• Title/Summary/Keyword: 와점성

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Rheological Properities of Soybean Oil Ester of the Oil and Their Mixtures with Diesel Fuel and Additives (대두유(大豆油)를 원료(原料)로 한 대체(代替) 디이젤연료(燃料)의 점성학적(粘性学的) 성질(性質))

  • Suh, Sang Ryong;Harris, F.D.
    • Journal of Biosystems Engineering
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    • v.9 no.2
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    • pp.58-64
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    • 1984
  • 디이젤엔진의 대체연료(代替燃料)로서 대두유(大豆油)는 대두유(大豆油)의 높은 점성(粘性)에 기인(起因)하는 문제점이 지적되고 있다. 이외 해결방법으로 대두유(大豆油)와 디이젤유(油)의 혼합(混合), 대두유(大豆油)의 에스테르화(化) 그리고 디이젤유(油) 첨가제(添加劑)의 첨가(添加) 등이 제시되고 있다. 본(本) 연구(硏究)는, 대두유(大豆油), 그의 에틸 에스테르 그리고 이러한 대체연료(代替燃料)의 디이젤유(油)와 혼합물(混合物) 또는 그 혼합물(混合物)의 첨가제(添加劑)와의 혼합물(混合物)의 점성학적 성질(性質)과 그 크기를 실험적 방법(方法)으로 구하였다. 그 결과 상기의 액체는 모두 뉴톤니안 액체이고, 첨가제(添加劑)는 상기 혼합물(混合物)의 점성(粘性)을 낮추는데 별로 효과가 없는 것으로 판단되었다.

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A Study on Fluid Flow of Various Viscosities in Coronary Artery (관상동맥 분지관에서 점도에 따른 유체의 유동현상 연구)

  • An, Gi-Yeong;Lee, Hyeon-Seop
    • Proceeding of EDISON Challenge
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    • 2013.04a
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    • pp.403-408
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    • 2013
  • 본 논문은 EDISON_CFD를 이용하여 관상동맥 분지관에서 점도에 따른 유체의 유동현상에 관하여 연구를 하였다. 뉴턴유체인 물의 점성계수 일때와 비뉴턴유체인 혈액의 Carreau model에서의 영전단율 점성계수(${\eta}_0$)와 무한전단율 점성계수(${\eta}_{\infty}$)일 때의 유동현상을 살펴보았다. 그 결과 점도가 증가할수록 재순환 영역에서 유체의 속도가 감소하였고 CF 및 CP값이 감소하는 구간의 수가 증가하여 벽면의 저전단응력으로 인해 생기는 재순환영역의 수가 증가하는 것으로 나타났다.

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Lateral Eddy Viscosity for Open-Channel Flows through Emergent Vegetation (정수식생 개수로 흐름에서 횡방향 와점성 계수)

  • Lee, Jin-Hwi;Choi, Sung-Uk
    • Proceedings of the Korea Water Resources Association Conference
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    • 2012.05a
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    • pp.74-78
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    • 2012
  • 본 연구는 하천에서 식생에 의한 흐름구조 변화가 오염물질 이동에 미치는 영향을 알아보기 위해 흐름방향 확산계수를 산정하였다. 정수식생 조건에서 횡방향 수심적분된 와점성계수는 비식생 조건에서의 와점성계수와 다르게 적용되어야 하며 이를 위해 유량 횡분배법을 Jordanova and James (2003) 실험에 적용하였다. 제시된 실험조건을 잘 재현하는 와점성계수의 값을 역산하였으며, 이에 관한 산술평균 값을 향후 수리모형의 적용을 위해 정수식생 조건에서의 무차원 와점성계수로 제안하였다. 결정된 무차원 와점성계수를 이용하여 부분식생 개수로 흐름에서 흐름방향 확산계수를 산정하여 오염물질의 이동에 대한 특성을 분석하였다.

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Densities, Viscosities and Excess Properties of 2-Bromopropane - Methanol Binary Mixtures at Temperature from (298.15 to 318.15) K (298.15~318.15 K 에서 2-브로모프로판-메탄올 이성분 혼합물의 밀도, 점성도, 여분 성질)

  • Li, Hua;Zhang, Zhen;Zhao, Lei
    • Journal of the Korean Chemical Society
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    • v.54 no.1
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    • pp.71-76
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    • 2010
  • The densities and viscosities of 2-bromopropane-methanol binary mixtures had been determined using an digital vibrating U-tube densimeter and Ubbelohde capillary viscometer respectively from (298.15 to 318.15) K. The dependence of densities and viscosities on temperature and concentration had been correlated. The excess molar volume and the excess viscosity of the binary system were calculated from the experimental density and viscosity data. The excess molar volumes were related to compositions by polynomial regression and regression parameters and total RMSD deviations were obtained; the excess viscosities was related to compositions by Redlich-Kister equation and regression coefficients and total RMSD deviation of the excess viscosity for 2-bromopropane and methanol binary system were obtained. The results showed that the model agreed very well with the experimental data.

A Numerical Analysis of Flow through Open Channel Constrictions using Turbulence Model (난류모델을 이용한 개수로 급축소부 흐름의 수치해석)

  • Choe, Heung-Sik
    • Journal of Korea Water Resources Association
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    • v.30 no.3
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    • pp.201-210
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    • 1997
  • To analyze the flow through open-channel constrictions using $\kappa$-$\varepsilon$ turbulence mode, a numerical model is developed. The simulated results agree well with existing experimental data which attributes to the adequate input of turbulent eddy-viscosity by turbulence model. A stream function and velocity distributions enable the analysis of flow characteristics at the downstream of constriction. Turbulent eddy viscosities over channel are spatially varied with stream pattern. For the evaluation of rapidly varied flow, the eddy-viscosity input by turbulence model is required instead of the empirical effective viscosity to solve a shallow water equation.

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INFLUENCE OF EDDY VISCOSITY COEFFICIENT ON ${\kappa}-{\varepsilon}$ TURBULENCE MODEL FOR SUPERSONIC BASE FLOW (초음속 기저부 유동에서 ${\kappa}-{\varepsilon}$ 난류 모델에 대한 와점성 계수의 영향)

  • Park, Soo-Hyung;Sa, Jeong-Hwan;Kim, Jee-Woong;Kwon, Jang-Hyuk;Kim, Chang-Joo
    • Journal of computational fluids engineering
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    • v.13 no.3
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    • pp.1-7
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    • 2008
  • A supersonic base flow is computed to investigate the effect of the eddy viscosity coefficient to the linear ${\kappa}-{\varepsilon}$ turbulence models. Slight modifications to the eddy viscosity coefficient, which are based on the realizability condition, are given to the Launder-Sharma turbulence model so that present models satisfy the realizability condition. Numerical results for supersonic base flow show that turbulence models with the weaky-nonlinear eddy viscosity coefficient can lead to reasonable enhancements in the prediction of the velocity and turbulent kinetic energy profiles.

Three Dimensional Analysis of Piled Abutment Adjacent to Surcharge Loads (3차원해석에 의한 교대말뚝기초의 측방유동 발생메카니즘 분석)

  • 서동희;서정주;장범수;정상섬
    • Journal of the Korean Geotechnical Society
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    • v.17 no.2
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    • pp.85-93
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    • 2001
  • 본 논문에서는 연약지반에 시공된 교대말뚝기초에 인접하여 성토하중이 재하될 때 발생하는 측방유동의 발생메커니즘을 규명하기 위해 3차원 유한요소해석을 수행하였다. 본 수치해석에서는 점성토 지반과 점성토-사질토 지반 그리고 사질토-점성토 지반에 선단지지된 강관말뚝에 대하여 성토하중 크기(q=20, 75, 100kPa)와 말뚝두부조건(변위구송, 회전구속) 그리고 말뚝중심간격(s=2.5d, 5.0d, 7.0d, 단독말뚝)에 따라 측방유동압의 분포형태와 크기를 분석하였다. 그 결과 측방유동압의 분포형태는 교대말뚝기초의 수평변위와 유사한 형태로 나타났으며 측방유동압의 크기는 배면 성토하중의 크기에 대한 비로써 결정할 수 있었다. 그리고 점성토 지반과 점성토-사질토 지반의 경우, 측방유동압의 분포형태와 크기는 말뚝두부조건에 가장 큰 영향을 받는 반면 사질토-점성토 지반의 경우에는 말뚝두부조건보다는 토층조건에 가장 큰 영향을 받는 것으로 분석되었다. 본 연구결과를 토대로 연약지반에 시공된 교대말뚝기초의 측방유동에 대한 설계 및 해석시 지침자료로서 측방유동압의 분포형태와 크기를 추천.제안한다.

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Evaluation of Parameters in Hydrodynamic Model (동수역학모형의 매개변수 산정)

  • Yun, Tae-Hun;Lee, Jong-Uk;Jagal, Sun-Dong
    • Journal of Korea Water Resources Association
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    • v.33 no.1
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    • pp.39-50
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    • 2000
  • Generally speaking, a hydrodynamic model needs a friction coefficient (Manning coefficient or Chezy coefficient) and eddy viscosity. For numerical solution the coefficients are usually determined by recursive calculations. The eddy viscosity in numerical model plays physical diffusion in flow and also acts as numerical viscosity. Hence its value has influence on the stability of numerical solution and for these reasons a consistent evaluation procedure is needed. By using records of stage and discharge in the downstream reach of the Han river, I-D models (HEC-2 and NETWORK) and 2-D model (SMS), estimated values of Manning coefficient and an empirical equation for eddy viscosity are presented. The computed results are verified through the recorded flow elevation data.n data.

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Viscosity of Helium Calculated by Using the Brake Theory of Viscosity (Brake 점성 이론으로 계산한 헬륨의 점성도)

  • Won-Soo Kim;Jin-Young Kim;Tong-Seek Chair
    • Journal of the Korean Chemical Society
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    • v.36 no.3
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    • pp.376-382
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    • 1992
  • Liquid helium is an exciting subject for the study of thermodynamic and transport properties because of its remarkable properties. The viscosity of liquid helium exhibits the abnormal behavior compared to other ordinary liquid. Below the $\lambda$ point liquid $^4He$ becomes superfluid, and it is obviously quite a different phenomenon from the change of liquid $^3He$. The brake theory of viscosity proposed by authors is successfully applied to liquid $^3He$, liquid $^4He$, dense gas and 4He with adjustable parameter $V_s$. The calculation results are satisfactory compared with the observed values.

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One-Dimensional Model for Flow Resistance of Floodplain Vegetation in Compound Open-Channel Flow (복단면 개수로흐름에서 홍수터 식생의 흐름저항을 반영한 1차원 모형)

  • Park, Moon-Hyeong
    • Journal of Korea Water Resources Association
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    • v.43 no.6
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    • pp.517-524
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    • 2010
  • In this study, the 1D apparent shear stress model for vegetated compound open-channel flows was suggested. To consider the effect of momentum exchange between main channel and floodplain, the eddy viscosity concept was used in the present model. The interfacial eddy viscosity in the interface of main channel and floodplain was determined from the 3D Reynolds stress model. The evaluated interfacial eddy viscosity appears to be good agreement with those proposed previously. To investigate the effect of interfacial eddy viscosity, sensitive analysis was carried out. the computed backwater profiles are nearly identical with respect to the value of the interfacial eddy viscosity. However, the discharge conveyed by the floodplain changes is proportional to the interfacial eddy viscosity. Finally, the changes of the interfacial eddy viscosity due to the vegetation density and vegetation height were examined. The computed results of interfacial eddy viscosity are in proportion to the vegetation density and vegetation height, and the interfacial eddy viscosity has a range of $(2-5)\;{\times}\;10^{-4}$.