• 제목/요약/키워드: Unsteady Wake Flow

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고 레이놀즈 수에서 분리된 분할판을 가진 원주의 유동장 특성 (Characteristics of Flowfield of a Circular Cylinder Having a Detached Splitter Plate with High Reynolds Number)

  • 노기덕;이한균;이종호;이정민;신진호;천강빈
    • 대한기계학회논문집B
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    • 제40권6호
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    • pp.373-381
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    • 2016
  • 본 연구는 고 레이놀즈 영역에서 후류측에 분리된 분할판(Detached splitter plate)을 가진 원주의 유동장 특성을 양 항력측정 실험과 PIV를 이용한 가시화 실험으로 파악한 것이다. 실험파라메터는 원주 한변의 길이에 대한 분할판의 폭비(H/B=0.5~1.5) 및 원주 후면에서부터 분할판의 앞전까지의 거리(G/B=0~2)로 했다. 분할판의 폭비를 고정시킨 경우 원주의 항력감소율은 간격비가 증가할수록 증가한 후 감소하는 특성을 보였다. 또한 같은 간격비에서는 분할판의 폭비가 클수록 원주의 항력감소율이 컸다. 분리된 분할판의 설치에 의해 분할판의 상, 하부에는 서로 반대방향의 볼테스가 발생되었고, 이 볼텍스가 원주 후류측에 역류를 발생시켜, 원주에 작용하는 항력을 감소시켰다.

플랫폼의 주기 운동을 고려한 부유식 해상 풍력터빈의 공력 성능 해석 (Aerodynamic Load Analysis of a Floating Offshore Wind Turbine Considering Platform Periodic Motion)

  • 김영진;유동옥;권오준
    • 한국항공우주학회지
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    • 제46권5호
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    • pp.368-375
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    • 2018
  • 본 연구에서는 부유식 플랫폼의 6자유도 방향으로의 주기 운동이 로터 공력 성능에 미치는 영향을 확인하기 위해 부유식 해상 풍력터빈에 대한 공력 해석이 수행되었다. 수치 해석을 위해 블레이드 요소 운동량 방법을 이용하였으며, 유동 박리와 후류 영향에 의한 비정상 공력 효과를 포착하기 위해 인디셜 응답 방법에 기반한 동적 실속 모델을 이용하였다. 로터에 의해 유도되는 내리 흐름은 운동량 이론과 난류 후류 상태에 대한 경험적 모델을 연계하여 계산하였다. heave, sway, surge 방향으로의 병진 운동과 roll, pitch, yaw 방향으로의 회전 운동을 포함한 플랫폼 주기 운동을 고려하였으며, 각각의 모션은 사인함수 형태로 적용되었다. 수치해석을 위한 대상 풍력터빈으로는 NREL 5MW 풍력터빈이 사용되었다. 해석 결과로부터 세 방향 병진 운동 모드 중, surge 운동 시 로터 공력 변화가 상대적으로 크게 나타났으며, 회전 운동 모드의 경우, pitch 운동에 의해 로터 공력이 크게 변화됨을 확인할 수 있었다.

RANS simulation of cavitation and hull pressure fluctuation for marine propeller operating behind-hull condition

  • Paik, Kwang-Jun;Park, Hyung-Gil;Seo, Jongsoo
    • International Journal of Naval Architecture and Ocean Engineering
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    • 제5권4호
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    • pp.502-512
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    • 2013
  • Simulations of cavitation flow and hull pressure fluctuation for a marine propeller operating behind a hull using the unsteady Reynolds-Averaged Navier-Stokes equations (RANS) are presented. A full hull body submerged under the free surface is modeled in the computational domain to simulate directly the wake field of the ship at the propeller plane. Simulations are performed in design and ballast draught conditions to study the effect of cavitation number. And two propellers with slightly different geometry are simulated to validate the detectability of the numerical simulation. All simulations are performed using a commercial CFD software FLUENT. Cavitation patterns of the simulations show good agreement with the experimental results carried out in Samsung CAvitation Tunnel (SCAT). The simulation results for the hull pressure fluctuation induced by a propeller are also compared with the experimental results showing good agreement in the tendency and amplitude, especially, for the first blade frequency.

CFD를 이용한 부분흡입형 터빈 공력형상 설계 (Aerodynamic Shape Design of a Partial Admission Turbine Using CFD)

  • 이은석
    • 대한기계학회논문집B
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    • 제30권11호
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    • pp.1131-1138
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    • 2006
  • Aerodynamic shape design of a partial admission turbine using CFD has been performed. Two step approaches are adopted in this study. Firstly, two-dimensional blade shape is optimized using CFD and genetic algorithm. Initially, the turbine cascade shape is represented by four design parameters. By controlling the design parameters as variables, the non-gradient search is analyzed for obtaining the maximum efficiency. The final two-dimensional blade proved to have a more blade power than the initial blade. Secondly, the three-dimensional CFD analysis including the nozzle, rotor and stator has been conducted. To avoid a heavy computational load due to an unsteady calculation, the frozen rotor method is implemented in steady calculation. The frozen rotor method can detect a variation of the flow-field dependent upon the blade's circumferential position relative to the nozzle. It gives a better idea of wake loss mechanism starting from the lip of the nozzle than the mixing plane concept. Finally, the combination of two and three dimensional design method of the partial admission turbine in this study has proven to be a robust tool in development phase.

Computation of Turbulent Flows and Radiated Sound From Axial Compressor Cascade

  • Lee, Seungbae;Kim, Hooi-Joong;Kim, Jin-Hwa;Song, Seung-Jin
    • Journal of Mechanical Science and Technology
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    • 제18권2호
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    • pp.272-285
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    • 2004
  • The losses at off-design points from a compressor cascade occur due to the deviation from a design incidence angle at the inlet of the cascade. The self-noise from the blade cascade at off-design points comes from a separated boundary layer and vortex sheddings. If the incidence angle to the cascade increases, stalling in blades may occur and the noise level increases significantly. This study applied Large-Eddy Simulations (LES) using deductive and deductive dynamic SGS models to low Mach-number, turbulent flow with each incidence angle to the cascade ranging from -40$^{\circ}$ to +20$^{\circ}$ and compared numerical predictions with measured data. It was observed that the oscillating separation bubbles attached to the suction surface do not modify wake flows dynamically for cases of negative incidence angles. However, an incidence angle greater than 8$^{\circ}$ caused a separated vortex near the leading edge to be shed downstream and created stalling. The computed performance parameters such as drag coefficient and total pressure loss coefficient showed good agreement with experimental results. Noise from the cascade of the compressor is summarized as sound generated by a structure interacting with unsteady, turbulent flows. The hybrid method using acoustic analogy was observed to closely predict the measured overall sound powers and directivity patterns at design and off-design points of blade cascade.

프로펠러와 허브 보오텍스 조절장치 상호작용 CFD 해석 (CFD Analysis of Marine Propeller-Hub Vortex Control Device Interaction)

  • 박현정;김기섭;서성부;박일룡
    • 대한조선학회논문집
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    • 제53권4호
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    • pp.266-274
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    • 2016
  • Many researchers have been trying to improve the propulsion efficiency of a propeller. In this study, the numerical analysis is carried out for the POW(Propeller Open Water test) performance of a propeller equipped with an energy saving device called PHVC(Propeller Hub Vortex Control). PHVC is aimed to control the propeller hub vortex behind the propeller so that the rotational kinetic energy loss can be reduced. The unsteady Reynolds Averaged Navier-Stokes(URANS) equations are assumed as the governing flow equations and are solved by using a commercial CFD(Computational Fluid Dynamics) software, where SST k-ω model is selected for turbulence closure. The computed characteristic values, thrust, torque and propulsion efficiency coefficients for the target propeller with and without PHVC and the local flows in the propeller wake region are validated by the model test results of KRISO LCT(Large Cavitation Tunnel). It is concluded from the present numerical results that CFD can be a good promising method in the assessment of the hydrodynamic performance of PHVC in the design stage.

와법을 이용한 원주군을 지나는 후류의 특성 계산 (The Characteristic Calculation of the Wake through Cylinders by Vortex Method)

  • 노기덕;오세경;변용수
    • Journal of Advanced Marine Engineering and Technology
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    • 제34권1호
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    • pp.76-83
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    • 2010
  • 본 연구는 정렬배열 및 엇갈림배열 상태에 놓인 원주군 주위의 유동장 특성을 와법으로 수치계산한 것이다. 계산은 피치 비 Pt/D=1.25~2.0, 레이놀즈 수 Re=$4.0{\times}10^1{\sim}4.0{\times}10^4$의 범위 내에서 각 유동장의 순간 볼텍스 분포, 순간 속도분포를 계산하였다. 정렬배열 및 엇갈림 배열 모두 각 원주의 상방에서는 시계방향의, 하방에서는 반시계방향의 볼텍스가 발생하였다. 각 배열 모두 원주군 후방에서 역류의 발생여부는 피치 비와 레이놀즈 수에 기인하며, 같은 레이놀즈 수에서는 피치 비가 작을수록, 그리고 같은 피치 비에서는 레이놀즈 수가 클수록 원주군 후방에서 역류발생이 쉽게 일어났다. 그리고 그 경계영역은 정렬배열의 경우 피치 비 Pt/D=1.5, 레이놀즈 수 Re=400~4,000, 엇갈림 배열의 경우 피치 비 Pt/D=1.4, 레이놀즈 수 Re=40~400에 존재했다.

주기 회전하는 원형 실린더 주위 층류 유동장의 수치 시뮬레이션 (Numerical Simulation on Laminar Flow Past a Rotary Oscillating Circular Cylinder)

  • 박종천;문진국;전호환;서성부
    • 대한조선학회논문집
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    • 제42권4호
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    • pp.368-378
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    • 2005
  • The effects of rotary oscillation on the unsteady laminar flow past a circular cylinder. are numerically investigated in the present study. The numerical solutions for the 20 Wavier-Stokes equation are obtained using a finite volume method Tn the framework of an overlapping grid system. The vortex formation behind a circular cylinder and the hydrodynamics of wake flows for different rotary oscillation conditions are analyzed from the results of numerical simulation. The lock-on region is defined as the region that the natural shedding frequency due to the Karmann Vortex shedding and the forcing frequency due to the forced oscillating a cylinder are nearly same, and the quasi-periodic states are observed around that region. At the intersection between lock-on and non-lock-on region the shedding frequency is bifurcated. After the bifurcation, one frequency fellows the forcing frequency($S_f$) and the other returns to the natural shedding frequency($St_0$). in the quasi-periodic states, the variation of magnitudes and relevant phase changes of $C_L$ with forcing phase are examined.

Large eddy simulation of flow around a stay cable with an artificial upper rivulet

  • Zhao, Yan;Du, Xiaoqing;Gu, Ming;Yang, Xiao;Li, Junjun;He, Ping
    • Wind and Structures
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    • 제26권4호
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    • pp.215-229
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    • 2018
  • The appearance of a rivulet at the upper surface of a stay cable is responsible for rain-wind-induced vibration (RWIV) of cables of cable-stayed bridges. However, the formation mechanism of the upper rivulet and its aerodynamic effects on the stay cable has not been fully understood. Large eddy simulation (LES) method is used to investigate flow around and aerodynamics of a circular cylinder with an upper rivulet at a Reynolds number of 140,000. Results show that the mean lift coefficients of the circular cylinder experience three distinct stages, zero-lift stage, positive-lift stage and negative-lift stage as the rivulet located at various positions. Both pressure-induced and friction-induced aerodynamic forces on the upper rivulet are helpful for its appearance on the upside of the stay cable. The friction-induced aerodynamic forces, which have not been considered in the previous theoretical models, may not be neglected in modeling the RWIV. In positive-lift stage, the shear layer separated from the upper rivulet can reattach on the surface of the cylinder and form separation bubbles, which result in a high non-zero mean lift of the cylinder and potentially induces the occurrence of RWIV. The separation bubbles are intrinsically unsteady flow phenomena. A serial of small eddies first appears in the laminar shear layer separated from the upper rivulet, which then coalesces and reattaches on the side surface of the cylinder and eventually sheds into the wake.

고가궤도에 근접한 자기부상열차 형상 주위의 3차원 난류유동에 대한 수치해석 (Computational Analysis of Three-Dimensional Turbulent Flow Around Magnetically Levitated Train Configurations in Elevated Track Proximity)

  • 맹주성;양시영
    • 한국자동차공학회논문집
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    • 제2권1호
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    • pp.9-25
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    • 1994
  • In the present study, the Reynolds-averaged Navier-Stokes equations, together with the equations of the $k-{\varepsilon}$ model of turbulence, were solved numerically in a general body-fitted coordinate system for three-dimensional turbulent flows around the six basic shapes of the magnetically levitated train(MAGLEV). The numerical computations were conducted on the MAGLEV model configurations to provide information on shapes of this type very near the elevated track at a constant Reynolds number of $1.48{\times}10^{6}$ based on the body length. The coordinate system was generated by numerically solving a set of Poisson equations. The convective transport equations were discretized using the finite-analytic scheme which employed analytic solutions of the locally-linearized equations. A time marching algorithm was employed to enable future extensions to be made to handle unsteady and fully-elliptic problems. The pressure-velocity coupling was treated with the SIMPLER-algorithm. Of particular interests were wall effect by the elevated track on the aerodynamic forces and flow characteristics of the six models calculated. The results indicated that the half-circle configuration with extended sides and with smooth curvature of sides was desirable because of the low aerodynamic forces and pitching moment. And it was found that the separation bubble was occured at wake region in near the elevated track.

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