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在微磁流体力学中利用脉宽调制磁场研究微流控T型交叉点内铁磁流体微滴的分裂动力学

Splitting dynamics of ferrofluid droplets inside a microfluidic T-junction using a pulse-width modulated magnetic field in micro-magnetofluidics.

作者信息

Bijarchi Mohamad Ali, Dizani Mahdi, Honarmand Mohammadmahdi, Shafii Mohammad Behshad

机构信息

Department of Mechanical Engineering, Sharif University of Technology, Tehran, Iran.

出版信息

Soft Matter. 2021 Feb 15;17(5):1317-1329. doi: 10.1039/d0sm01764g.

DOI:10.1039/d0sm01764g
PMID:33313630
Abstract

Micro-magnetofluidics offers a promising tool for better control over the ferrofluid droplet manipulation which has been vastly utilized in biomedical applications in recent years. In this study, the ferrofluid droplet splitting under an asymmetric Pulse-Width-Modulated (PWM) magnetic field in a T-junction is numerically investigated using a finite volume method and VOF two-phase model. By utilizing the PWM magnetic field, two novel regimes of ferrofluid droplet splitting named as Flowing through the Same Branch (FSB) and Double Splitting (DS) have been observed for the first time. In the FSB regime, the daughter droplets move out of the same microchannel outlet, and in the DS regime, the droplet splitting occurs two times which results in generating three daughter droplets. The main problem related to the asymmetric droplet splitting under a steady magnetic field is daughter droplet trapping. By using a PWM magnetic field, this issue is resolved and the trapped/escaped regions are obtained in terms of the duty cycle and dimensionless magnetic field frequency. The effects of six important dimensionless parameters on the splitting ratio, including magnetic Bond number, duty cycle, dimensionless magnetic field frequency, capillary number, dimensionless mother droplet length, and dimensionless dipole position are investigated. The results showed that the splitting ratio increases with increasing magnetic Bond number or duty cycle, or decreasing the dimensionless magnetic field frequency. Eventually, a correlation is offered for the splitting ratio based on the dimensionless variables with an average relative error of 2.67%.

摘要

微磁流体力学为更好地控制铁磁流体液滴操纵提供了一种很有前景的工具,近年来该技术在生物医学应用中得到了广泛应用。在本研究中,采用有限体积法和VOF两相模型,对T型结中不对称脉宽调制(PWM)磁场作用下的铁磁流体液滴分裂进行了数值研究。通过利用PWM磁场,首次观察到了两种新型的铁磁流体液滴分裂模式,即同支流出(FSB)和双重分裂(DS)。在FSB模式下,子液滴从同一个微通道出口流出,而在DS模式下,液滴分裂发生两次,从而产生三个子液滴。与稳定磁场下不对称液滴分裂相关的主要问题是子液滴捕获。通过使用PWM磁场,解决了这个问题,并根据占空比和无量纲磁场频率获得了捕获/逸出区域。研究了六个重要的无量纲参数对分裂比的影响,包括磁邦德数、占空比、无量纲磁场频率、毛细管数、无量纲母液滴长度和无量纲偶极子位置。结果表明,分裂比随磁邦德数或占空比的增加而增加,或随无量纲磁场频率的降低而增加。最终,基于无量纲变量给出了分裂比的关联式,平均相对误差为2.67%。

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