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Turbulence models for cfd in the 21st century

机译:21世纪CFD的湍流模型

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The two approaches to turbulence modelling Both Osborne Reynolds (1884) and Ludwig Prandtl (1925) regarded turbulence as an expression of the near-random intermingling of sizeable fragments of unlike fluid, which, during a succession of brief encounters, bended to equilibrium. Their concept found however no explicit place in the family of turbulence models springing from Kolmogorov's (1942) proposal to attend only to statistical measures of the turbulent motion, such as energy and frequency. The intermingling-fragments idea was nevertheless preserved in the models of Spalding (1971) and Magnussen (1976) ("eddy-break-up" and "eddy-dissipation", respectively) which are still used for combustion simulation.
机译:湍流模拟奥斯本雷诺(1884)和Ludwig Prandtl(1925)的两种方法被认为是湍流,作为与液体不同的相当碎片的近似随机混合的表达,这在连续的短暂遇到期间弯曲到平衡。他们的概念发现,湍流模型中没有明确的地方,从Kolmogorov(1942)的建议中,只参加湍流运动的统计测量,例如能量和频率。然而,混合碎片的想法是保存在Spalding(1971)和Magnussen(1976)的模型中(“涡旋 - 分手”和“涡流”),分别仍然用于燃烧模拟。

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