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Issue 17, 2016
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Contact line of adsorbed colloid–polymer droplets in theory and experiment

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Abstract

The contact line between the colloid-rich bulk liquid and an adsorbed thin film in colloid–polymer mixtures (CPM) is studied by means of an interface displacement model. The interface displacement profiles are compared to laser scanning confocal microscopy (LSCM) images. The mixtures consist of poly(methylmetacrylate) (PMMA) colloids and polystyrene (PS) polymers with polymer-to-colloid size ratio q = 1.18. Based on the experimental parameters, the theoretical model predicts a contact angle for colloid-rich liquid droplets adsorbed on glass of θ = 59°, assuming a contact line with infinite radius, R = ∞. When a contact-line curvature correction and a correction for the protein-limit character of the CPM are taken into account, a modest shift is obtained. The refined theory predicts θ ≈ 56°. The contact angle determined visually from the LSCM images is θ ≈ 30°. The model predicts a three-phase contact-line tension of τ = −1.2 × 10−12 N (uncorrected) and τ = −2.3 × 10−13 N (with protein-limit correction), which is physically sound both in sign and magnitude. The line tension influences the contact angle to a small extent due to the contact line curvature. The predicted width of the transition zone between the thin film and the droplet is about 2 μm. The effect of gravity is noticeable as a deformation near the middle of the droplet.

Graphical abstract: Contact line of adsorbed colloid–polymer droplets in theory and experiment

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Publication details

The article was received on 09 Dec 2015, accepted on 21 Mar 2016 and first published on 22 Mar 2016


Article type: Paper
DOI: 10.1039/C5SM02978C
Citation: Soft Matter, 2016,12, 4052-4058
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    Contact line of adsorbed colloid–polymer droplets in theory and experiment

    J. Koning, Y. Hennequin, D. Bonn and J. O. Indekeu, Soft Matter, 2016, 12, 4052
    DOI: 10.1039/C5SM02978C

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