Bubble-induced acoustic mixing in a microfluidic device

Huaying Chen, K. Petkovic-Duran, M. Best, Yonggang Zhu
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引用次数: 1

Abstract

Homogeneous and fast mixing of samples at microscale is a critical requirement for successful applications of microfluidics in biochemical analysis, chemical synthesis, drug delivery and nanomaterial synthesis. This paper reports the optimisation of bubble-induced mixing in a microfluidic device in terms of voltage, driving frequency, piezo transducer position and PDMS thickness. The microfluidic device consists of a microwell (with the diameter of 1mm and volume of ~95 nL) with two rectangular bubble traps (400×400μm) on both sides of the well. After the injection of liquid, air bubbles were spontaneously trapped in two rectangular traps. When the frequency of a piezo was equal to the resonance frequency of air bubbles, strong liquid recirculation formed (so called acoustic microstreaming) in the vicinity of the interface of air bubbles and water. The acoustic induced flow of microbeads and mixing of water and fluorescence dye were imaged to study the mixing efficiency. For a given voltage and PDMS thickness, when the piezo was placed on top of the well, the mixing was most vigorous. For a given frequency, the mixing efficiency was directly proportional to the voltage (4-20V) and inversely proportional to the PDMS thickness (0.3-2mm). When the frequency driving the piezo was approaching the resonance frequency of air bubbles, the mixing efficiency was maximal, while when it was far away from the resonance frequency of air bubbles, the mixing efficiency was much lower. This work provides guidance to the design and the application of bubble-induced acoustic mixing in microfluidics.
微流控装置中气泡诱导的声混合
在微尺度下样品的均匀和快速混合是微流体在生化分析、化学合成、药物传递和纳米材料合成中成功应用的关键要求。本文从电压、驱动频率、压电换能器位置和PDMS厚度等方面对微流控装置中气泡诱导混合进行了优化。微流控装置由一个直径为1mm,容积为~95 nL的微孔和两个矩形泡阱(400×400μm)组成。注入液体后,气泡被自发地困在两个矩形陷阱中。当压电的频率与气泡的共振频率相等时,在气泡与水的界面附近形成强烈的液体再循环(即声微流)。对微珠的声诱导流动和水与荧光染料的混合进行了成像,研究了混合效率。对于给定的电压和PDMS厚度,当压电放置在井的顶部时,混合是最有力的。在给定频率下,混合效率与电压(4 ~ 20v)成正比,与PDMS厚度(0.3 ~ 2mm)成反比。当驱动压电片的频率接近气泡共振频率时,混合效率最大,远离气泡共振频率时,混合效率较低。该工作对微流体中气泡声混合的设计和应用具有指导意义。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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