中国物理B ›› 2022, Vol. 31 ›› Issue (3): 34703-034703.doi: 10.1088/1674-1056/ac248a

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Particle captured by a field-modulating vortex through dielectrophoresis force

Bing Yan(严兵), Bo Chen(陈波), Zerui Peng(彭泽瑞), and Yong-Liang Xiong(熊永亮)   

  1. School of Aerospace Engineering, Huazhong University of Science and Technology, Wuhan 430074, China
  • 收稿日期:2021-07-02 修回日期:2021-08-18 接受日期:2021-09-08 出版日期:2022-02-22 发布日期:2022-02-24
  • 通讯作者: Bo Chen, Zerui Peng E-mail:chbo76@hust.edu.cn;zeruipeng@hust.edu.cn
  • 基金资助:
    Project supported by the National Natural Science Foundation of China (Granmt Nos. 11572139, 11872187, and 12072125).

Particle captured by a field-modulating vortex through dielectrophoresis force

Bing Yan(严兵), Bo Chen(陈波), Zerui Peng(彭泽瑞), and Yong-Liang Xiong(熊永亮)   

  1. School of Aerospace Engineering, Huazhong University of Science and Technology, Wuhan 430074, China
  • Received:2021-07-02 Revised:2021-08-18 Accepted:2021-09-08 Online:2022-02-22 Published:2022-02-24
  • Contact: Bo Chen, Zerui Peng E-mail:chbo76@hust.edu.cn;zeruipeng@hust.edu.cn
  • Supported by:
    Project supported by the National Natural Science Foundation of China (Granmt Nos. 11572139, 11872187, and 12072125).

摘要: In microfluidic technology, dielectrophoresis (DEP) is commonly used to manipulate particles. In this work, the fluid-particle interactions in a microfluidic system are investigated numerically by a finite difference method (FDM) for electric field distribution and a lattice Boltzmann method (LBM) for the fluid flow. In this system, efficient particle manipulation may be realized by combining DEP and field-modulating vortex. The influence of the density ($\rho_{\rm p}$), radius ($r$), and initial position of the particle in the $y$ direction ($y_{\rm p0}$), and the slip velocity ($u_{0}$) on the particle manipulation are studied systematically. It is found that compared with the particle without action of DEP force, the particle subjected to a DEP force may be captured by the vortex over a wider range of parameters. In the $y$ direction, as $\rho_{\rm p}$ or $r $ increases, the particle can be captured more easily by the vortex since it is subjected to a stronger DEP force. When $u_{0}$ is low, particle is more likely to be captured due to the vortex-particle interaction. Furthermore, the flow field around the particle is analyzed to explore the underlying mechanism. The results obtained in the present study may provide theoretical support for engineering applications of field-controlled vortices to manipulate particles.

关键词: field-modulating vortex, dielectrophoresis, fluid—particle interactions

Abstract: In microfluidic technology, dielectrophoresis (DEP) is commonly used to manipulate particles. In this work, the fluid-particle interactions in a microfluidic system are investigated numerically by a finite difference method (FDM) for electric field distribution and a lattice Boltzmann method (LBM) for the fluid flow. In this system, efficient particle manipulation may be realized by combining DEP and field-modulating vortex. The influence of the density ($\rho_{\rm p}$), radius ($r$), and initial position of the particle in the $y$ direction ($y_{\rm p0}$), and the slip velocity ($u_{0}$) on the particle manipulation are studied systematically. It is found that compared with the particle without action of DEP force, the particle subjected to a DEP force may be captured by the vortex over a wider range of parameters. In the $y$ direction, as $\rho_{\rm p}$ or $r $ increases, the particle can be captured more easily by the vortex since it is subjected to a stronger DEP force. When $u_{0}$ is low, particle is more likely to be captured due to the vortex-particle interaction. Furthermore, the flow field around the particle is analyzed to explore the underlying mechanism. The results obtained in the present study may provide theoretical support for engineering applications of field-controlled vortices to manipulate particles.

Key words: field-modulating vortex, dielectrophoresis, fluid—particle interactions

中图分类号:  (Electrokinetic effects)

  • 47.57.jd
47.61.-k (Micro- and nano- scale flow phenomena) 47.15.Rq (Laminar flows in cavities, channels, ducts, and conduits)