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薄膜限制诱导两亲嵌段共聚物薄膜中的“跳跃渗流”润湿转变。

Film Confinement Induced "Jump-Percolation" Wetting Transition in Amphiphilic Block Copolymer Films.

机构信息

Department of Polymer Engineering, The University of Akron , 250 South Forge Street, Akron, Ohio 44325-0301, United States.

National Institute of Standards and Technology , Gaithersburg, Maryland 20899, United States.

出版信息

ACS Appl Mater Interfaces. 2017 Oct 11;9(40):35349-35359. doi: 10.1021/acsami.7b07245. Epub 2017 Oct 2.

Abstract

We report a first-order like sharp surface wettability transition with varying film thickness dependent morphology in cast films of an amphiphilic triblock copolymer. Films composed of poly(2-(N-ethylperfluorooctanesulfonamido) ethyl methyl acrylate), poly(FOSM), and poly(N,N'-dimethyl acrylamide), poly(DMA), with thickness (h) in the transition-range, 200 < h < 300 nm, exhibited an abrupt hydrophobic to hydrophilic dynamic water contact angle transition. After an induction time, t ≈ 40 to 180 s, water contact angle varied as θ ≈ 116° to 40° with an ultrafast contact angle decay time constant, [Formula: see text] ≈ -18°/s. This behavior is a result of competing heterogeneous and antagonistic effects of bumpy poly(DMA) wetting domains against a nonwetting planar poly(FOSM) background, with a "jump percolation" wetting transition when the poly(DMA) domain density reaches unity. Outside of this film thickness range, relatively shallow decreasing water contact angle gradients were observed with a monotonically increasing poly(DMA) domain area coverage with increasing film thickness in the overall range of 40 nm (hydrophobic, θ ≈ 118°) < h < 500 nm (hydrophilic, θ ≈ 8°). The optical diffuse reflectance properties of these rough surfaces exhibit an onset of diffuse reflectance maxima correlated to the transition morphology film thickness.

摘要

我们报告了在两亲性三嵌段共聚物的铸膜中存在厚度相关形态的一级类表面润湿性转变。厚度在转变范围内(200< h <300nm)的聚(2-(N-乙基全氟辛烷磺酰胺基)乙基甲基丙烯酰胺)、聚(FOSM)和聚(N,N'-二甲基丙烯酰胺)、聚(DMA)组成的薄膜,表现出突然的从疏水到亲水的动态水接触角转变。在诱导时间 t ≈ 40 到 180 秒后,水接触角随着θ ≈ 116°到 40°的变化,具有超快的接触角衰减时间常数,[Formula: see text] ≈ -18°/s。这种行为是由凹凸不平的聚(DMA)润湿域与非润湿的平面聚(FOSM)背景之间的竞争非均匀和拮抗效应引起的,当聚(DMA)域密度达到 1 时,会发生“跳跃渗流”润湿转变。在这个薄膜厚度范围之外,观察到相对较浅的水接触角梯度减小,随着薄膜厚度的增加,聚(DMA)域面积覆盖率呈单调增加,在整个 40nm(疏水,θ ≈ 118°)< h <500nm(亲水,θ ≈ 8°)范围内。这些粗糙表面的光学漫反射性质表现出与转变形态薄膜厚度相关的漫反射最大值的起始。

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