• 제목/요약/키워드: Turbulent Normal Stress

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Development and validation of a non-linear k-ε model for flow over a full-scale building

  • Wright, N.G.;Easom, G.J.;Hoxey, R.J.
    • Wind and Structures
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    • 제4권3호
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    • pp.177-196
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    • 2001
  • At present the most popular turbulence models used for engineering solutions to flow problems are the $k-{\varepsilon}$ and Reynolds stress models. The shortcoming of these models based on the isotropic eddy viscosity concept and Reynolds averaging in flow fields of the type found in the field of Wind Engineering are well documented. In view of these shortcomings this paper presents the implementation of a non-linear model and its evaluation for flow around a building. Tests were undertaken using the classical bluff body shape, a surface mounted cube, with orientations both normal and skewed at $45^{\circ}$ to the incident wind. Full-scale investigations have been undertaken at the Silsoe Research Institute with a 6 m surface mounted cube and a fetch of roughness height equal to 0.01 m. All tests were originally undertaken for a number of turbulence models including the standard, RNG and MMK $k-{\varepsilon}$ models and the differential stress model. The sensitivity of the CFD results to a number of solver parameters was tested. The accuracy of the turbulence model used was deduced by comparison to the full-scale predicted roof and wake recirculation zone lengths. Mean values of the predicted pressure coefficients were used to further validate the turbulence models. Preliminary comparisons have also been made with available published experimental and large eddy simulation data. Initial investigations suggested that a suitable turbulence model should be able to model the anisotropy of turbulent flow such as the Reynolds stress model whilst maintaining the ease of use and computational stability of the two equations models. Therefore development work concentrated on non-linear quadratic and cubic expansions of the Boussinesq eddy viscosity assumption. Comparisons of these with models based on an isotropic assumption are presented along with comparisons with measured data.

청평호 및 팔당호 어류군집 비교 연구 (The Comparative Study on the Fish Community in Lake Chungpyung and Lake Paldang)

  • 박혜경;이장호;윤석환;최명재
    • 한국물환경학회지
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    • 제29권1호
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    • pp.7-18
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    • 2013
  • We compared the structure of fish community and condition of major fish species in Lake Chungpyung and Lake Paldang, which are relatively shallow, meso-eutrophic, cascading dam reservoirs on the North Han River. Two lakes have wide littoral zone in the lakeside providing similarly good habitat for fishes, whereas fishery and water recreational activities such as motorboating, water skiing are allowed in Lake Chungpyung but are prohibited in Lake Paldang. The average lengths of large size fishes in Lake Chungpyung are shorter than those of same species in Lake Paldang, resulting in the slight distortion of generation distribution of those species in Lake Chungpyung, possibly owing to the active fishery such as fixed shore net fishing, gill net fishing and angling. Meanwhile the condition of fishes represented by the length-weight relationship of fish species did not show the significant differences between two lakes and showed normal condition. To evaluate the impact of physical disturbance such as loud noise and turbulent wave from water recreational activities to fishes precisely, further studies including physiological responses to stress an spawing activity should be needed.

쇄파대(碎波帶) 밖에서 return flow의 수학적(數學的) 모형(模型) (A Mathematical Model of Return Flow outside the Surf Zone)

  • 이종섭;박일흠
    • 대한토목학회논문집
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    • 제14권2호
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    • pp.355-365
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    • 1994
  • 쇄파대(碎波帶) 밖에서 return flow에 관한 해석적(解釋的) 모형(模型)을 제시(提示)하였다. Navier-Stokes 방정식(方程式)과 연속방정식(連續方程式)으로부터 기초방정식(基礎方程式)이 유도(誘導)되었으며, 기초방정식(基礎方程式)의 각 항(項)은 ordering 해석방법(解釋方法)으로 상대적(相對的)인 크기가 평가(評價)되었다. 이에 따라 미소항(微小項)인 난류법선응력항(亂流法線應力項), 연직방향(鉛直方向) 수립자속도(水粒子速度) 제곱항(項) 및 streaming velocity 항(項)이 무시(無視)될 수 있었다. return flow의 기동력(起動力)이 되는 파동성분(波動成分)의 각 항(項)은 선형파이론(線形波理論)을 천해파근사(淺海波近似)하여 산정(算定)하였으며, 특히 파고(波高)의 공간적(空間的) 변화율(變化率)은 천수계수(淺水係數)를 고려(考慮)하여 나타내었다. 그리고 와동점성계수(渦動粘性係數)의 연직분포(鉛直分布)는 기존(旣存)의 상수형(常數型), 선형함수형(線形函數型) 그리고 자연지수함수형(自然指數函數型)의 3가지 형태(形態)에 대하여 검토(檢討)하였으며, 해(解)의 정도(精度)에 민감(敏感)한 영향(影響)을 미치는 와동점성계수(渦動粘性係數)의 절대(絶對)값은 파곡점(波谷點)에서 유속(流速)이 zero라는 새로운 경계조건(境界條件)을 도입(導入)하여 일의적(一義的)으로 결정(決定)하였다. 2계(階) 미분방정식(微分方程式)으로 나타나는 기초방정식(基礎方程式)의 해(解)를 구하기 위하여 저면(底面)에서 경계조건(境界條件) 및 연속조건(連續條件)을 사용(使用)하였다. 여러 가지 수리실험자료(水理實驗資料)와 본(本) 모형(模型)의 해(解)를 비교(比較)한 결과(結果), 와동점성계수(渦動粘性係數)의 연직분포(鉛直分布)를 상수형(常數型) 혹은 자연지수함수형(自然指數函數型)으로 가정(假定)하였을 때 좋은 결과(結果)를 나타내었다.

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