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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Liu, Danqing
Eindhoven University of Technology
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2024Photonic cognition of liquid crystal polymers for unlocking electrical locomotioncitations
- 2020Localized Liquid Secretion from a Photopatterned Liquid-Crystal Polymer Skincitations
- 2020Localized Liquid Secretion from a Photopatterned Liquid-Crystal Polymer Skincitations
- 2020Artificial Organic Skin Wets Its Surface by Field-Induced Liquid Secretioncitations
- 2019Oscillating surfaces fueled by a continuous AC electric fieldcitations
- 2016Reconfiguring nanocomposite liquid crystal polymer films with visible lightcitations
- 2016Regulating the modulus of a chiral liquid crystal polymer network by lightcitations
- 2013Photoswitchable hydrogel surface topographies by polymerisation-induced diffusioncitations
Places of action
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article
Oscillating surfaces fueled by a continuous AC electric field
Abstract
Recent developments in soft matter science provide options to add mobility and motility to polymer films and surfaces. Restrictively, the dynamics in these materials are modulated by a pulsated trigger and the route to autonomous dynamics is still a most intriguing challenge. Here, is the design of a self-sustaining oscillating surface is reported that is fueled by a continuous AC electric field without an intermittent on–off switch. The underlying principle is based on the polarity inversion over the poly(dimethyl siloxane) layer with a 10 nm thick silicon oxide top layer by an integrated tri-electrode structure connected to an alternating power source. In absence of the electric signal, the coating surface is flat. By applying an AC field, the surface corrugates into a sinusoidal morphology and starts oscillating to develop a continuous standing wave. Typically, the oscillation frequency is 0–5 Hz and the modulation depth is 150 nm. The topographical dynamics are analyzed in terms of viscoelastic materials properties and actuation kinetics and are supported by finite element calculations.