Materials and Energy Research Center, P.O. Box 14155-4777, Tehran, Iran.
J Phys Chem B. 2013 Feb 14;117(6):1660-3. doi: 10.1021/jp3054235. Epub 2012 Nov 27.
In the present study, electrophoretic deposition (EPD) of TiO(2) nanoparticles under the application of symmetric AC fields was investigated. In the first step, EPD of TiO(2) nanoparticles under a DC field at 50 V resulted in the particles' deposition on one electrode, consistent with conventional EPD principles. However, no deposits were formed on any of the electrode surfaces for symmetric sinusoidal waves at 1 Hz. In this case, enhancing the electric field strength through the application of higher potentials was considered to extend the electric field affected zone (EFAZ) in front of the electrode, increasing the particles' opportunity to deposit. A kinetic model was then derived based on the Hamaker approach to calculate the deposited mass under an AC electric field. Although this model was found to be in agreement with experimental results at 1 Hz above 200 V, some deviation was detected at lower voltages. This trend shows that there is a threshold field strength below which EFAZ is not wide enough to let particles deposit under an AC electric field.
在本研究中,考察了对称交流场下 TiO(2)纳米粒子的电泳沉积(EPD)。在第一步中,在 50 V 的直流场下进行 TiO(2)纳米粒子的 EPD,导致粒子沉积在一个电极上,这符合传统的 EPD 原理。然而,对于 1 Hz 的对称正弦波,在任何电极表面都没有形成沉积物。在这种情况下,通过施加更高的电势来增强电场强度被认为可以扩展电极前方的电场影响区(EFAZ),增加粒子沉积的机会。然后基于 Hamaker 方法推导出一个动力学模型,用于计算交流电场下的沉积质量。尽管该模型在 200 V 以上 1 Hz 的情况下与实验结果一致,但在较低电压下检测到一些偏差。这种趋势表明,存在一个阈值场强,低于该场强,EFAZ 不够宽,无法使粒子在交流电场下沉积。