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Lagrangian statistics across the turbulent-nonturbulent interface in a turbulent plane jet

机译:湍流平面射流中湍流-非湍流界面的拉格朗日统计

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Lagrangian statistics from millions of particles are used to study the turbulent entrainment mechanismnin a direct numerical simulation of a turbulent plane jet at Reλ ≈ 110. The particles (tracers) are initiallynseeded at the irrotational region of the jet near the turbulent shear layer and are followed as they arendrawn into the turbulent region across the turbulent-nonturbulent interface (TNTI), allowing the study ofnthe enstrophy buildup and thereby characterizing the turbulent entrainment mechanism in the jet. Thenuse of Lagrangian statistics following fluid particles gives a more correct description of the entrainmentnmechanism than in previous works since the statistics in relation to the TNTI position involve data fromnthe trajectories of the entraining fluid particles. The Lagrangian statistics for the particles show the existencenof a velocity jump and a characteristic vorticity jump (with a thickness which is one order of magnitudengreater than the Kolmogorov microscale), in agreement with previous results using Eulerian statistics. Thenparticles initially acquire enstrophy by viscous diffusion and later by enstrophy production, which becomesn“active” only deep inside the turbulent region. Both enstrophy diffusion and production near the TNTIndiffer substantially from inside the turbulent region. Only about 1% of all particles find their way intonpockets of irrotational flow engulfed into the turbulent shear layer region, indicating that “engulfment”nis not significant for the present flow, indirectly suggesting that the entrainment is largely due to “nibbling”nsmall-scale mechanisms acting along the entire TNTI surface. Probability density functions of particle positionsnsuggests that the particles spend more time crossing the region near the TNTI than traveling inside the turbulentnregion, consistent with the particles moving tangent to the interface around the time they cross it.
机译:在直接对Reλ≈110处的湍流平面射流进行数值模拟时,使用了来自数百万个粒子的拉格朗日统计量来研究湍流夹带机制。最初将粒子(示踪物)接种在湍流剪切层附近的射流的非旋动区域,然后进行跟踪当它们穿过湍流-非湍流界面(TNTI)进入湍流区域时,可以研究涡旋集聚,从而表征射流中的湍流夹带机制。然后,与先前的工作相比,在流体粒子之后使用拉格朗日统计量能更准确地描述夹带机制,因为与TNTI位置有关的统计量涉及来自夹带流体粒子轨迹的数据。粒子的拉格朗日统计表明存在速度跳跃和特征涡旋跳跃(厚度比Kolmogorov微米级大一个数量级),与先前使用欧拉统计的结果一致。然后,粒子首先通过粘性扩散获得回旋力,然后通过产生回旋力,仅在湍流区域的深处才变得“活跃”。涡流的扩散和产生都在TNTIndiffer附近,基本上是从湍流区域内部产生的。所有颗粒中只有约1%会发现无节流进入湍流剪切层区域,这表明“吞噬”对于当前的流动并不重要,这间接表明夹带主要是由于“吞噬”了小规模的沿整个TNTI表面起作用的机制。粒子位置的概率密度函数表明,粒子穿过TNTI附近区域的时间比在湍流区域内移动的时间更长,这与粒子在穿过该区域时切线移动到界面的方向相符。

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  • 来源
    《PHYSICAL REVIEW E》 |2013年第4期|1-12|共12页
  • 作者单位

    IDMEC/Instituto Superior T´ecnico Technical University of Lisbon Pav. Mecˆanica I 1o andar/esq./LASEFAv. Rovisco Pais 1049-001 Lisboa Portugal;

    IDMEC/Instituto Superior T´ecnico Technical University of Lisbon Pav. Mecˆanica I 1o andar/esq./LASEFAv. Rovisco Pais 1049-001 Lisboa Portugal;

    IDMEC/Instituto Superior T´ecnico Technical University of Lisbon Pav. Mecˆanica I 1o andar/esq./LASEFAv. Rovisco Pais 1049-001 Lisboa Portugal;

    IDMEC/Instituto Superior T´ecnico Technical University of Lisbon Pav. Mecˆanica I 1o andar/esq./LASEFAv. Rovisco Pais 1049-001 Lisboa Portugal;

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