Park Jeongeun, Cha Beomseok, Almus Furkan Ginaz, Sahin Mehmet Akif, Kang Hyochan, Kang Yeseul, Destgeer Ghulam, Park Jinsoo
Department of Mechanical Engineering, Chonnam National University, Yongbong-ro 77, Buk-gu, Gwangju, 61186, Republic of Korea.
Control and Manipulation of Microscale Living Objects, Center for Translational Cancer Research (TranslaTUM), Munich Institute of Biomedical Engineering (MIBE), Department of Electrical Engineering, School of Computation, Information and Technology (CIT), Technical University of Munich, Einsteinstraße 25, 81675, Munich, Germany.
Adv Sci (Weinh). 2024 Dec;11(47):e2407293. doi: 10.1002/advs.202407293. Epub 2024 Oct 30.
Acoustofluidics is a promising technology that leverages acoustic waves for precise manipulation of micro/nano-scale flows and suspended objects within microchannels. Despite many advantages, the practical applicability of conventional acoustofluidic platforms is limited by irreversible bonding between the piezoelectric actuator and the microfluidic chip. Recently, reconfigurable acoustofluidic platforms are enabled by reversible bonding between the reusable actuator and the replaceable polydimethylsiloxane (PDMS) microfluidic chip by incorporating a PDMS membrane for sealing the microchannel and coupling the acoustic waves with the fluid inside. However, a quantitative guideline for selecting a suitable PDMS membrane for various acoustofluidic applications is still missing. Here, a design rule for reconfigurable acoustofluidic platforms is explored based on a thorough investigation of the PDMS thickness effect on acoustofluidic phenomena: acousto-thermal heating (ATH), acoustic radiation force (ARF), and acoustic streaming flow (ASF). These findings suggest that the relative thickness of the PDMS membrane (t) for acoustic wavelength (λ) determines the wave attenuation in the PDMS and the acoustofluidic phenomena. For t/λ ≈ O(1), the transmission of acoustic waves through the membrane leads to the ARF and ASF phenomena, whereas, for t/λ ≈ O(10), the acoustic waves are entirely absorbed within the membrane, resulting in the ATH phenomenon.
声流控技术是一项很有前景的技术,它利用声波在微通道内对微/纳尺度的流体和悬浮物体进行精确操控。尽管有诸多优点,但传统声流控平台的实际适用性受到压电致动器与微流控芯片之间不可逆键合的限制。最近,通过在可重复使用的致动器和可替换的聚二甲基硅氧烷(PDMS)微流控芯片之间采用可逆键合,并结合用于密封微通道以及使声波与内部流体耦合的PDMS膜,实现了可重构声流控平台。然而,对于各种声流控应用而言,仍缺乏选择合适PDMS膜的定量指导原则。在此,基于对PDMS厚度对声流控现象(声热加热(ATH)、声辐射力(ARF)和声流(ASF))影响的深入研究,探索了可重构声流控平台的设计规则。这些研究结果表明,PDMS膜厚度(t)与声波波长(λ)的相对值决定了声波在PDMS中的衰减以及声流控现象。当t/λ≈O(1)时,声波透过膜的传输会导致ARF和声流现象,而当t/λ≈O(10)时,声波会完全被膜吸收,从而导致ATH现象。