sudden phase shifting of 90 degrees is appeared near downstream edge, and this is coincident with the phase lag suggested in original Rossiter's equation. The results give a further understanding of the physical phenomenon of noise generation, and the resonance of flow and acoustic in cavity. Moreover, modified Rossiter's equation, which is more accurate and can be applied in various conditions, is suggested. The distance from the point of vortex generation to the point of vortex collapsing acts as effective distance of cavity resonance, and the phase difference between the point of vortex collapsing and the point of acoustic source acts as phase lag. The mechanism of acoustic generation is fully understood in this paper. The mechanism of acoustic generation is fully understood in this paper.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2006년도 제27회 추계학술대회논문집
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• pp.363-366
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• 2006

본 연구에서는 초음속 공동유동장에서 발생하는 압력 진동을 완화시키기 위하여 사용된 두 가지 피동제어방법들의 유효성을 수치해석적으로 조사하였다. 사용된 제어 장치들은 삼각돌기와 sub-cavity로, 전단층의 발달 특성을 조절하기 위하여 공동 전단 부근에 설치된다. 공동유동의 압력변동 특성을 조사하기 위하여 3차원 비정상 Navier-Stokes 방정식에 유한체적법을 적용하여 유동장을 모사하였으며, 유동의 난류상태량들은 LES 방법을 사용하여 계산하였다. 그 결과, 공동유동의 진동 특성은 공동의 후단 벽면에서 발생하는 압력 진동에 의해 지배되며, 제시된 방법들의 효과는 공동의 후단에서 가장 크게 나타났다. 특히, sub-cavity는 삼각돌기나 블로잉이 있는 경우에 비하여 압력 진동 저감효과가 상대적으로 크며, sub-cavity가 큰 경우 압력 진동의 저감효과가 더욱 뚜렷하게 나타났다.

• 한국추진공학회지
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• 제8권1호
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• pp.61-69
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• 2004

본 연구는 극초음속 모델 스크램제트 엔진 연소기의 화염지지와 연료-공기 혼합과정의 특성을 살펴보기 위하여 수치해석을 이용하여 수행되었다. 연료분사 방법으로 수소연료가 초음속 유동장에 수직분사되는 경우와 공동내부에 분사되는 두 가지 경우를 채택하였으며 각각 UQ(University of Queensland, Australia)와 ANU(Australian National University, Australia)의 충격파 풍동을 이용하여 실험이 수행되었다. 수치해석을 통하여 수직분사 상류의 박리영역과 공동주변에서 연소현상이 관찰되었다. 수직분사의 박리영역과 공동내부분사의 공동은 재순환 영역을 발생시키며, 이 재순환 영역은 연료-공기의 혼합을 촉진시킨다. 또한 자발점화가 박리영역-자유류, 공동-자유류 경계면에서 발생함을 알 수 있었다.

• 유체기계공업학회:학술대회논문집
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• 유체기계공업학회 2005년도 연구개발 발표회 논문집
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• pp.311-317
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• 2005

Measurements of the leakage flow in the shrouded cavity were performed in axial compressor cascades at $Re=2.6{\times}10^5$. This paper describes the effects of the leakage flow tangential velocity on kinematics of the leakage flow in the shrouded cavity and consequent overall loss and exit flow turning at stator blade row downstream. Flow data and flow visualization images consistently indicate that leakage flow circumferentially migrates 2, 4 and 5 blade passages in the direction of rotation for ${\upsilon}_y/c=0.09$, 0.35 and 0.45, respectively where ${\upsilon}_y$ is the leakage tangential velocity and c is the mainstream velocity. The leakage flow contracts to a jet across the seal-tooth resulting in an increase in the leakage axial velocity-doubling the leakage axial velocity in upstream cavity compared to that in the downstream cavity. Consequently, two flow regions are distinguished before and after the seal-tooth. As increasing the leakage tangential velocity, the overall loss downstream of stator blade row decreases and the exit flow turning in the range of span. from the hub endwall to 15% increases while the decreases in the flow turning from 15% to 30% span is observed.

• 한국항공우주학회지
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• 제30권5호
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• pp.101-108
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• 2002

본 연구는 비압축성 열린 공동 유동에 대한 수치적 모사이다. 2차원 Navier-Stokes 방적식을 제어체적에 대해 엇갈림 격자계를 이용하여 공간에 대해서는 C-QUICK을 시간에 대해서는 내재적 기법을 이용하여 적분하였다. 압력장은 SIMPLE-C 알고리즘에 의하여 계산 되었다. 정상 모드에서는 나타나지 않지만 전단층 모드의 경우에 나타나는 세 번째 소용돌이가 공동 유동의 안정성에 중요한 역할을 하는 것을 알 수 있었다. 이를 바탕으로 공동 앞전 아래 벽면에 Jet blowing을 정상 상태와 비정상 상태로 가하여 그 영향을 알아보았다. 주기적인 blowing 인 경우 가진 주기와 위상차 그리고 속도 크기가 중요한 변수이며 이 변수들에 의한 영향을 연구하였다.

• 한국추진공학회:학술대회논문집
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• 한국추진공학회 2004년도 제22회 춘계학술대회논문집
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• pp.42-47
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• 2004

Air-fuel mixing and flame-holding are two important factors that have to be considered in the design of an injection system. Different injection strategies have been proposed with particular concern for rapid air-fuel mixing and flame-holding. Two representative injection techniques can be applied in a supersonic combustor. One of the simplest approaches is a transverse(normal) injection. The cavity flame holder, an integrated fuel injection/flame-holding approach, has been proposed as a new concept for flame holding and air-fuel mixing in a supersonic combustor. This paper describes numerical efforts to characterize the flame-holding and air-fuel mixing process of a model scramjet engine combustor, where hydrogen is injected into a supersonic cross flow and a cavity. The combustion phenomena in a model scramjet engine, which has been experimentally studied at University of Queensland and Australian National University using a free-piston shock tunnel, were observed around the separation region of the transverse injector upstream and the inside cavity. The results show that this flow separation generates recirculation regions which increase air-fuel mixing. Self-ignition occurs in the separation-freestream and cavity-fteestream interfaces.

• 한국전산유체공학회:학술대회논문집
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• 한국전산유체공학회 2006년도 PARALLEL CFD 2006
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• pp.311-314
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• 2006

The supersonic flow around tandem cavities was investigated by three- dimensional numerical simulations using the Reynolds-Averaged Navier-Stokes(RANS) equation with the $\kappa-\omega$ thrbulence model. The flow around a cavity is characterized as unsteady flow because of the formation and dissipation of vortices due to the interaction between the freestream shear layer and cavity internal flow, the generation of shock and expansion waves, and the acoustic effect transmitted from wake flow to upstream. The upwind TVD scheme based on the flux vector split using van Leer's limiter was used as the numerical method. Numerical calculations were performed by the parallel processing with time discretizations carried out by the 4th-order Runge-Kutta method. The aspect ratio of cavities are 3 for the first cavity and 1 for the second cavity. The ratio of cavity interval to depth is 1. The ratio of cavity width to depth is 1 in the case of three dimensional flow. The Mach number and the Reynolds number were 1.5 and $4.5{\times}10^5$, respectively. The characteristics of the dominant frequency between two-dimensional and three-dimensional flows were compared, and the characteristics of the second cavity flow due to the fire cavity flow cavity flow was analyzed. Both two dimensional and three dimensional flow oscillations were in the 'shear layer mode', which is based on the feedback mechanism of Rossiter's formula. However, three dimensional flow was much less turbulent than two dimensional flow, depending on whether it could inflow and outflow laterally. The dominant frequencies of the two dimensional flow and three dimensional flows coincided with Rossiter's 2nd mode frequency. The another dominant frequency of the three dimensional flow corresponded to Rossiter's 1st mode frequency.

• Journal of Mechanical Science and Technology
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• 제20권8호
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• pp.1256-1265
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• 2006

The supersonic flows around tandem cavities were investigated by two-dimensional and three-dimensional numerical simulations using the Reynolds-Averaged Navier-Stokes (RANS) equation with the k- ω turbulence model. The flow around a cavity is characterized as unsteady flow because of the formation and dissipation of vortices due to the interaction between the freestream shear layer and cavity internal flow, the generation of shock and expansion waves, and the acoustic effect transmitted from wake flow to upstream. The upwind TVD scheme based on the flux vector split with van Leer's limiter was used as the numerical method. Numerical calculations were performed by the parallel processing with time discretizations carried out by the 4th-order Runge- Kutta method. The aspect ratios of cavities are 3 for the first cavity and 1 for the second cavity. The ratio of cavity interval to depth is 1. The ratio of cavity width to depth is 1 in the case of three dimensional flow. The Mach number and the Reynolds number were 1.5 and $4.5{\times}10^5$, respectively. The characteristics of the dominant frequency between two- dimensional and three-dimensional flows were compared, and the characteristics of the second cavity flow due to the first cavity flow was analyzed. Both two dimensional and three dimensional flow oscillations were in the 'shear layer mode', which is based on the feedback mechanism of Rossiter's formula. However, three dimensional flow was much less turbulent than two dimensional flow, depending on whether it could inflow and outflow laterally. The dominant frequencies of the two dimensional flow and three dimensional flows coincided with Rossiter's 2nd mode frequency. The another dominant frequency of the three dimensional flow corresponded to Rossiter's 1st mode frequency.