• Title/Summary/Keyword: 난류 응집구조

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A Framework for Size Distribution of Noncohesive Sediment (비점착성 유사의 입도 분포 모형에 관한 Framework)

  • Byun, Jisun;Son, Minwoo;Park, Byeoung Eun;Moon, Hyejin
    • Proceedings of the Korea Water Resources Association Conference
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    • 2017.05a
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    • pp.282-282
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    • 2017
  • 모래, 실트 및 자갈과 같은 비점착성 유사는 하천에서의 이동 형태에 따라 소류사와 부유사로 구분된다. 부유사는 난류로 인해 흐름 내에서 부유 상태로 이동하는 유사로, 대부분의 자연 하천에서 유사는 부유사 형태로 이송된다. 유수동역학적 조건 하에서 이동하는 부유사의 입도 분포는 유사 입자의 부유와 퇴적에 따라 불규칙적으로 변화하기 때문에 여러 연구에서 주요한 문제로 다뤄지고 있다. 부유사의 입도 분포는 흐름 유속, 부유사의 부유 높이, 하상 재료의 특성 등에 따라 변화하며, 로그 정규분포를 따르는 것으로 알려져 있다. 이에 본 연구에서는 여러 다양한 하천 흐름 조건에서 부유사의 입도 분포를 모의할 수 있는 입도 분포 모형에 관한 개념적 틀(Framework)을 제안한다. 유사 입자의 입도 분포 모의는 추계학적 방법의 적용을 통해 얻어진다. 본래 점착성 유사의 입도 분포를 모의하기 위한 추계학적 입도 분포 모형으로부터 제안된 개념적 틀로, 다양한 흐름 조건 하에서 특정 확률 분포형을 띠는 입도 분포를 모의할 수 있다. 점착성 유사의 이동 모형에서는 점착성을 띠는 유사 입자들의 응집 현상에 따른 크기 변화를 모의하기 위한 응집 모형이 필수적이다. 시간에 따른 크기 변화를 모의하는 응집 모형에서, 흐름 내 여러 특성들에 의해 결정되는 응집 인자와 달리 파괴 인자의 경우 불규칙적 난류 운동으로 인해 무작위한 특성을 띤다. 모형에서 요구되는 파괴 인자를 특정 확률 분포형을 띠는 난수로 고려함으로써 점착성 유사의 입도 분포 모형이 개발되었다. 이 때, 점착성 유사는 프랙탈 구조를 가지는 것으로 가정하기 때문에 크기에 따라 밀도와 침강 속도가 변화한다. 반면 비점착성 유사는 크기에 따른 밀도 변화가 일어나지 않으므로, 고정된 밀도와 프랙탈 차원을 적용하여 점착성 유사의 입도 분포모형으로부터 비점착성 유사의 입도 분포 모의가 가능할 것으로 판단된다. 이러한 추계학적 방법의 적용을 통해, 하나의 경계 조건으로 대변되는 하상 특성에 따른 단점 또한 보완될 것으로 예측된다. 예를 들어 로그 정규 분포를 띤다고 가정할 때 보정을 통해 결정해야하는 변수는 평균과 분산으로 두 개가 요구된다. 유사의 평균 크기로부터 확률분포형의 평균값이 결정되면, 하상에 존재하는 유사의 특성에 따른 입도 분포의 분산은 난수의 분산을 결정함으로써 모의할 수 있다.

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A Study on the Effect of Large Coherent Structures to the Skin Friction by POD Analysis (적합직교분해(POD)기법을 사용한 난류 응집구조 거동에 관한 연구)

  • Shin, Seong-Yun;Jung, Kwang-Hyo;Kang, Yong-Duck;Suh, Sung-Bu;Kim, Jin;An, Nam-Hyun
    • Journal of the Society of Naval Architects of Korea
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    • v.54 no.5
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    • pp.406-414
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    • 2017
  • An experimental study in a recirculating water channel was carried out to investigate the effect of large coherent structures to the skin friction on a flat plate. Particle Image Velocimetry (PIV) technique was used to quantify characteristic features of coherent structures growing to the boundary layer. In the PIV measurement, it is difficult to calculate the friction velocity near the wall region due to laser deflection and uncertainty so that Clauser fitting method at the logarithmic region was adopted to compute the friction velocity and compared with the one directly measured by the dynamometer. With changing the free-stream velocity from 0.5 m/s to 1.0 m/s, the activity of coherent structures in the logarithmic region was increased over three times in terms of Reynolds stress. The flow field was separated by Variable Interval Time Averaging (VITA) technique into the weak and the strong structure case depending on the existence large coherent structures in order to validate its effectiveness. The stream-wise velocity fluctuation was scanned through at the boundary thickness whether it had a large deviation from background flow. With coherent structures connected from near-wall to the boundary layer, mean wall shear stress was higher than that of weak structure case. Proper Orthogonal Decomposition (POD) analysis was also applied to compare the energy budget between them at each free-stream velocity.

Bio-mediated Flocculation by Extracellular Polymeric Substances in Cohesive Sediment Suspensions: Experimental Study (생체고분자물질이 부유사 응집에 미치는 영향 연구)

  • Baek, Seung-Ryong;Kim, Jae-In;O, Min-Ji;Lee, Byeong-Jun
    • Proceedings of the Korea Water Resources Association Conference
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    • 2015.05a
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    • pp.107-107
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    • 2015
  • 최근 기후변화로 인한 강우강도 증대, 산업화에 따른 토지개발 등으로 인하여 다량의 점착성 부유사(Cohesive Sediments)가 하천, 호소 등 수자원 환경으로 유입되고 있다. 점착성 부유사는 하천, 호소의 난류 조건에 따라 부유하거나 혹은 응집, 침전하여 하상 저니층을 형성한다. 부유사, 미생물 및 각종 유기입자가 포함된 하상 저니층은 검은색으로 외관상 보기 좋지 않을 뿐 아니라, 혐기성상태에서 부패하여 수생태계의 건강성을 해치게 된다. 또한 미세 부유사 및 미생물 입자는 각종 중금속, 유기오염물질을 흡착하고, 조건에 따라 재용출할 수 있는 저장매체로 작용하기 때문에 수자원환경에 미치는 영향이 아주 크다. 특히, 수중 미생물(조류) 작용에 의해 생성되는 EPS (Extracellular Polymeric Substances)는 부유사 및 미생물 입자들을 서로 엉겨 붙게 하여, 부유사-미생물 혼합 응집체 및 저니층 형성을 가속화하게 된다. 본 연구에서는 EPS가 부유사 응집에 미치는 영향을 파악하기 위하여, Xanthan Gum (Sigma-Aldrich, USA)을 EPS의 지표 물질로 사용하고, Kaolinite(Sigma-Aldrich, USA)를 수자원환경에 존재하는 대표적인 부유사로 사용하여 응집실험(Jar Test)을 수행하였다. 이온농도가 응집에 미치는 영향을 파악하기 위하여 수체 이온농도를 0.0001M NaCl, 0.001M NaCl, 0.01M NaCl, 그리고 0.001M NaCl + 0.1mg/L $Ca^{2+}$, 0.001M NaCl + 0.5mg/L $Ca^{2+}$, 0.001M NaCl + 1.0 mg/L $Ca^{2+}$으로 보정하여 응집실험을 수행하였다. 250 rpm 급속 교반 1븐, 50 rpm 완속교반 5시간, 침잔 1시간 후 응집체를 채취하여 응집체 이미지 분석을 통해 응집체 크기 및 형상을 측정하였고, 수표면 2 cm 지점에서 상등액을 채수하여 잔류 고형물 농도 분석을 실시하였다. 응집실험을 통하여 다음과 같은 결과를 도출하였다.. 낮은 이온농도의 경우, EPS가 큰 고분자 구조체에 부유 입자들이 엮어 응집되는 Sweeping Flocculation의 특징을 나타내었다. 하지만, 이온농도가 높아질수록 경우, EPS 고분자 구조체 내부 반발력이 감소하여 크기가 축소되고, 이에 따라 부유 입자 표면에 패치 형태로 흡착되었다. EPS가 패치형태로 입자에 흡착한 경우, 응집제 농도 증가에 따라 응집능 최적점이 형성되고, 이후 표면하전 역전이나 Steric Stabilization에 의해 응집능이 저감되는 형태를 나타낸다. 따라서,수중이온농도가 EPS의 사슬형 고분자 응집제의 크기, 형태(Morphology)를 결정하고, 더 나아가 응집능을 결정하는 중요한 인자로 나타났다. 따라서, 후속 연구를 통하여 생체고분자물질의 크기 및 형태 변화, 이에 따른 응집능변화를 면밀히 연구하고자 한다.

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Spanwise growth of coherent structures in turbulent pipe flow (난류 파이프 유동 내 응집 구조의 횡 방향 성장)

  • Ahn, Junsun;Lee, Jinyoung;Hwang, Jinyul
    • Journal of the Korean Society of Visualization
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    • v.19 no.2
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    • pp.26-31
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    • 2021
  • The spanwise growth of turbulence structures in turbulent pipe flow was investigated using the direct numerical simulation data of Re𝜏 = 544, 934 and 3008. Two-point correlations and pre-multiplied energy spectra of streamwise velocity fluctuations were examined along the spanwise direction. The arclength direction is defined as r𝛳, which is useful for an analogy with the spanwise direction for channels or boundary layers; here, r and 𝛳 are the radial distance from the core and the azimuthal angles, respectively. Both analyses showed that the arclength scales increased with increasing the wall-normal distance. It showed that the coherent structures were confined in the core region due to the crowding effect of a circular pipe geometry. The pipe flow simulation could describe a realistic geometrical flow along the azimuthal direction, unlike the simulations of turbulent channel or boundary layer flow using periodic boundary conditions along the spanwise direction. The present results provided the spanwise organization of energy-containing motions over a broad range of scales in turbulent pipe flow.

Dynamic characteristics analysis of forcing jet by Karhunen-Loeve transformation (Karhunen-Loeve 변환을 이용한 Forcing 제트의 동적 특성 해석)

  • Lee, Chan-Hui;Lee, Sang-Hwan
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.21 no.6
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    • pp.758-772
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    • 1997
  • The snapshot method is introduced to approximate the coherent structures of planar forcing jet flow. The numerical simulation of flow field is simulated by discrete vortex method. With snapshot method we could treat the data efficiently and approximate coherent structures inhered in the planer jet flow. By forcing the jet at a sufficient amplitude and at a well-chosen frequency, the paring can be controlled in the region of the jet. Finally we expressed the underlying coherent structures of planar jet flow in the minimum number of modes by Karhunen-Loeve transformation in order to understand jet flow and to make the information storage and management in computers easier.

Transition of Turbulent Boundary Layer with a Step Change from Smooth to Rough Surface (표면 형상 변화에 따른 난류경계층 유동장 분석)

  • Lee, Jae Hwa
    • Journal of the Korean Society of Visualization
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    • v.12 no.3
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    • pp.15-20
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    • 2014
  • Direct numerical simulation (DNS) dataset of a turbulent boundary layer (TBL) with a step change from smooth to rough surface is analyzed to examine spatially developing flow characteristics. The roughness elements are periodically arranged two-dimensional (2-D) spanwise rods with a streamwise pitch of ${\lambda}=8k$ ($=12{\theta}_{in}$), and the roughness height is $k=15{\theta}_{in}$, where ${\theta}_{in}$ is the inlet momentum thickness. The step change is introduced $80{\theta}_{in}$ downstream from the inlet. For the first time, full images from the DNS data with the step change from the smooth to rough walls is present to get some idea of the geometry of turbulent coherent structures over rough wall, especially focusing on their existence and partial dynamics over the rough wall. The results show predominance of hairpin vortices over the rough wall and their spanwise scale growth mechanism by merging.

Coherent Structures of Turbulent Wake Past a Rotating Circular Cylinder with a Tripping Wire (Tripping wire가 부착된 회전원주에 의한 난류휴류의 응집구조)

  • 부정숙;이종춘
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.19 no.8
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    • pp.1927-1939
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    • 1995
  • An experimental investigation is conducted to find out the large scale coherent structures in the intermediate wake past a rotating cylinder with a single tripping wire attached. Relation between the vortex shedding frequency and the spin rate of rotating cylinder and the effects of the tripping wire on the flow characteristics were studied by using spectral analysis and conditional phase average technique, respectively. It is found that the vortex shedding frequency is bound to a certain range and varies regularly as spin rate increases. The coherent structures are compared with those of the plain rotating cylinder in the case of spin rate of 1.0. Distance between the upper and lower center of vortices increase and the vortex shedding time is delayed, the velocity fluctuation energy decreases near the center line of vortices and it spreads out to the outer region. The Reynolds shear stress increases highly in the upper region and the turbulent wake width expands with strong entrainment process.

Large-Scale Vertical Structure in Separated and Reattaching Turbulent flow over a Backward Facing Step (후향계단 난류 박리재부착 유동에서의 대형와의 구조)

  • Ahn, Seung-Kwang;Lee, In-Won;Sung, Hyung-Jin
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.26 no.12
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    • pp.1674-1680
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    • 2002
  • An experimental study was made of a large-scale vortical structure over a backward-facing step. The Reynolds number based on the step height was R $e_{H}$ =33,000. To recognize the large-scale vortex, three components of velocity were measured. The measurements were performed in the recirculation zone (x/H=4.0) and the reattachment zone(x/H=7.5). To measure the wall pressure fluctuations in a turbulent flow over a backward-facing step, a 32-channel microphone array was installed beneath the wall in the streamwise and spanwise directions. From the measured pressure field, the size of large-scale vortex was obtained. As a detailed study, a conditionally-averaging technique was employed to characterize the coherent structure of the large-scale vortex. To see the relationship between the flow field and the relevant spatial mode of the pressure field, the spatial box filtering (SBF) was examined. A cross-correlation between velocity and pressure fluctuations was performed to identify the structure and the length scale of the large-scale vortex.x.

A Study on the Characteristics of Cylinder Wake Placed in Thermally Stratified Flow (IV) -On the Cylinder Wake with Various Heating Rates- (열성층유동장에 놓인 원주후류의 특성에 대한 연구 (4) -가열량의 변화에 따른 원주후류에 대하여-)

  • 김경천;정양범
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.19 no.5
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    • pp.1340-1350
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    • 1995
  • The effects of thermal stratification on the flow past a heated circular cylinder with various heating rates were examined in a wind tunnel. Turbulent intensities, r.m.s.values of temperature and turbulent convective heat flux distributions in the cylinder wakes with and without thermal stratification were measured by using a hot-wire and cold-wire combination probe. The phase averaging method was also used to estimate coherent contributions to the turbulent flow field in the near wake. The results show that the scalar mixing process is very different according to the mean temperature fields especially in the upper part of the wake. The coherent structure of the temperature field makes a large contribution to the time mean value like velocity components. However, the coherency of the temperature fluctuation is very different with the change of mean temperature fields, though the velocity coherent motions are quite similar in all experimental conditions.

A Study of 3-Dimensional Turbulent Channel Flow Using Discrete Wavelet Transform (이산 웨이블릿 변환을 이용한 3차원 난류 채널 유동에 관한 연구)

  • Kim Kangshik;Lee Sanghwan
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.29 no.3 s.234
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    • pp.314-321
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    • 2005
  • Discrete Wavelet Transform (DWT) has been applied to the Direct Numerical Simulation (DNS) data of turbulent channel flow. DWT splits the turbulent flow into two orthogonal parts, one corresponding to coherent structures and the other to incoherent background flow. The coherent structure is extracted from not vorticity field but velocity's since the channel flow is not isoropic. By comparing DWT's result of channel flow with that of isotropic flow, it is shown that coherent structure maintains the properties of original channel flow. The velocity field of coherent structures can be represented by few wavelet modes and that these modes are sufficient to reproduce the velocity probability density function (PDF) and the energy spectrum over the entire inertial range. The remaining incoherent background flow is homogeneous, has small amplitude, and is uncorrelated. These results are compared with those obtained for the same compression rate using large eddy simulation (LES) filtering. In contrast to the incoherent background flow of DWT, the LES subgrid scales have a much larger amplitude and are correlated, which makes their statistical modeling more difficult.