• 제목/요약/키워드: Vorticity Field

검색결과 153건 처리시간 0.028초

쓰나미 파형이 수중식생의 에너지소산에 미치는 영향 (Effects of Tsunami Waveform on Energy Dissipation of Aquatic Vegetation)

  • 이우동;박종률;전호성;허동수
    • 한국해양공학회지
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    • 제31권2호
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    • pp.121-129
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    • 2017
  • The present study numerically investigated the influence of the waveform distribution on the tsunami-vegetation interaction using a non-reflected wave generation system for various tsunami waveforms in a two-dimensional numerical wave tank. First, it was possible to determine the wave attenuation mechanism due to the tsunami-vegetation interaction from the spatial waveform, flow field, vorticity field, and wave height distribution. The combination of fluid resistance in the vegetation and a large gap and creates a vortex according to the flow velocity difference in and out of the vegetation zone. Thus, the energy of a tsunami was increasingly reduced, resulting in a gradual reduction in wave height. Compared to existing approximation theories, the double volumetric ratio of the waveform increased the reflection coefficient of the tsunami-vegetation interaction by 34%, while decreasing the transfer coefficient and energy attenuation coefficient by 25% and 13%, respectively. Therefore, the hydraulic characteristics of a tsunami is highly likely to be underestimated if the solitary wave of the approximation theory is applied for the tsunami.

PIV 계측과 CFD 해석을 통한 오일펜스 만곡부 단면에서의 유동장 특성 (Characteristics of Flow Field at Curved Section of Oil Fence using PIV Measurements and CFD Simulations)

  • 김태호;장덕종;나선철;배재현;김대안
    • 해양환경안전학회지
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    • 제17권1호
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    • pp.29-37
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    • 2011
  • 유속의 변화에 따른 오일펜스 만곡부 후면의 속도장과 압력장, 와도 및 난류 강도를 계측한 PIV 실험의 결과 유속이 증가함에 따라 유동 경계역의 후면부에서의 흐름 방향이 전면부의 흐름 방향에 가까워지는 현상이 나타났고, 압력 분포의 양상이 달라졌으며 난류도 더욱 불규칙적인 형태로 나타났다. PIV 실험과 동일 조건으로 수행한 CFD 해석 결과, 후류의 유동 패턴이 0.3m/s이하의 저속인 경우는 PIV 실험 결과와 유사하게 나타났으나, 유속이 0.4m/s일 때는 오일펜스 자체의 유연성으로 인해 다소 차이가 나타났고, 오일펜스 하단의 압력차로 인한 불규칙한 난류가 수면까지 영향을 주었다.

PIV기법을 이용한 트랜섬 선미 후류 점성유동장 계측 (PIV Measurement of Viscous Flow Field in the Wake of Transom Stern)

  • 이경우;김옥석
    • 한국항해항만학회지
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    • 제35권10호
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    • pp.805-810
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    • 2011
  • 트랜섬 선미 형상변화에 따른 후류 유동특성을 알아보기 위해 $Re=3.5{\times}103$$Re=7.0{\times}103$에서 수면하부 유동을 계측하였다. 선미형상변화에 따른 유동장 계측을 위해 2-프레임 그레이레벨 상호상관 PIV기법을 이용하여 분석하였다. 선미형상은 실선조사 결과를 바탕으로 선저와 이루는 각을 각각 $45^{\circ}$(모델 A), $90^{\circ}$(모델 B) 및 $135^{\circ}$(모델 C)를 실험에 적용하였다. 모델의 선미 침수면의 깊이는 자유 수면으로부터 40mm를 기초하였다. 레이놀즈수가 증가함에 따라, 와의 규모가 증가하고 하류로 길게 형성되는 경향을 나타냈다.

자동차 후류에서 에어스포일러의 영향에 대한 PIV 측정 (Effects of the Air Spoiler on the Wake Behind a Road Vehicle by PIV Measurements)

  • 김진석;성재용;김정수;최종욱;김성초
    • 대한기계학회논문집B
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    • 제30권2호
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    • pp.136-143
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    • 2006
  • A particle image velocimetry (PlV) technique has been applied to measure the quantitative flow field characteristics behind a road vehicle with/without an air spoiler attached on its trunk and to estimate its effect on the wake. A vehicle model scaled in the ratio of 1/43 is set up in the mid-section of a closed-loop water tunnel. The Reynolds number based on the vehicle length is $10^5$. To investigate the three-dimensional structure of the recirculation zone and vortices, measurements are carried out on the planes both parallel and perpendicular to the free stream, respectively. The results show significant differences in the recirculation region and the vorticity distributions according to the existence of the air spoiler. The focus and the saddle point, appearing just behind the air spoiler, are disposed differently along the spanwise direction. Regarding the streamwise vortices, the air spoiler produces large wing tip vortices. They have opposite rotational directions to C-pillar vortices which are commonly observed in case that the air spoiler is absent. The wing tip vortices generate the down-force and as a result, they can make the vehicle more stable in driving.

Lattice-Boltzmann Simulation of Fluid Flow around a Pair of Rectangular Cylinders

  • Taher, M.A.;Baek, Tae-Sil;Lee, Yeon-Won
    • Journal of Advanced Marine Engineering and Technology
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    • 제33권1호
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    • pp.62-70
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    • 2009
  • In this paper, the fluid flow behavior past a pair of rectangular cylinders placed in a two dimensional horizontal channel has been investigated using Lattice-Boltzmann Method(LBM). The LBM has built up on the D2Q9 model and the single relaxation time method called the Lattice-BGK(Bhatnagar-Gross-Krook)model. Streamlines, velocity, vorticity and pressure contours are provided to analyze the important characteristics of the flow field for a wide range of non dimensional parameters that present in our simulation. Special attention is paid to the effect of spacing(d) between two cylinders and the blockage ratio A(=h/H), where H is the channel height and h is the rectangular cylinder height. for different Reynolds numbers. The first cylinder is called upstream cylinder and the second one as downstream cylinder. The downstream fluid flow fields have been more influenced by its blockage ratios(A) and Reynolds numbers(Re) whereas the upstream flow patterns(in front of downstream cylinder) by the gap length(d) between two cylinders. Moreover, it is observed that after a certain gap, both upstream and downstream flow patterns are almost similar size and shape. The simulation result has been compared with analytical solution and it is found to be in excellent agreement.

고차의 수치적 기법을 적용한 충격소음의 생성 및 전파 해석 (Numerical analysis of the impulsive noise generation and propagation using high order scheme)

  • 김민우;김성태;김규홍;이수갑
    • 한국소음진동공학회:학술대회논문집
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    • 한국소음진동공학회 2007년도 추계학술대회논문집
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    • pp.1494-1498
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    • 2007
  • Impulsive shooting noise is basically complex phenomenon which contains the linear and non-linear characteristics. For those reasons, numerical analysis of impulsive shooting noise has the difficulties in control of the numerical stability and accuracy on the simulation. In this research, Wave-number Extended Finite Volume Scheme (WEFVS) is applied to the numerical analysis of impulsive shooting noise. In the muzzle blast flow simulation, the generation of the precursor wave and the induced vortex ring are observed. Consequently, blast wave. vortex ring interaction and vortex ring. bow shock wave interaction are evaluated on the shooting process using the accurate and stable scheme. The sound generation in the interactions can be explained by the vorticity transport theorem. The shear layer is evolved behind the projectiles due to the jet flow. In these computations, the impulsive shooting noise is generated by the complex interaction with shooting process and is propagated to the far-field boundary. The impulsive shooting noise generation can be observed by the applications of WEFVS and analyzed by the physical phenomena.

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평행평판 내의 지주에 의한 와동 유동에 관한 수치해석 (Numerical Computation of Vertex Behind a Bluff Body in the Flow between Parallel Plates)

  • 김동성;유영환
    • 대한기계학회논문집
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    • 제16권6호
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    • pp.1163-1170
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    • 1992
  • 본 연구에서는 자동차 전자제어식 공기유량계를 Fig.2와 같이 평행평판 안에 사각 지주가 있다고 단순화하고 공기는 이차원 비 압축성 점성유동으로 가정했다. 지배방정식은 유체 운동량방정식(navier-Stokes equation)을 와도 전달 방정식(vorti- city transport equation)과 유량 함수 방정식(stream function equation)으로 변환하 여 사용하였다. Peacemanrachford ADI 방법으로 수치해석 하였으며, 유량 함수 방정 식의 수렴성을 좋게 하기 위하여 Wachspress parameter를 사용하였다. 벽면의 경계 조건은 Briely의 4th-order Lagrange interpolation 방법을 따랐다. Reynolds 수 200과 500에서의 비정상유동(unsteady flow)을 계산하였으며, 유동이 정상상태(steady state)에 도달하였을 때에 유동을 교란시켜 와동 흘림(vortex shedding)을 구하였다.

단일공급 스월 혼합챔버 내의 와류유동에 대한 실험적 연구 (Experimental Investigation on the Vortical Flows in a Single-Entry Swirl Mixing Chamber)

  • 김형민;윤웅섭
    • 한국추진공학회:학술대회논문집
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    • 한국추진공학회 2011년도 제37회 추계학술대회논문집
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    • pp.445-450
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    • 2011
  • 금속분말을 연소시키기 위한 스월 연소기 설계의 기초단계로써 단일 접선 공급유로를 갖는 스월 혼합챔버를 제작하고 Paticle Image Velocimetry(PIV)를 사용하여 스월 혼합챔버의 내부 유동장 측정실험을 수행하였다. 상온의 공기를 작동유체로 사용하였으며 접선 공급유량이 증가하는 경우의 스월 혼합 챔버 내 축방향 및 접선방향 성분 속도를 획득하였다. 측정된 유동장을 바탕으로 스월유동과 역압력 구배로 인해 발생하는 외부 유입유동간의 혼합특성을 평가 하였다.

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Numerical Experiment on the Sogcho Eddy due to the strong offshore winds in the East Sea

  • Kim Soon Young;Lee Hyong Sun;Lee Jae Chul
    • Fisheries and Aquatic Sciences
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    • 제1권1호
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    • pp.7-18
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    • 1998
  • In order to understand the generation of the Sogcho Eddy due to the strong offshore winds, we first investigated the characteristics of winds at Sogcho, Kangnung and Samchuk, and then carried out a series of numerical experiments using the nonlinear 1 1/2-layer model. The models were forced by wind stress fields, similar in structure to the prevailing winds that a field in the east coast of Korea during the winter season. The winds were composed of the background winds $(-1\;dyne/cm^2)$ for 90 days and the local winds $(-4\;dyne/cm^2)$ for 30 days. The analysis of wind data at three stations (Sogcho, Kangnung, and Samchuk) showed that the wind was stronger in winter than in other seasons and the offshore component was much dominant. According to our numerical solutions, the Sogcho Eddy of about 200 km in diameter was generated due to the strong offshore winds prevailing in the Kangnung - Sogcho regions. The eastward propagation of the Rossby waves reflected at the western boundary resulted in the eastward meandering motion from the eastern side of the eddy.

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Wiggle Instability of Magnetized Spiral Shocks

  • Kim, Yonghwi;Kim, Woong-Tae
    • 천문학회보
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    • 제39권2호
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    • pp.77.1-77.1
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    • 2014
  • Galactic spiral arms are abundant with interesting gaseous substructures. It has been suggested that arm substructures arise from the wiggle instability (WI) of spiral shocks. While the nature of the WI remained elusive, our recent work without considering magnetic fields shows that the WI is physically originated from the accumulation of potential vorticity (PV) generated by deformed shock fronts. To elucidate the characteristics of the WI in more realistic galactic situations, we extend our previous linear stability analysis of spiral shocks by including magnetic fields. We find that magnetic fields reduce the amount of density compression at shocks, making the shock fronts to move toward the upstream direction. Magnetic tension forces from bent field lines stabilize the WI by prevent the generation of PV. When the spiral-arm forcing is F=5% of the centrifugal force of galaxy rotation, the maximum growth rate of the WI is found to be about 1.0, 0.4, and 0.2 times the orbital angular frequency for the plasma parameter ${\beta}=100$, 10, and 5, respectively. Shocks with ${\beta}=1$ are stable to the WI for F=5%, while becoming still unstable when F=10%.

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