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Lagrangian mixing in straight compound channels

机译:拉格朗日混合在直的复合通道中

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Recently Stocchino & Brocchini (J. Fluid Mech., vol. 643, 2010, p. 425 have studied the dynamics of two-dimensional (2D) large-scale vortices with vertical axis evolving in a straight compound channel under quasi-uniform flow conditions. The mixing processes associated with such vortical structures are here analysed through the results of a dedicated experimental campaign. Time-resolved Eulerian surface velocity fields, measured using a 2D particle-image velocimetry system, form the basis for a Lagrangian analysis of the dispersive processes that occur in compound channels when the controlling physical parameters, i.e. the flow depth ratio (rh) and the Froude number (Fr) are changed. Lagrangian mixing is studied by means of various approaches based either on single-particle or multiple-particle statistics (relative and absolute statistics, probability density functions (p.d.f.s) of relative displacements and finite-scale Lyapunov exponents). Absolute statistics reveal that transitional macrovortices, typical of shallow flow conditions, strongly influence the growth in time of the total absolute dispersion, after the initial ballistic regime, leading to a non-monotonic behaviour. In deep flow conditions, on the contrary, the absolute dispersion displays a monotonic growth because the generation of transitional macrovortices does not take place. In all cases an asymptotic diffusive regime is reached. Multiple-particle dynamics is controlled by rh and Fr. Different growth regimes of the relative diffusivity have been found depending on the flow conditions. This behaviour can be associated with different energy transfer processes and it is further confirmed by the p.d.f.s of relative displacements, which show a different asymptotical shape depending on the separation scales and the Froude number. Finally, an equilibrium regime is observed for all the experiments by analysing the decay of the finite-scale Lyapunov exponents with the particle separations.
机译:最近,Stocchino&Brocchini(J. Fluid Mech。,第643卷,2010,第425页)研究了在准均匀流动条件下垂直轴在直复合通道中演化的二维(2D)大尺度涡旋的动力学。通过专门实验的结果分析了与这种涡旋结构相关的混合过程,使用二维粒子图像测速系统测量的时间分辨欧拉表面速度场构成了拉格朗日分析分散过程的基础当控制物理参数(即流深比(rh)和弗洛德数(Fr))发生变化时,复合通道中会发生这种情况。基于单颗粒或多颗粒统计,通过各种方法研究了拉格朗日混合(相对和绝对统计,相对位移的概率密度函数(pdfs)和有限尺度Lyapunov指数。在初始弹道状态之后,典型的浅涡流大涡会强烈影响总绝对分散时间的增长,从而导致非单调行为。相反,在深流条件下,绝对色散显示出单调增长,因为不会发生过渡大涡旋。在所有情况下都达到渐近扩散状态。多粒子动力学受rh和Fr控制。根据流动条件,已发现相对扩散率的不同生长方式。这种现象可能与不同的能量传递过程有关,并且通过相对位移的p.d.f.s进一步证实,相对位移根据分离规模和弗洛德数显示出不同的渐近形状。最后,通过分析有限尺度Lyapunov指数随颗粒分离的衰减,可以观察到所有实验的平衡状态。

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