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首页> 外文期刊>Journal of Applied Mechanics >RAYLEIGH-TAYLOR INSTABILITY OF A CYLINDRICAL INTERFACE BETWEEN TWO INVISCID FLUIDS
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RAYLEIGH-TAYLOR INSTABILITY OF A CYLINDRICAL INTERFACE BETWEEN TWO INVISCID FLUIDS

机译:两种无粘性流体之间的圆柱界面的Rayleigh-Taylor不稳定性

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A theoretical analysis for the instability of a fluid film around a cylinder in an immiscible fluid is presented. A general dispersion equation, relating wave number to Department al Mining and growth rate, is derived with consideration of the effects of the cylindrical interface and a finite film thickness. Application of the dispersion equation to the breakup of a liquid film around a cylindrical body in still air leads to a prediction of the dominant wavelength by lambda = 2 pi root 2/root(1/R(2) + rho(1)g/q), where R is the radius of the cylinder, rho(1) is the density of the liquid, g is the acceleration due to gravity, sigma is the surface tension. Experiments showed good agreement with the present analysis. The dominant wavelength decreases with a decrease in the radius of the cylindrical body. A previous report on the breakup of a liquid film around a horizontal cylindrical body is shown to be error. [References: 12]
机译:提出了在不互溶的流体中圆柱体周围的流体膜的不稳定性的理论分析。考虑到圆柱界面和有限膜厚的影响,得出了一个一般的色散方程,将波数与部门采矿和增长率联系起来。将色散方程应用于静止空气中圆柱体周围液膜的破裂,可通过λ= 2 pi root 2 / root(1 / R(2)+ rho(1)g /预测主波长q),其中R是圆柱体的半径,rho(1)是液体的密度,g是在重力作用下的加速度,sigma是表面张力。实验表明与目前的分析吻合良好。主波长随着圆柱体半径的减小而减小。先前关于水平圆柱体周围液膜破裂的报告显示是错误的。 [参考:12]

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