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Adaptation of a Styrene–Acrylic Acid Copolymer Surface to Water
[Image: see text] Solid surfaces, in particular polymer surfaces, are able to adapt upon contact with a liquid. Adaptation results in an increase in contact angle hysteresis and influences the mobility of sliding drops on surfaces. To study adaptation and its kinetics, we synthesized a random copoly...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American
Chemical Society
2021
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7880564/ https://www.ncbi.nlm.nih.gov/pubmed/33439030 http://dx.doi.org/10.1021/acs.langmuir.0c03226 |
Sumario: | [Image: see text] Solid surfaces, in particular polymer surfaces, are able to adapt upon contact with a liquid. Adaptation results in an increase in contact angle hysteresis and influences the mobility of sliding drops on surfaces. To study adaptation and its kinetics, we synthesized a random copolymer composed of styrene and 11–25 mol% acrylic acid (PS/PAA). We measured the dynamic advancing (θ(A)) and receding (θ(R)) contact angles of water drops sliding down a tilted plate coated with this polymer. We measured θ(A) ≈ 87° for velocities of the contact line <20 μm/s. At higher velocities, θ(A) gradually increased to ∼98°. This value is similar to θ(A) of a pure polystyrene (PS) film, which we studied for comparison. We associate the gradual increase in θ(A) to the adaptation process to water: The presence of water leads to swelling and/or an enrichment of acid groups at the water/polymer interface. By applying the latest adaptation theory (Butt et al. Langmuir2018, 34, 1129230110544), we estimated the time constant of this adaptation process to be ≪1 s. For sliding water drops, θ(R) is ∼10° lower compared to the reference PS surface for all tested velocities. Thus, at the receding side of a sliding drop, the surface is already enriched by acid groups. For a water drop with a width of 5 mm, the increase in contact angle hysteresis corresponds to an increase in capillary force in the range of 45–60 μN, depending on sliding velocity. |
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