Yamashita Hiroshi, Akinaga Takeshi, Sugihara-Seki Masako
Department of Pure and Applied Physics, Kansai University, 3-3-35 Yamate-cho, Suita, Osaka 564-8680, Japan.
Department of Systems Design Engineering, Akita University, 1-1 Tegatagakuen-Machi, Akita 010-8502, Japan.
Micromachines (Basel). 2021 Oct 14;12(10):1242. doi: 10.3390/mi12101242.
The continuous separation and filtration of particles immersed in fluid flows are important interests in various applications. Although the inertial focusing of particles suspended in a duct flow is promising in microfluidics, predicting the focusing positions depending on the parameters, such as the shape of the duct cross-section and the Reynolds number (Re) has not been achieved owing to the diversity of the inertial-focusing phenomena. In this study, we aimed to elucidate the variation of the inertial focusing depending on Re in rectangular duct flows. We performed a numerical simulation of the lift force exerted on a spherical particle flowing in a rectangular duct and determined the lift-force map within the duct cross-section over a wide range of Re. We estimated the particle trajectories based on the lift map and Stokes drag, and identified the particle-focusing points appeared in the cross-section. For an aspect ratio of the duct cross-section of 2, we found that the blockage ratio changes transition structure of particle focusing. For blockage ratios smaller than 0.3, particles focus near the centres of the long sides of the cross-section at low Re and near the centres of both the long and short sides at relatively higher Re. This transition is expressed as a subcritical pitchfork bifurcation. For blockage ratio larger than 0.3, another focusing pattern appears between these two focusing regimes, where particles are focused on the centres of the long sides and at intermediate positions near the corners. Thus, there are three regimes; the transition between adjacent regimes at lower Re is found to be expressed as a saddle-node bifurcation and the other transition as a supercritical pitchfork bifurcation.
对沉浸在流体流中的颗粒进行连续分离和过滤是各种应用中的重要研究方向。尽管在微流体中,管道流中悬浮颗粒的惯性聚焦很有前景,但由于惯性聚焦现象的多样性,尚未实现根据诸如管道横截面形状和雷诺数(Re)等参数来预测聚焦位置。在本研究中,我们旨在阐明矩形管道流中惯性聚焦随雷诺数的变化情况。我们对在矩形管道中流动的球形颗粒上施加的升力进行了数值模拟,并在很宽的雷诺数范围内确定了管道横截面上的升力图。我们基于升力图和斯托克斯阻力估算了颗粒轨迹,并确定了横截面上出现的颗粒聚焦点。对于管道横截面的纵横比为2的情况,我们发现阻塞率会改变颗粒聚焦的转变结构。对于小于0.3的阻塞率,颗粒在低雷诺数下聚焦在横截面长边的中心附近,在相对较高的雷诺数下聚焦在长边和短边的中心附近。这种转变表现为亚临界叉形分岔。对于大于0.3的阻塞率,在这两种聚焦状态之间会出现另一种聚焦模式,即颗粒聚焦在长边的中心和靠近角落的中间位置。因此,存在三种状态;发现在较低雷诺数下相邻状态之间的转变表现为鞍结分岔,而另一种转变表现为超临界叉形分岔。