Materials Map

Discover the materials research landscape. Find experts, partners, networks.

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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Materials Map under construction

The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Deblais, Antoine

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University of Amsterdam

in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (8/8 displayed)

  • 2024Beware of CaBER:Filament thinning rheometry does not always give 'the' relaxation time of polymer solutionscitations
  • 2024Beware of CaBER13citations
  • 2023Towards a constitutive relation for emulsions exhibiting a yield stress3citations
  • 2022Rheology of emulsions with polymer solutions as the continuous phase13citations
  • 2022Understanding the Behaviour of Real Metaborates in Solution9citations
  • 2018Dewetting of thin liquid films surrounding air bubbles in microchannels23citations
  • 2015Spreading of an Oil-in-Water Emulsion on a Glass Plate: Phase Inversion and Pattern Formation15citations
  • 2014Spreading of an Oil-in-Water Emulsion on a Glass Plate: Phase Inversion and Pattern Formation15citations

Places of action

Chart of shared publication
Herrada, Miguel Angel
2 / 2 shared
Eggers, Jens G.
1 / 2 shared
Bonn, Daniel
4 / 23 shared
Gaillard, Antoine
2 / 3 shared
Eggers, Jg
1 / 5 shared
Velikov, Krassimir Petkov
1 / 13 shared
Bonn, D.
2 / 34 shared
Gaillard, A.
1 / 1 shared
Denn, M. M.
1 / 3 shared
Hendrix, Y.
1 / 1 shared
Kibbelaar, H. V. M.
2 / 2 shared
Briand, G.
1 / 1 shared
Dekker, Riande
1 / 2 shared
Rothenberg, G.
1 / 5 shared
Pope, F.
1 / 1 shared
Watson, N. I.
1 / 1 shared
Khodaparast, S.
1 / 4 shared
Stone, H. A.
1 / 1 shared
Scheid, B.
1 / 1 shared
Atasi, O.
1 / 1 shared
Colin, Annie
2 / 13 shared
Kellay, Hamid
2 / 9 shared
Harich, Rim
2 / 2 shared
Chart of publication period
2024
2023
2022
2018
2015
2014

Co-Authors (by relevance)

  • Herrada, Miguel Angel
  • Eggers, Jens G.
  • Bonn, Daniel
  • Gaillard, Antoine
  • Eggers, Jg
  • Velikov, Krassimir Petkov
  • Bonn, D.
  • Gaillard, A.
  • Denn, M. M.
  • Hendrix, Y.
  • Kibbelaar, H. V. M.
  • Briand, G.
  • Dekker, Riande
  • Rothenberg, G.
  • Pope, F.
  • Watson, N. I.
  • Khodaparast, S.
  • Stone, H. A.
  • Scheid, B.
  • Atasi, O.
  • Colin, Annie
  • Kellay, Hamid
  • Harich, Rim
OrganizationsLocationPeople

article

Dewetting of thin liquid films surrounding air bubbles in microchannels

  • Deblais, Antoine
  • Khodaparast, S.
  • Stone, H. A.
  • Scheid, B.
  • Atasi, O.
Abstract

As an air bubble translates in a microchannel, a thin film of liquid is formed on the bounding walls. In a microchannel with a rectangular cross section, the liquid in the film leaks towards the low-pressure corners of the geometry, which leads to the appearance of local minima in the film thickness in the cross-sectional plane. In such a configuration, theory suggests that the minimum film thickness scales with Ca and Ca(4/3) depending on the distance from the nose of the bubble, where Ca = μUb/γ is the flow capillary number based on the bubble velocity Ub, liquid viscosity μ and surface tension γ. We show that the film of a partially wetting liquid dewets on the channel wall at the sites of the local minima in the film thickness as it acquires thicknesses smaller than 100 nm. Our experiments show that the distance Lw between the nose of the bubble and the initial dewetting location is a function of Ca and surface wettability. For channels of different wettability, Lw always scales proportional to Caα, where 1.7 < α < 2 for the range of 10-5 < Ca < 10-2. Moreover, Lw increases up to 10 times by enhancing the wettability of the surface at a given Ca. Our present measurements of Lw provide a design constraint on the lengths of bubbles to maintain a liquid wet channel without dry patches on the wall.

Topics
  • impedance spectroscopy
  • surface
  • theory
  • experiment
  • thin film
  • viscosity