• 제목/요약/키워드: unsteady-state simulation

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Eulerian-Lagrangian 다상 유동해석법에 의한 피에조 인젝터의 노즐 내부 비정상 캐비테이션 유동해석 (Analysis of Unsteady Cavitating Flows in Fuel Injection Nozzle of Piezo-driven Injector by Eulerian-Lagrangian Multi-phase Method)

  • 이진욱;민경덕;강건용
    • 한국분무공학회지
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    • 제9권4호
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    • pp.38-45
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    • 2004
  • This study describes the analysis results of unsteady cavitating flows behavior inside nozzle of the prototype piezo-driven injector. This piezo-driven injector has been recognised as one of the next generation diesel injector due to a higher driven efficiency than the conventional solenoid-driven injector. The three dimensional geometry model along the central cross-section regarding of one injection hole has been used to simulate the cavitating flows for injection time by at fully transient simulation with cavitation model. The cavitation model incorporates many of the fundamental physical processes assumed to take place in cavitating flows. The simulations performed were both fully transient and 'pseudo' steady state, even if under steady state boundary conditions. We could analyze the effect the pressure drop to the sudden acceleration of fuel, which is due to the fastest response of needle, on the degree of cavitation existed in piezo-driven injector nozzle

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익산 지역의 지하수 유동 모델 (Groundwater Flow Model of Igsan Area)

  • 함세영;김연기
    • 자원환경지질
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    • 제22권4호
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    • pp.381-393
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    • 1989
  • 익산지역의 지하수 유동계를 평가하기 위한 수리지질학적 모델링이 수행되었다. 연구지역의 범위는 $790km^2$이다. 본 지역의 지질은 쥬라기의 대보화강암과 편마상화강암 그리고 선캠브리아기의 변성암으로 구성되어 있다. 채수량은 편마상화강암지역에서 가장 높으며 이는 10km내지 25m두께의 비교적 두껍게 발달된 풍화대 때문이다. 본 모델 시뮬레이션에는 콜로라도 주립대학의 유한차분법모델이 사용되었다. 본 모델은 불균일한 격자간격을 가지며, 28행과 31열로 이루어져 있다. 본 모델은 정류상태와 부정류상태에서 보정되었다.. 정류상태 시뮬레이션의 결과를1985년 9월의 수위등고선과 비교하여 투수율과 우기의 순충전률을 결정하였다. 부정류상태 시뮬레이션은 지하수 채수에 따른 대수층의 반응을 알기 위한 것이다. 부정류상태를 보정에서는 1986년5월의 수위등고선과 맞춤으로서 비산출율의 크기와 분포 그리고 건기의 채수량과 충전량을 결정하였다. 보정된 모델을 이용하여 1985년 10월부터 1995년 9월까지의 지하수채수 및 자연적인 충전에 의한 지하수위변동을 예측하여 보았다. 보정된 모델은 광역적인 지하수개발계획에 이용될 수 있다. 그러나 국부적인 지하수위변동을 예측하는데는 이용될 수 없다.

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Quasi-steady State Simulation of Rotating Detonation Engine

  • Niyasdeen, Mohammed;Oh, Sejong;Kim, Kui Soon;Choi, Jeong-Yeol
    • International Journal of Aeronautical and Space Sciences
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    • 제16권4호
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    • pp.548-559
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    • 2015
  • We performed a numerical simulation based on the two-dimensional (2-D) unsteady Euler's equation with a single-step Arrhenius reaction model in order to investigate the detonation wave front propagation of an Argon (Ar) diluted oxy-hydrogen mixture ($2H_2+O_2+12Ar$). This simulation operates in the detonation frame of reference. We examine the effect of grid size and the performance impact of integrated quantities such as mass flow. For a given set of baseline conditions, the minimal and maximum grid resolutions required to simulate the respective detonation waves and the detonation cell structures are determined. Tertiary shock wave behavior for various grids and pre-exponential factors are analyzed. We found that particle fluctuation can be weakened by controlling the mass flow going through the oblique shock waves.

초고온가스로의 RCCS 해석을 위한 축대칭 모사 방법론 평가 (EVALUATION OF METHODOLOGY FOR AXISYMMETRIC SIMULATION OF RCCS IN VHTR)

  • 김성훈;조봉현;탁남일;김민환
    • 한국전산유체공학회지
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    • 제15권1호
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    • pp.1-8
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    • 2010
  • RCCS is a passive safety-related system that removes the decay heat of VHTR when normal decay heat removal systems are in failure. Understanding thermo-hydraulics of RCCS is important to design a safer VHTR. RCCS consists of 292 cooling panels, which are placed in the reactor cavity. The layout of RCCS gives an idea that, for CFD simulations, cooling panels can be assumed to be one annulus tube. This assumption can reduce significantly the computational time, especially for the unsteady simulation. To simulate RCCS in an axisymmetric manner, three models were suggested and compared. Each model has (1) the same outer radius, (2) the same cross-sectional area (3) the same pressure drop, respectively, as the RCCS cooling panels. The steady-state simulation was conducted with these three models and the DO radiation model. It is found that over 90% of the heat from the outer wall of the reactor pressure vessel is transported to the RCCS by radiative heat transfer. The simulation with the third model, which has the same pressure drop as the design, estimates the closest wall temperature profiles to a thermo-hydraulic code, GAMMA+, result.

대규모와 모사에 의한 3차원 소형축류홴의 운전부하에 따른 난류유동장 구조에 대한 연구 (A Study on the Structure of Turbulent Flow Fields According to the Operating Loads of Three-Dimensional Small-Size Axial Fan by Large Eddy Simulation)

  • 김장권;오석형
    • 동력기계공학회지
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    • 제19권5호
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    • pp.80-85
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    • 2015
  • The unsteady-state, incompressible and three-dimensional large eddy simulation(LES) was carried out to analyze the structure of turbulent flow fields according to the operating loads of three-dimensional small-size axial fan(SSAF). LES shows the best prediction performance in comparison with any other Reynolds averaged Navier-Stokes(RANS) method because static pressure coefficients analysed by LES show a little bit larger than measurements including all flow coefficients. Also, it can be known that the wake of SSAF is divided into from axial flow to radial flow before and behind stall region according to the increase of static pressure through LES analysis.

운전점에 따른 3차원 소형축류홴의 와도 특성에 대한 대규모 와 모사 (Large Eddy Simulation on the Vorticity Characteristics of Three-Dimensional Small-Size Axial Fan with Different Operating Points)

  • 김장권;오석형
    • 동력기계공학회지
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    • 제20권6호
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    • pp.64-70
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    • 2016
  • The unsteady-state, incompressible and three-dimensional large-eddy simulation(LES) was carried out to evaluate the vorticity distribution of a small-size axial fan(SSAF). The X-component vorticity profiles developed around blade tips turn from axial to radial, and diminish the density of distribution according to the increase of static pressure. Otherwise, the Z-component vorticity profiles evenly develop at the region larger than the half radial distance of blade at the operating points of A and B, partly at the trailing-edge region of blade and radially over bellmouth according to the increase of static pressure.

운전부하에 따른 3차원 소형축류홴 날개표면에 작용하는 정압과 항력에 대한 대규모와 모사 (Large Eddy Simulation on the Drag and Static Pressure Acting on the Blade Surface of Three-Dimensional Small-Size Axial Fan with Different Operating Loads)

  • 김장권;오석형
    • 동력기계공학회지
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    • 제21권2호
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    • pp.57-63
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    • 2017
  • The large-eddy simulation(LES) was carried out to evaluate the drag and static pressure acting on the blade surface of a small-size axial fan(SSAF) under the condition of unsteady-state, incompressible fluid and three-dimensional coordination. The axial component of drag coefficient increases with the increase of operating load, but the radial components have negligible sizes regardless of operating loads. Otherwise, the static pressures acting on the blade surfaces of SSAF show different distributions around the operating point of D equivalent to the stall. Also, with the increase of operating load, the static pressures acting on the pressure and suction surfaces of blade concentrate at the tips and leading-edges as a whole.

AA5083-H18 판재의 마찰 교반 점 용접 공정에 대한 전산 해석 (Numerical Simulation of friction Stir Spot Welding Process with AA5083-H18)

  • 김돈건;;유일;김지훈;김종민;;;정관수
    • 한국소성가공학회:학술대회논문집
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    • 한국소성가공학회 2009년도 춘계학술대회 논문집
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    • pp.458-461
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    • 2009
  • Thermo-mechanical simulation of the Friction Stir Spot Welding (FSSW) processes was performed for the AA5083-H18 sheets, utilizing commercial Finite Element Method (FEM) and Finite Volume Method (FVM) which are based on Lagrangian and Eulerian formulations, respectively. The Lagrangian explicit dynamic FEM code, PAM-CRASH, and the Eulerian Computational Fluid Dynamics (CFD) FVM code, STAR-CD, were utilized to understand the effect of pin geometry on weld strength and material flow under the unsteady state condition. Using FVM code, material flow pattern near the tool boundary was analyzed to explain the weld strength difference between the weld by cylindrical pin and the weld by triangular pin, while the frictional energy concept using the FEM code had limitation to explain the weld strength difference.

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연속 회분식 반응조에서 생물학적 영양염류 제거에 대한 모델링 및 동적 시뮬레이션(I) (Modeling and Dynamic Simulation for Biological Nutrient Removal in a Sequencing Batch Reactor(I))

  • 김동한;정태학
    • 상하수도학회지
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    • 제13권3호
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    • pp.42-55
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    • 1999
  • A mathematical model for biological nutrient removal in a sequencing batch reactor process, which is based on the IAWQ Activated Sludge Model No. 2 with a few modifications, has been developed. Twenty water quality components and twenty three kinetic equations are incorporated in the model. The model is structured in the matrix form based on the law of mass conservation using stoichiometry and kinetic equations. Stoichiometric coefficients and kinetic parameters included in the model equations are chosen from the literature. A multistep predictor-corrector algorithm of variable step-size is adopted for solving the vector nonlinear ordinary differential equations. The simulation for experimental results is conducted to evaluate the validity of the model and to calibrate coefficients and parameters. The simulation using the model well represents the experimental results from laboratory. The mathematical model developed in this study may be utilized for the design and operation of a sequencing batch reactor process under the steady and unsteady-state at various environmental conditions.

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Numerical studies on non-shear and shear flows past a 5:1 rectangular cylinder

  • Zhou, Qiang;Cao, Shuyang;Zhou, Zhiyong
    • Wind and Structures
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    • 제17권4호
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    • pp.379-397
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    • 2013
  • Large Eddy Simulations (LES) were carried out to investigate the aerodynamic characteristics of a rectangular cylinder with side ratio B/D=5 at Reynolds number Re=22,000 (based on cylinder thickness). Particular attention was devoted to the effects of velocity shear in the oncoming flow. Time-averaged and unsteady flow patterns around the cylinder were studied to enhance understanding of the effects of velocity shear. The simulation results showed that the Strouhal number has no significant variation with oncoming velocity shear, while the peak fluctuation frequency of the drag coefficient becomes identical to that of the lift coefficient with increase in velocity shear. The intermittently-reattached flow that features the aerodynamics of the 5:1 rectangular cylinder in non-shear flow becomes more stably reattached on the high-velocity side, and more stably separated on the low-velocity side. Both the mean and fluctuating drag coefficients increase slightly with increase in velocity shear. The mean and fluctuating lift and moment coefficients increase almost linearly with velocity shear. Lift force acts from the high-velocity side to the low-velocity side, which is similar to that of a circular cylinder but opposite to that of a square cylinder under the same oncoming shear flow.