• 한국가시화정보학회지
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• 제18권2호
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• pp.39-45
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• 2020

Problems related with flows around structures are typical in various engineering fields. The characteristics of these flow structures depend strongly on the shape of the body. The flow regime around square cylinders which are also employed in various applications has also been investigated. In addition to a single body, flows past closely spaced structures arranged in tandem are observed in numerous practical applications. In this study, the flow characteristics around the circular and the square cylinder were investigated according to S/D. The velocity fields and Reynolds stress of the single cylinders were acquired to explain the flow behaviors between tandem cylinders. The differences observed in the flow behaviors of square and circular cylinders were studied. The flow patterns around two tandem cylinders can be classified into three types of wake interference behaviors according to S/D. This is related with the flows between cylinders.

• 대한기계학회논문집B
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• 제37권4호
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• pp.359-366
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• 2013

본 연구는 두 원기둥의 유동에 기인한 진동에 관한 실험적 연구이다. 두 원기둥이 직렬 배열(${\alpha}=0^{\circ}$), 대각선 배열(${\alpha}=5^{\circ}$, $10^{\circ}$, $15^{\circ}$, $25^{\circ}$, $45^{\circ}$, $60^{\circ}$), 병렬 배열(${\alpha}=90^{\circ}$) 됐을 때 두 원기둥의 간격(L/D)과 유속을 변화 시켰을 때의 진동 특성을 조사했다. 그 결과 다음과 같은 결과를 얻었다. (i)직렬, 대각선, 병렬 배열된 두 원기둥에서 발생하는 유동에 기인한 진동의 패턴은 7 개 패턴이다. (ii)복수로 존재하는 두 원기둥의 유동에 기인한 진동은 서로 진동을 유발시킨다. (iii) 두 원기둥의 직렬, 대각선, 병렬 배열 중에 유동에 기인한 진동을 유발하기 가장 쉬운 배열은 병렬 배열이다. (iv) 모든 배열에서 두 원기둥의 간격변화에 따른 최대 진폭의 변화는 변동 양력 계수의 변화와 유사하다.

• Journal of Advanced Marine Engineering and Technology
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• 제27권1호
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• pp.49-56
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• 2003

The hydrodynamic interference between two circular cylinders in tandem and side by side arrangements was investigated by measuring of lift and drag on each cylinder. The time variations of interference lift and drag coefficients in each arrangement were observed at center-to-center pitch ratios of P/D=1.25 and 2.5 and Reynolds number of $Re=1.5\times10^4$. Average interference lift and drag coefficients were also observed at pitch ratios from P/D=1.25 to 2.5 and Reynolds number from $Re=1.5\times10^4$ to $1.5\times10^4$. The hydrodynamic interference between two circular cylinders differed with the shape of the arrangement and the pitch ratio, but the characteristics were revealed by measuring of lift and drag on each cylinder.

• 대한기계학회논문집
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• 제17권6호
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• pp.1518-1528
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• 1993

본 연구는 단일 원주의 와여기 진동특성에 관한 연구의 연속연구로서 풍동내 에 직렬로 배열된 두 원주의 직교유동에 의한 두 가지 경우의 동적 거동을 조사하였다. 첫째는 상류측 탄성지지 원주의 후류내에 가깝게 놓여진 하류측 고정원주의 간섭에 의한 상류측 원주의 진동(proximity-induced vibration)이며, 둘째는 상류측의 고정원 주의 후류내에 가깝게 놓여진 하류측 탄성지지 원주의 공기역학적 진동(wake-induced vibration)이다. 본 연구의 목적으로 직렬로 배열된 동일 직경의 두 원주에 있어서 어느 한 쪽의 원주가 탄성지지가 되어 있을 경우, 두 원주사이의 간격과 유속변화에 따른 와여기 진동과 유력탄성 불안정 진동의 진동특성 및 후류내에서의 와유출 특성을 명확히 하기 위해 실험적으로 조사, 연구하였다.

• Journal of Advanced Marine Engineering and Technology
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• 제31권2호
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• pp.159-165
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• 2007

The Characteristics of the flowfield around two circular cylinders in tandem arrangement was investigated by PIV. Strouhal numbers. velocity vectors and velocity profiles were observed at centre-to-centre space ratios of P/D= 1.5. 2.0 and 2.5, and Reynolds number of $Re=3.0{\times}10^3{\sim}5.0{\times}10^3$. As the results the Strouhal numbers measured in the rear region of the cylinder of wake side were decreased with the space ratios. The flow between two cylinders was almost stagnated and the size of the stagnated region was larger in the close side than in the far side of the front cylinder. The direction of vortex between two cylinders was opposed each other with the small difference(${\alpha}\;{\pm}1.0^{\circ}$) of the attack angle ${\alpha}$.

• Wind and Structures
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• 제30권5호
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• pp.475-483
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• 2020

This work investigates Reynolds number Re (= 50 - 200) effects on the flows around a single cylinder and the two tandem (center-to-center spacing L^⁎= L/D = 4) cylinders, each of a diameter D. Vorticity structures, Strouhal numbers, and time-mean and fluctuating forces are presented and discussed. For the single cylinder, with increasing Re in the range examined, the vorticity magnitude, Strouhal number and fluctuating lift all monotonically rise but time-mean drag, vortex formation length, and lateral distance between the two rows of vortices all shrink. For the two tandem cylinders, the increase in Re leads to the formation of three distinct flows, namely reattachment flow (50 ≤ Re ≤ 75), transition flow (75 < Re < 100), and coshedding flow (100 ≤ Re ≤ 200). The reattachment flow at Re = 50 is steady. When Re is increased from 75 to 200, the Strouhal number of the two cylinders, jumping from 0.113 to 0.15 in the transition flow regime, swells to 0.188. The two-cylinder flow is more sensitive to Re than the single cylinder flow. Fluctuating lift is greater for the downstream cylinder than the upstream cylinder while time-mean drag is higher for the upstream cylinder than for the other. The time-mean drags of the upstream cylinder and single cylinder behaves similar to each other, both declining with increasing Re.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2001년도 춘계학술대회논문집E
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• pp.582-587
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• 2001

A numerical method using FLUENT code was employed to investigate fluid drag and lift forces on a cylinder in a group of circular cylinders, subjected to a uniform cross flow. The cylinders can be arranged in tandem or in a staggered arrangements relative to the free stream flow. A vortex street behind the cylinder pairs or jets between the cylinders forms according to the arrangements. Vibration on a cylinder can occurs due to vortex shedding, fluid-elastic stiffness and wake galloping. The flow is first investigated and then the forces acting on the cylinder are calculated. The lift and drag forces on an elastically mounted cylinder in the wake of an upstream fixed cylinder arise from the mean flow plus velocity and pressure gradients in the wake. The analytical results of two staggered cylinder were compared with the existing experimental ones for validation of the present method. The analytical results of the forces were in good agreement with the experimental ones. The present method can be used for the analysis of the fluid induced vibration where the group of circular cylinders are subjected to a cross flow.

• 한국수자원학회:학술대회논문집
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• 한국수자원학회 2015년도 학술발표회
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• pp.334-334
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• 2015

The results of flow feature around two circular cylinders in various arrangements are carried out using two-dimensional simulation at Reynolds number of 200. In this work, time-averaged fluid force acting on the upstream and downstream cylinders were calculated for staggered angle ${\alpha}=0{\sim}90^{\circ}$ in the range of L/D = 1.1~5, where ${\alpha}$ is the angle between the free-stream flow and the line connecting the centers of the cylinders, L is centre-to-centre distance and D is cylinder diameter. The dependence of magnitudes and trends of fluid force coefficient on the spacing ratio L/D and ${\alpha}$ are discussed. In all arrangements of two cylinders, tandem arrangement (${\alpha}=0^{\circ}$) is the case produced a minimum drag coefficient for downstream cylinder. Moreover, the locations of separation and stagnation points or pressure coefficient on surface of the cylinder were examined. Acknowledgement: "This research was a part of the project titled 'Development of integrated estuarine management system', funded by the Ministry of Oceans and Fisheries, Korea."

• 한국항공우주학회지
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• 제36권2호
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• pp.131-136
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• 2008

본 연구는 다양한 배열 상태에 놓인 2원주 주위의 유동장 특성을 PIV를 이용하여 파악한 것이다. 직렬배열에서 하류측 원주의 후방에서 측정한 Strouhal 수는 수평 간격비가 클수록 작게 나타났다. 직렬배열에서 2원주 사이의 흐름은 거의 정체되어 있으며, 상류측 원주에 가까울수록 정체 범위가 크게 나타났다. 직렬배열에서 자유류와 2원주의 중심선이 이루는 받음각()의 미소 변화(${\alpha}$=${\pm}1.0^{\circ}$)에 따라 2원주 사이에는 서로 반대 방향의 와류가 생성되었다. 병렬배열에서 수직 간격비가 클수록 2원주 사이의 유속이 크게 나타났다.

• 한국입자에어로졸학회지
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• 제17권4호
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• pp.81-89
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• 2021

Understanding particle-laden flow around cylindrical bodies is essential for the better design of various applications such as filters. In this study, laminar flows around two tandem cylinders and the motions of particles in the flow are numerically investigated at low Reynolds numbers. We aim to reveal the effects of the spacing between cylinders, Reynolds number and particle Stokes number on the characteristics of particle trajectories. When the cylinders are placed close, the unsteady flow inside the inter-cylinder gap at Re = 100 shows a considerable modification. However, the steady recirculation flow in the wake at Re = 10 and 40 shows an insignificant change. The change in the flow structure leads to the variation of particle dispersion pattern, particularly of small Stokes number particles. However, the dispersion of particles with a large Stokes number is hardly affected by the flow structure. As a result, few particles are observed in the cylinder gap regardless of the cylinder spacing and the Reynolds number. The deposition efficiency of the upstream cylinder shows no difference from that of a single cylinder, increasing as the Stokes number increases. However, the deposition on the downstream cylinder is found only at Re = 100 with large spacing. At this time, the deposition efficiency is generally small compared to that of an upstream cylinder, and the deposition location is also changed with no deposited particles near the stagnation point.