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Wave motion of incompressible turbulent fluid

机译:不可压缩湍流的波动

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Evolution of small disturbances in a fully developed incompressible turbulent flow is considered on the base of the transport equation for the single-point probability density function (PDF) of velocity fluctuations. It is shown that at high frequencies this equation is similar to the Vlasov equation for charged plasma in a self-consistent electromagnetic field having longitudinal wave solutions for turbulent stresses similar to Langmuir waves. It is found that the longitudinal waves of turbulent stresses have a constant phase velocity and can be damped, neutral, or growing waves, depending on the type of undisturbed probability density function of velocity fluctuations. The obtained result differs from the previously published solutions to this problem using the statistical moments closures according to which the wave disturbances should be neutral or damped. The possibilities of experimental observation of longitudinal waves of turbulent stresses are analyzed.
机译:在速度波动的单点概率密度函数(PDF)的输运方程的基础上,考虑了充分发展的不可压缩湍流中小扰动的演化。结果表明,在高频下,该方程式类似于自洽电磁场中带电等离子体的Vlasov方程式,该方程式具有类似于Langmuir波的湍流应力纵向波解。发现湍流应力的纵波具有恒定的相速度,并且可以衰减,中性或增长,这取决于速度波动的不受干扰概率密度函数的类型。所获得的结果与以前使用统计矩闭合来解决此问题的方法有所不同,根据统计矩闭合,应将波动干扰设为中性或衰减。分析了湍流纵向波实验观测的可能性。

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