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首页> 外文期刊>Journal of Fluid Mechanics >Particle dispersion induced by vortical interactions in a particle-laden upward jet with a partial crossflow
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Particle dispersion induced by vortical interactions in a particle-laden upward jet with a partial crossflow

机译:通过颗粒上向上喷射的血管相互作用引起的颗粒分散液,其中偏横向流动

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摘要

In the present study particle dispersions (concentrations) through vortical interactions are experimentally investigated for a particle-laden upward jet, with a horizontal crossflow covering a vertical range partially near the jet exit (Reynolds numbers of 1170-5200). We focus on the influences of the dynamics of counter-rotating vortex pairs existing in the flow on changes in the particle dispersion patterns, depending on the velocity (jet/crossflow) ratio and particle Stokes number (St = 0.01-27.42). Without crossflow, there is no dominant vortical structure along the horizontal direction; thus, the particles are not dispersed significantly out of the jet core in most cases, except for the case with the highest particle inertia (i.e. St). With crossflow, on the other hand, counter-rotating vortex pairs appear above the jet exit and become stronger as the velocity ratio decreases. With a lower velocity ratio, the vortices are tilted more toward the leeward side and dissipate faster. Driven by the vortex pairs, the drag force acting on the particles becomes stronger and, thus, particles with St < 1.0 are dragged out of the jet core following the rotation of the vortices. Those with St similar or equal to 1.0 are concentrated between the vortex pairs before the vortices collapse. When St 1.0, particles are simply transported by the inertial effect. Finally, we suggest different regimes for particle dispersion (concentration) as classified by the Stokes number and velocity ratio, and elucidate their mechanisms, which are further extended to empirical particle dispersion models.
机译:在本研究中,通过涡流相互作用对含颗粒向上射流的颗粒分散(浓度)进行了实验研究,水平横流覆盖了部分靠近射流出口的垂直范围(雷诺数为1170-5200)。我们重点研究了流动中存在的反向旋转涡对的动力学对粒子分散模式变化的影响,这取决于速度(射流/横流)比和粒子斯托克斯数(St=0.01-27.42)。没有横流,水平方向上没有主导涡结构;因此,在大多数情况下,颗粒不会明显分散在射流核心之外,但具有最高颗粒惯性(即St)的情况除外。另一方面,在横流情况下,射流出口上方出现反向旋转涡对,并随着速度比的减小而变得更强。速度比越低,漩涡越倾向背风面,消散速度越快。在涡对的驱动下,作用在颗粒上的阻力变得更强,因此,St<1.0的颗粒随着涡的旋转被拖出射流核心。St接近或等于1.0的涡在涡崩溃之前集中在涡对之间。当St1.0时,粒子仅通过惯性效应传输。最后,我们提出了按斯托克斯数和速度比分类的颗粒分散(浓度)的不同机制,并阐明了它们的机制,这些机制进一步扩展到了经验颗粒分散模型。

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