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Concentration of diffusional particles in viscous boundary sublayer of turbulent flow

机译:湍流粘性边界子层中扩散粒子的浓度

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The motion of inertial particles suspended in the viscous boundary sublayer of a wall-bounded turbulent flow is considered. We show that there is the diffusional region near the wall occupied by the particle moving in the local-equilibrium with the turbulent fluctuations which are modelled by Ornstein-Uhlenbeck process. The stationary spatial distribution of inertial particles is found for arbitrary Stokes number (dimensionless measure of the inertia). The weakly inertial particles placed in the diffusional region go away from the wall and escape the viscous sublayer. However, the direction of particle migration reverses when the Stokes number is getting larger than the critical value that we determine. The standard turbophoresis becomes more and more pronounced with the increase of Stokes number so that sufficiently inertial particles turn out to be trapped in the viscous boundary sublayer. (C) 2015 Elsevier B.V. All rights reserved.
机译:考虑了悬浮在有壁湍流的粘性边界子层中的惯性粒子的运动。我们表明,在壁附近有一个扩散区域,该粒子在局部平衡中运动,具有湍流涨落,这是通过Ornstein-Uhlenbeck过程建模的。对于任意斯托克斯数(惯性的无量纲度量),可以找到惯性粒子的静态空间分布。放置在扩散区域中的弱惯性粒子远离壁,逸出粘性子层。但是,当斯托克斯数变得大于我们确定的临界值时,粒子迁移的方向会反转。随着斯托克斯数的增加,标准涡轮电泳变得越来越明显,以至于足够的惯性粒子被困在粘性边界子层中。 (C)2015 Elsevier B.V.保留所有权利。

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