• 한국화재소방학회논문지
• /
• 제33권5호
• /
• pp.48-54
• /
• 2019

본 연구에서는 Eddy Dissipation Concept (EDC) 1-step 연소모델을 이용하여 백드래프트에 대한 대와동모사를 성공적으로 수행하였다. 기존 연구와는 달리 EDC 1-step의 유한화학반응에서 활성화에너지를 적절히 조절함으로써 백드래프트에 대한 예측이 가능하였다. EDC 1-step 연소모델을 이용한 예측결과는 Mixing-Controlled Fast Chemistry(MCFC) 연소모델의 예측결과와 비교 검토되었다. 얻어진 결과에서는 백드래프트 발생 시점을 제외하면 EDC 1-step과 MCFC 결과들은 매우 유사한 것을 확인하였고, 실험에서 얻어진 최고 압력값에 대해서도 합리적인 수준에서 예측하는 것은 알 수 있었다. 그러나 EDC 1-step 연소모델도 MCFC와 마찬가지로 백드래프트 전개과정의 첫 번째 압력 피크에 대해서는 예측하지 못하는 한계를 확인할 수 있었다.

• Wind and Structures
• /
• 제5권2_3_4호
• /
• pp.369-378
• /
• 2002

The application of Large Eddy Simulation (LES) in a curvilinear coordinate system to the flow around a square cylinder is presented. In order to obtain sufficient resolution near the side of the cylinder, we use an O-type grid. Even with a curvilinear coordinate system, it is difficult to avoid the numerical oscillation arising in high-Reynolds-number flows past a bluff body, without using an extremely fine grid used. An upwind scheme has the effect of removing the numerical oscillations, but, it is accompanied by numerical dissipation that is a kind of an additional sub-grid scale effect. Firstly, we investigate the effect of numerical dissipation on the computational results in a case where turbulent dissipation is removed in order to clarify the differences between the effect of numerical dissipation. Next, the applicability and the limitations of the present method, which combine the dynamic SGS model with acceptable numerical dissipation, are discussed.

• 한국추진공학회:학술대회논문집
• /
• 한국추진공학회 2005년도 제25회 추계학술대회논문집
• /
• pp.450-454
• /
• 2005

축대칭 동축형 램제트 연소기에 대한 반응 유동장 해석을 수행하였다. 2차원 축대칭 Wavier-Stokes 방정식과 낮은 레이놀즈 수 $k-\varepsilon$ 난류 모델을 이용하였고, 유한반응률 화학반응 모델을 적용하였다. 난류 연소 모델인 EDM (Eddy-Dissipation Model)과 층류 반응 모델을 적용한 경우를 서로 비교하였다. 급확대 연소기와 wedge형 보염기를 장착한 동축형 램제트 연소기에 대한 반응 유동장 수치해석을 통해 두 가지 결과를 화염안정 측면에서 서로 비교하였다.

• 대한기계학회논문집B
• /
• 제22권5호
• /
• pp.685-697
• /
• 1998

Series of recent k-.epsilon. model modification have been carried out with the aid of DNS data to include the effect of near wall. Though these methods opened new way of turbulence modelings, newly developed turbulence models of its kind had yet shortcomings in prediction for the turbulent flows with various Reynolds numbers and various geometric conditions. As a remedy for these shortcomings, a new k-.epsilon. model proposed here by improving the dissipation rate equation and the damping function for eddy viscosity model. The new dissipation rate equation was modeled based on the energy spectrum and magnitude analysis. The damping function for eddy viscosity was also formulated on the ground of distribution of dissipation rate length scales near a wall and the DNS data. The new k-.epsilon. model was applied to the fully developed turbulent flows in a channel and a pipe with a wide range of Reynolds numbers. Prediction results showed that the present model represents properly the turbulence properties in all turbulent regions over a wide range of Reynolds numbers.

• Journal of Mechanical Science and Technology
• /
• 제19권3호
• /
• pp.913-923
• /
• 2005

The dynamic mixed model (DMM) combined with a box filter of Zang et. al. (1993) has been generalized for passive scalar transport and applied to large eddy simulation of turbulent channel flows with Prandtl number up to 10. Results from a priori test showed that DMM is capable of predicting both subgrid-scale (SGS) scalar flux and dissipation rather accurately for the Prandtl numbers considered. This would suggest that the favorable feature of DMM, originally developed for the velocity field, works equally well for scalar transport problem. The validity of the DMM has also been tested a posteriori. The results of the large eddy simulation showed that DMM is superior to the dynamic Smagorinsky model in the prediction of scalar field and the model performance of DMM depends to a lesser degree on the ratio of test to grid filter widths, unlike in the a priori test.

• 한국화재소방학회논문지
• /
• 제31권4호
• /
• pp.35-42
• /
• 2017

구획실 내부의 고온 메탄연료에서 발생하는 백드래프트 현상에 대해 FDS v6를 이용한 LES를 수행하였다. EDC 연소모델을 적용하였고 여기 필요한 화학반응기구에 대해서는 5가지를 검토하여 백드래프트에 대한 예측성능을 검토하였다. 구획실 내, 외부의 온도, 연료, 속도 및 압력분포에 대한 수치계산 결과고찰과 실험에서 얻어진 압력변화와의 비교를 수행하였다. FDS v6에서 기본적으로 제공하는 EDC 연소모델을 적용하면 LES 기법을 이용하여 백드래프트에 대한 수치계산이 가능함을 확인하였다. 그러나, 결합되는 화학반응기구에 따라서 백드래프트에 대한 예측성능이 큰 차이를 보였다. FDS에서 EDC 연소모델을 적용하여 백드래프트에 대한 LES를 수행할 경우에는 연료특성에 맞는 화학반응기구의 적합성을 우선 검토하는 것이 필요함을 확인하였다.

• 한국해양공학회:학술대회논문집
• /
• 한국해양공학회 2000년도 춘계학술대회 논문집
• /
• pp.75-80
• /
• 2000

We revisit the arrested Ekman boundary layer problem, using a fully non-linear numerical model with the subgrid dissipation modeled by the large eddy simulation method (LES). The main objective of this study is to find out whether the dynamic balance of the arrested Ekman boundary layer explained by MacCready and Rhines (1991) is valid for high Reynolds number. The model solution indicates that for high Reynolds number and low Richardson number flows, the density anomaly diffusion by near-wall turbulent action may become intense enough to homogenize completely the density structure within the boundary layer, in the direction perpendicular to the sloping wall. Then the buoyancy effect becomes negligible allowing a near-equilibrium Ekman boundary layer flow to persist for a long period.

• 항공우주시스템공학회지
• /
• 제13권5호
• /
• pp.39-48
• /
• 2019

회전-고정자 혼합기 내의 난류 유동은 고속으로 회전하는 회전자와 고정자의 상호작용에 의해 발생되는 전단특성을 기반으로 한다. 본 연구에서는 유화연료 관련 회전-고정자 혼합기 시제품 모델에서 회전자와 고정자간의 상호작용에 의한 비정상상태 유동 특성 분석을 ANSYS FLUENT $k-{\varepsilon}$ (RKE) 난류 모델을 MRF 및 SMM에 적용하여 수행하였다. 회전자와 고정자의 경계에서 발생하는 유동 입자들의 거동과 전단 특성 그리고 설계 파라미터에 따른 속도분포와 난류와류소산 등의 경향을 전산유체역학 해석을 통해 예측 비교하여 모델의 효율성을 검증하였다.

• 대한기계학회논문집B
• /
• 제33권12호
• /
• pp.1014-1021
• /
• 2009

A new eddy viscosity equation was formulated from assumption of turbulence length scale equation and specific dissipation ratio equation. Then, a set of turbulence model equations for the turbulent kinetic energy ${\kappa}$, the viscosity ${\nu}_t$, and the intermittency factor ${\gamma}$ is proposed by considering the entrainment effect. Closure coefficients are determined by experimental data and resorting to numerical optimization. Present model has been applied to compute four representative cases of free shear flows and successfully compared with experimental data. In particular, the spreading rate, the centreline mean velocity and the profiles of intermittency are calculated with improved accuracy. Also, the proposed ${\nu}_t-{\kappa}-{\gamma}$ model was applied to channel flow by considering the wall effect and the results show good agreements with the Direct Numerical Simulation data.

• 한국수자원학회논문집
• /
• 제44권6호
• /
• pp.461-470
• /
• 2011

Abrupt and gradual levee breach analyses on the flat domain were implemented by laboratory experiments and numerical simulations. To avoid the reflective wave from the side wall the experiment was performed in a large domain surrounded by waterway. A numerical model was developed for solving the two-dimensional gradual levee breach flow. The results of the numerical simulation developed in this study showed good agreement with those of the experimental data. However, even if the numerical schemes effectively replicated the trends of the observed water depth for the first shock, there were little differences for the second shock. In addition, even though the model considered the Smagorinsky horizontal eddy viscosity, the location and height of the hydraulic jump in the numerical simulation were not fairly well agree with experimental measurements. This shows the shallow water equation solver has a limitation which does not exactly reproduce the energy dissipation from the hydraulic jump. Further study might be required, considering the energy dissipation due to the hydraulic jump or transition flow from reflective wave.