2020
DOI: 10.3390/mi11030292
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Microparticle Acoustophoresis in Aluminum-Based Acoustofluidic Devices with PDMS Covers

Abstract: We present a numerical model for the recently introduced simple and inexpensive micromachined aluminum devices with a polydimethylsiloxane (PDMS) cover for microparticle acoustophoresis. We validate the model experimentally for a basic design, where a microchannel is milled into the surface of an aluminum substrate, sealed with a PDMS cover, and driven at MHz frequencies by a piezoelectric lead-zirconate-titanate (PZT) transducer. Both experimentally and numerically we find that the soft PDMS cover suppresses … Show more

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Cited by 24 publications
(18 citation statements)
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“…The basic theory and modeling for such a thin-film PZE-transducer-driven acoustofluidic system, was developed in a perturbation scheme involving the acoustic first-order fields and the steady time-averaged secondorder fields in our previous work [3], founded on the theory for bulk PZE-transducer-driven systems [22] taking the acoustic boundary layers into account analytically through effective boundary conditions [23]. Numerical simulations based on this theory have been validated experimentally for several different microscale acoustofluidic systems [2,9,10,22]. In the following we briefly summarize this basic theory and its numerical implementation and adapt the previous cartesian-coordinate formulation into the cylindrical coordinates of the present axisymmetric system.…”
Section: Model System Theory and Numerical Implementationmentioning
confidence: 99%
See 1 more Smart Citation
“…The basic theory and modeling for such a thin-film PZE-transducer-driven acoustofluidic system, was developed in a perturbation scheme involving the acoustic first-order fields and the steady time-averaged secondorder fields in our previous work [3], founded on the theory for bulk PZE-transducer-driven systems [22] taking the acoustic boundary layers into account analytically through effective boundary conditions [23]. Numerical simulations based on this theory have been validated experimentally for several different microscale acoustofluidic systems [2,9,10,22]. In the following we briefly summarize this basic theory and its numerical implementation and adapt the previous cartesian-coordinate formulation into the cylindrical coordinates of the present axisymmetric system.…”
Section: Model System Theory and Numerical Implementationmentioning
confidence: 99%
“…However, when dealing with bulk acoustic waves (BAW), the topic of this work, electrode shaping is rarely used, and not at all for the above-mentioned membrane devices. A simple split-electrode configuration with an applied anti-symmetric driving voltage, has been used on experiments on bulk piezoelectric (PZE) transducers [9,10] and on thin-film transducers [1] to obtain a strong excitation of anti-symmetric modes for optimal particle focusing. Such systems has also been studied in numerical simulations [3,[11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…To ensure an optimal anti-symmetric motion in the yz plane, the top electrode of the transducer is split in two halves by cutting a small groove using a dicing saw along the x-direction and driven by respective AC-voltages with a 180°phase difference similar to the work reported in the literature. 9,17,18 III. THEORY…”
Section: The Devicementioning
confidence: 99%
“…The underlying mechanism of acoustofluidics uses acoustic waves to generate acoustic radiation forces on particles in the fluid; the strength of the acoustic radiation force depends on the size and density of the particle 12,[29][30][31][32][33] . The high biocompatibility of acoustofluidic devices also benefits downstream analysis by providing samples with complete structures and components [34][35][36][37][38] . Previously, we used acoustofluidics to separate bioparticles, including cells, bacteria, and platelets, in a highly biocompatible manner [39][40][41] .…”
Section: Introductionmentioning
confidence: 99%