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Small internal waves in sheared flows: lower bound for the vorticity transient growth and propagation bound in the parameter space

机译:剪切流中的小内波:涡度的下限   在参数空间中的瞬态增长和传播

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摘要

We show that transient kinetic energy growth of small traveling waves insideincompressible viscous wall flows is not a sufficient condition for theirenstrophy (the size of vorticity) growth. Historically, mathematicaldifficulties related to the wall vorticity boundary conditions left thevorticity perturbation problem open. In the last decades of the 20th century,the discovery of the transient perturbation growth and its link to thesubcritical transition to turbulence was still treated by means of energy-basedanalysis. By using the non-modal approach, we extend the work of J. L. Synge(1930s) which was an alternative way to attack the flow stability problem basedon the flow vorticity analysis instead of the classical kinetic energyanalysis. Our calculations leads to the lower bound for the algebraic enstrophygrowth as a function of the perturbation wavelength. This highlights how theenstrophy monotonic decay region inside the wavenumber - Reynolds number (Re)map is wider than that of the kinetic energy. By taking the general point ofview of internal wave propagation in a medium, we present and discuss thedispersion variability inside the stability map. By keeping fixed the flowcontrol parameter, we observe that this variability implies that inside ageneral wave packet, there will be a subset of waves that disperse aside asubset of waves that do not. In association to a situation where wave packetsundergo powerful and long-lasting transient growth, this information is key tothe understanding of a potential process of nonlinear coupling onset.
机译:我们表明,不可压缩的粘性壁流内部小的行波的瞬态动能增长并不是其涡旋(涡度的大小)增长的充分条件。从历史上看,与壁涡旋边界条件有关的数学难题使涡旋扰动问题悬而未决。在20世纪的最后几十年中,瞬态扰动增长的发现及其与从亚临界过渡到湍流的联系仍通过基于能量的分析加以处理。通过使用非模态方法,我们扩展了J. L. Synge(1930s)的工作,这是一种基于流动涡度分析而不是经典的动能分析的解决流动稳定性问题的替代方法。我们的计算导致了代数熵增长的下界随扰动波长的变化。这突出显示了波数-雷诺数(Re)映射内的涡旋单调衰减区域比动能宽。通过从内部波在介质中传播的一般角度出发,我们介绍并讨论了稳定性图内部的色散变化性。通过保持固定的流量控制参数,我们观察到这种可变性意味着在一般的波包内部,将会有一部分波子散开,而另一部分波子则没有散开。与波包经历强大而持久的瞬态增长的情况相关,此信息对于理解非线性耦合发作的潜在过程至关重要。

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