Khan Iftekhar, Castelletto Stefania, Rosengarten Gary
Future Technologies, College of VE, RMIT University, Melbourne, VIC 3000, Australia.
School of Engineering, RMIT University, Melbourne, VIC 3000, Australia.
Micromachines (Basel). 2023 Jan 30;14(2):348. doi: 10.3390/mi14020348.
The ability to manipulate a liquid meniscus using electrowetting has many applications. In any electrowetting design, at least two electrodes are required: one forms the field to change the contact angle and the other functions as a ground electrode. The contribution of the ground electrode (GE) to the dynamics of electrowetting has not yet been thoroughly investigated. In this paper, we discovered that with a bare ground electrode, the contact angle of a sessile drop increases instead of decreases when a direct current (DC) voltage varying from zero to the threshold voltage is applied. This phenomenon is opposite to what occurs when the GE is coated with a dielectric, where the contact-angle change follows the Lippmann-Young equation above the threshold voltage of electrowetting. However, this behaviour is not observed with either a dielectric-coated electrode using direct current (DC) or a bare ground electrode using alternating current (AC) voltage electrowetting. This study explains this phenomenon with finite element simulation and theory. From previous research work, the ground electrode configuration is inconsistent. In some studies, the ground electrode is exposed to water; in other studies, the ground electrode is covered with dielectric. This study identified that an exposed ground electrode is not required in electrowetting. Moreover, this research work suggests that for applications where precise control of the contact angle is paramount, a dielectric-coated ground electrode should be used since it prevents the increase in the contact angle when increasing the applied potential from zero to the threshold voltage. This study also identified that contact angle hysteresis is lower with a Cytop-coated ground electrode and DC voltage than with a bare ground electrode using AC or DC voltages.
利用电润湿操纵液体弯月面的能力有许多应用。在任何电润湿设计中,至少需要两个电极:一个形成改变接触角的电场,另一个用作接地电极。接地电极(GE)对电润湿动力学的贡献尚未得到充分研究。在本文中,我们发现,对于裸露的接地电极,当施加从零到阈值电压变化的直流(DC)电压时,静止液滴的接触角会增大而不是减小。这种现象与接地电极涂有介电材料时的情况相反,在电润湿阈值电压以上,接触角的变化遵循 Lippmann-Young 方程。然而,无论是使用直流(DC)的介电涂层电极还是使用交流(AC)电压电润湿的裸露接地电极,都没有观察到这种行为。本研究通过有限元模拟和理论解释了这一现象。从以前的研究工作来看,接地电极的配置并不一致。在一些研究中,接地电极暴露在水中;在其他研究中,接地电极覆盖有介电材料。本研究确定在电润湿中不需要暴露的接地电极。此外,这项研究工作表明,对于接触角精确控制至关重要的应用,应使用介电涂层接地电极,因为当施加的电位从零增加到阈值电压时,它可以防止接触角增大。本研究还确定,与使用交流或直流电压的裸露接地电极相比,使用 Cytop 涂层接地电极和直流电压时接触角滞后更低。