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Voltage-Induced Buckling of Dielectric Films using Fluid Electrodes
Fluid Dynamics · Submitted 12 Jan 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim These results demonstrate that the voltage--induced buckling of embedded microstructures using fluid electrodes provides a means for high speed attenuation of microfluidic flow.
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The abstract, sentence by sentence
Accurate and integrable control of different flows within microfluidic channels is crucial to further development of lab-on-a-chip and fully integrated adaptable structures. Here we introduce a flexible microactuator that buckles at a high deformation rate and alters the downstream fluid flow. The microactuator consists of a confined, thin, dielectric film that buckles into the microfluidic channel when exposed to voltage supplied through conductive fluid electrodes. We estimate the critical buckling voltage, and characterize the buckled shape of the actuator. Finally, we investigate the effects of frequency, flow rate, and the pressure differences on the behavior of the buckling structure and the resulting fluid flow. These results demonstrate that the voltage--induced buckling of embedded microstructures using fluid electrodes provides a means for high speed attenuation of microfluidic flow.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Accurate and integrable control of different flows within microfluidic channels is crucial to further development of lab-on-a-chip and fully integrated adaptable structures. | background 1.00 | 0.04 | 0.02 | asserted 0.99 |
| s1 | Here we introduce a flexible microactuator that buckles at a high deformation rate and alters the downstream fluid flow. | contribution 1.00 | 0.84 | 0.09 | asserted 1.00 |
| s2 | The microactuator consists of a confined, thin, dielectric film that buckles into the microfluidic channel when exposed to voltage supplied through conductive fluid electrodes. | method 0.69 | 0.36 | 0.05 | asserted 1.00 |
| s3 | We estimate the critical buckling voltage, and characterize the buckled shape of the actuator. | contribution 0.52 | 0.96 | 0.04 | asserted 0.90 |
| s4 | Finally, we investigate the effects of frequency, flow rate, and the pressure differences on the behavior of the buckling structure and the resulting fluid flow. | method 0.52 | 0.95 | 0.05 | asserted 0.59 |
| s5 | These results demonstrate that the voltage--induced buckling of embedded microstructures using fluid electrodes provides a means for high speed attenuation of microfluidic flow. | interpretation 0.98 | 0.91 | 0.94 | asserted 1.00 |
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Original abstract
Accurate and integrable control of different flows within microfluidic channels is crucial to further development of lab-on-a-chip and fully integrated adaptable structures. Here we introduce a flexible microactuator that buckles at a high deformation rate and alters the downstream fluid flow. The microactuator consists of a confined, thin, dielectric film that buckles into the microfluidic channel when exposed to voltage supplied through conductive fluid electrodes. We estimate the critical buckling voltage, and characterize the buckled shape of the actuator. Finally, we investigate the effects of frequency, flow rate, and the pressure differences on the behavior of the buckling structure and the resulting fluid flow. These results demonstrate that the voltage--induced buckling of embedded microstructures using fluid electrodes provides a means for high speed attenuation of microfluidic flow.
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While this material instability is irreversible, reversible elastic instabilities can also be triggered, including creasing and wrinkling instabilities in the presence of surface tension [ref] , bending [ref] and buckling [ref] using fluid electrodes, and snap–through instabilities in the presence of pressure [ref] .
Snapping of Bistable, Prestressed Cylindrical Shells · Introduction · 0.80
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