2020
DOI: 10.1016/j.jcis.2019.10.008
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Controlled disassembly of colloidal aggregates confined at fluid interfaces using magnetic dipolar interactions

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Cited by 13 publications
(29 citation statements)
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“…[11] They show specific structures and dynamics not observable in the bulk of liquids. [20,58] The strategy of transport introduced in this work, easily implemented but unique to strongly confined suspensions, takes advantage of the higher affinity of the particles to one of the media and the anisotropic character of the magnetic dipolar interaction to transport colloids or molecules onto fluid interfaces, through loosely packed self-assembled lattices. In contrast to other experimental realizations, which require of sophisticated prefabricated substrates or optical ratchets, [6,8,59] here the active control over colloids is dynamically achieved thanks to the driven potential generated by the adsorbed particles themselves.…”
Section: Resultsmentioning
confidence: 99%
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“…[11] They show specific structures and dynamics not observable in the bulk of liquids. [20,58] The strategy of transport introduced in this work, easily implemented but unique to strongly confined suspensions, takes advantage of the higher affinity of the particles to one of the media and the anisotropic character of the magnetic dipolar interaction to transport colloids or molecules onto fluid interfaces, through loosely packed self-assembled lattices. In contrast to other experimental realizations, which require of sophisticated prefabricated substrates or optical ratchets, [6,8,59] here the active control over colloids is dynamically achieved thanks to the driven potential generated by the adsorbed particles themselves.…”
Section: Resultsmentioning
confidence: 99%
“…In a binary system of paramagnetic particles of different size, with radius R B and R s , adsorbed onto a fluid interface, the particle centers are confined to planes separated by a distance Δ z , According to the SEM images of the magnetic particles obtained with the gel trapping technique (GET) (see inset in Figure a and ref. [ 20 ] ), the affinity of the two types of particles is preferentially to the water phase, and Δ z ≈ R B − R s = 0.9 µm. The application of a field parallel to the interface in the X direction, H x , induces the formation of linear aggregates, composed by small and big particles aligned along the X axis.…”
Section: Resultsmentioning
confidence: 99%
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