School of Materials Science and Engineering, Tianjin University, Tianjin 300072, P R China.
Langmuir. 2013 Jun 11;29(23):7170-7. doi: 10.1021/la4010517. Epub 2013 Jun 3.
Herein the edge effect from the traction-free boundary condition is utilized to direct the spontaneous surface wrinkling. This boundary condition is attained by a simple combination of mechanical straining and selective exposure of polydimethylsiloxane (PDMS) substrate to O2 plasma (OP) through a copper grid. When the strained PDMS sheet is subjected to selective OP treatment, a patterned heterogeneous surface composed of the OP-exposed "hard" oxidized SiOx region (denoted as D1) and the OP-unexposed "soft" region (denoted as D2) is produced. The subsequent full release of the prestrain (ε(pre)) leads to the selective wrinkling in D1, rather than in D2. It is seen that even in D1, no wrinkling occurs in the vicinity of the D1 edge that is perpendicular to the wavevector. Furthermore, the average wrinkle wavelength in D1 (λ(D1)) is smaller than that of the exposed copper grid-free blank area (λ(blank)). This wavelength decrement between λ(D1) and λ(blank), which can be used to roughly estimate the edge-effect extent, increases with the applied mesh number of copper grids and exposure duration, while decreases with the increase of ε(pre). Meanwhile, there exists a decrease in the amplitude of the patterned wrinkles, when compared with that of the blank region. Additionally, hierarchical wrinkling is induced when the strain-free PDMS substrate is selectively exposed to OP, followed by uniaxial stretching and the subsequent blanket exposure. Consequently, oriented wrinkles perpendicular to the stretching direction are generated in D2. With respect to D1, no wrinkling happens or orthogonal wrinkles occur in this region depending on the applied mesh number, exposure duration, and ε(pre). In the above wrinkling process, the combinative edge effects in two perpendicular directions that are involved sequentially have been discussed.
在此,利用无牵引力边界条件的边缘效应来引导自发表面皱缩。这种边界条件是通过机械应变和对聚二甲基硅氧烷(PDMS)基底的选择性暴露于氧气等离子体(OP)的简单组合来实现的,方法是通过铜网格进行。当应变的 PDMS 片受到选择性 OP 处理时,会产生由 OP 暴露的“硬”氧化硅层(记为 D1)和 OP 未暴露的“软”区域(记为 D2)组成的图案化不均匀表面。随后完全释放预应变(ε(pre))会导致 D1 选择性皱缩,而不是 D2。可以看出,即使在 D1 中,与波矢垂直的 D1 边缘附近也不会发生皱缩。此外,D1 中的平均皱缩波长(λ(D1))小于暴露的无铜网格空白区域(λ(blank))的波长。λ(D1)和 λ(blank)之间的波长减小量(可用于大致估计边缘效应的程度)随施加的铜网格数量和暴露持续时间的增加而增加,而随ε(pre)的增加而减小。同时,与空白区域相比,图案化皱折的振幅减小。此外,当应变自由的 PDMS 基底被选择性地暴露于 OP 之后,进行单轴拉伸和随后的覆盖暴露,会诱导分层皱缩。因此,在 D2 中产生垂直于拉伸方向的定向皱折。对于 D1,根据施加的网格数量、暴露持续时间和ε(pre),该区域不会发生皱缩或出现正交皱折。在上述皱缩过程中,已经讨论了涉及两个垂直方向的组合边缘效应。