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Clustering and preferential concentration of finite-size particles in forced homogeneous-isotropic turbulence

机译:有限尺寸粒子的聚类和优先浓度   强制均匀 - 各向同性湍流

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摘要

We have performed interface-resolved direct numerical simulations of forcedhomogeneous-isotropic turbulence in a dilute suspension of spherical particlesin the Reynolds number range Re-lambda=115-140. The solid-fluid density ratiowas set to 1.5, gravity was set to zero, and two particle diameters wereinvestigated corresponding to approximately 5 and 11 Kolmogorov lengths. Notethat these particle sizes are clearly outside the range of validity of thepoint-particle approximation, as has been shown by Homann & Bec (2010). At thepresent parameter points the global effect of the particles upon the fluid flowis weak. We observe that the dispersed phase exhibits clustering with moderateintensity. The tendency to cluster, which was quantified in terms of thestandard deviation of Voronoi cell volumes, decreases with the particlediameter. We have analyzed the relation between particle locations and thelocation of intense vortical flow structures. The results do not reveal anysignificant statistical correlation. Contrarily, we have detected a small butstatistically significant preferential location of particles with respect tothe `sticky points' proposed by Goto & Vassilicos (2008), i.e. points where thefluid acceleration field is acting such as to increase the local particleconcentration in one-way coupled point-particle models under Stokes drag. Thepresently found statistical correlation between the `sticky points' and theparticle locations further increases when focusing on regions with high localconcentration. Our results suggest that small finite-size particles can bebrought together along the expansive directions of the fluid accelerationfield, as previously observed only for the simplest model for sub-Kolmogorovparticles. We further discuss the effect of density ratio and collectiveparticle motion upon the basic Eulerian and Lagrangian statistics.
机译:我们已经在Reynolds数范围Re-lambda = 115-140范围内的球形颗粒稀悬浮液中进行了强迫同质各向同性湍流的界面解析直接数值模拟。固-液密度比设定为1.5,重力设定为零,并且研究了对应于大约5和11Kolmogorov长度的两个粒径。请注意,正如Homann&Bec(2010)所表明的那样,这些粒径明显超出了点-粒子近似的有效性范围。在目前的参数点上,颗粒对流体流动的整体作用微弱。我们观察到分散相表现出中等强度的聚集。用Voronoi细胞体积的标准偏差来量化的聚集趋势随颗粒直径而减小。我们分析了粒子位置与强涡流结构位置之间的关系。结果没有显示任何显着的统计相关性。相反,相对于Goto&Vassilicos(2008)提出的“粘性点”,我们检测到了一个小的但统计上显着的优先位置,即流体加速场所起作用的点,例如,增加了单向耦合点中的局部粒子浓度。 -Stokes拖动下的粒子模型。目前发现,当关注具有高局部浓度的区域时,“粘性点”与颗粒位置之间的统计相关性进一步增加。我们的研究结果表明,可以沿流体加速场的扩展方向将有限尺寸的小颗粒聚集在一起,如先前仅针对最简单的亚Kolmogorov颗粒模型所观察到的那样。我们进一步讨论密度比和集体粒子运动对基本欧拉和拉格朗日统计的影响。

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