介电微杆在圆极化电场中的可控电旋转行为

李艳波; 高江琦; 刘维宇; 姚博彬; 武奇生

doi:10.7652/xjtuxb202201017

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介电微杆在圆极化电场中的可控电旋转行为

更新时间：2025-05-08

- 介电微杆在圆极化电场中的可控电旋转行为
- Controllable Electrical Rotation Behavior of Dielectric Micro-Rod in a Circularly Polarized Electric Field
- 西安交通大学学报 2022年56卷第1期页码：151-157
- 作者机构：
  
  长安大学电子与控制工程学院,西安,710064
- 作者简介：
- 基金信息：
  
  : 2021-02-22。作者简介: 李艳波(1980—),男,副教授;刘维宇(通信作者),男,副教授。基金项目: 陕西省重点研发计划资助项目(2021KW-13);河南省交通运输厅科技计划资助项目(2021G10);西安市未央区科技计划资助项目(202017)
- DOI：10.7652/xjtuxb202201017
  中图分类号： TN42
- 网络首发：2022-01-10，
  
  纸质出版：2022
- 稿件说明：
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李艳波, 高江琦, 刘维宇, 等. 介电微杆在圆极化电场中的可控电旋转行为[J]. 西安交通大学学报, 2022,56(1):151-157.

LI Yanbo, GAO Jiangqi, LIU Weiyu, et al. Controllable Electrical Rotation Behavior of Dielectric Micro-Rod in a Circularly Polarized Electric Field[J]. 2022, 56(1): 151-157.
李艳波, 高江琦, 刘维宇, 等. 介电微杆在圆极化电场中的可控电旋转行为[J]. 西安交通大学学报, 2022,56(1):151-157. DOI： 10.7652/xjtuxb202201017.

LI Yanbo, GAO Jiangqi, LIU Weiyu, et al. Controllable Electrical Rotation Behavior of Dielectric Micro-Rod in a Circularly Polarized Electric Field[J]. 2022, 56(1): 151-157. DOI： 10.7652/xjtuxb202201017.

摘要

为了解决悬浮在电解质溶液中的介电杆旋转方向难以改变的问题

并实现对介电杆的灵活控制

提出了单个介电微杆在外加旋转电场作用下旋转方向可以主动调节的方法。通过建立微流控芯片模型

在四相电极阵列中心布置或去除结构化的悬浮微电极

对电解质溶液中的介电微杆的运动开展研究。实验结果表明:在没有理想的可极化金属表面的情况下

测得的与行波电场相反的电旋转角速度总是远大于考虑非均匀表面传导的Maxwell-Wager界面极化理论所预测的角速度

最大角速度可达2.9(°)/s; 在嵌入了偶极悬浮微电极的情况下

诱导出的双电层极化导致了一种新型的共场旋转模式

平均角速度从0.18(°)/s变化为-3.15(°)/s。提出的方法不仅实现了介电杆从反场到同场电动旋转行为的调节

而且大大加快了杆运动的角速度

为研究电旋转特性提供一定的参考。

Abstract

To govern the rotation direction of the dielectric rod suspended in the electrolyte solution and realize flexible control of the dielectric rod

a method for adjusting the rotation direction of a single dielectric micro-rod under the action of external rotating electric field is proposed. By establishing a model of the microfluidic chip and arranging or removing the structured suspending microelectrode in the center of the four-phase electrode array

the rotating motions of the rigid dielectric micro-rod in electrolyte are researched. Experimental results show that without the polarizable metal surface

the measured angular velocity of anti-field electrorotation can reach 2.9(°)/s

more significant than that predicted by the Maxwell-Wager theory about the polarizable surface with consideration of uneven surface conduction. It is found that in the case of embedded dipole-suspended microelectrodes

the polarization of double electric layer leads to a new co-field rotation mode. This model changes the average angular velocity from 0.18(°)/s to -3.15(°)/s. The proposed method not only adjusts the electrorotation behavior of the dielectric rod from anti-field to co-field but also greatly speeds up the angular velocity

and it may provide a general reference for the design of the rotation characteristics.

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references

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