Dan F. Smith Department of Chemical Engineering, Lamar University, Beaumont, Texas 77710, United States.
Langmuir. 2012 Apr 3;28(13):5795-801. doi: 10.1021/la3000153. Epub 2012 Mar 15.
Viscoelastic braking theories developed by Shanahan and de Gennes and by others predict deformation of a solid surface at the solid-liquid-air contact line. This phenomenon has only been observed for soft smooth surfaces and results in a protrusion of the solid surface at the three-phase contact line, in agreement with the theoretical predictions. Despite the large (enough to break chemical bonds) forces associated with it, this deformation was not confirmed experimentally for hard surfaces, especially for hydrophobic ones. In this study we use superhydrophobic surfaces composed of an array of silicon nanostructures whose Young modulus is 4 orders of magnitude higher than that of surfaces in earlier recorded viscoelastic braking experiments. We distinguish between two cases: when a water drop forms an adhesive contact, albeit small, with the apparent contact angle θ < 180° and when the drop-surface adhesion is such that the conditions for placing a resting drop on the surface cannot be reached (i.e., θ = 180°). In the first case we show that there is a surface deformation at the three-phase contact line which is associated with a reduction in the hydrophobicity of the surface. For the second case, however, there cannot be a three-phase contact line associated with a drop in contact with the surface, and indeed, if we force-place a drop on the surface by holding it with a needle, no deformation is detected, nor is there a reduction in the hydrophobic properties of the surface. Yet, if we create a long horizontal three-phase contact line by partially immersing the superhydrophobic substrate in a water bath, we see a localized reduction in the hydrophobic properties of the surface in the region where the three-phase contact line used to be. The SEM scan of that region shows a narrow horizontal stripe where the nanorods are no longer there, and instead there is only a shallow structure that is lower than the nanorods height and resembles fused or removed nanorods. Away from that region, either on the part of the surface which was exposed to bulk water or the part which was exposed to air, no change in the hydrophobic properties of the surface is observed, and the SEM scan confirms that the nanorods seem intact in both regions.
山纳汉和德热内等人提出的黏弹性制动理论预测了固液气三相接触线处固体表面的变形。这种现象仅在软而光滑的表面上观察到,导致三相接触线处固体表面的突出,这与理论预测一致。尽管与这种变形相关的力很大(足以破坏化学键),但这种变形在硬表面,尤其是疏水面上,尚未得到实验证实。在这项研究中,我们使用由硅纳米结构阵列组成的超疏水表面,其杨氏模量比以前记录的黏弹性制动实验中的表面高 4 个数量级。我们区分了两种情况:当水滴与表面形成小的粘弹性接触时,表观接触角θ<180°;当液滴与表面的附着力使得无法达到将静止液滴放置在表面上的条件时(即θ=180°)。在第一种情况下,我们表明三相接触线处存在表面变形,这与表面疏水性的降低有关。然而,在后一种情况下,与表面接触的液滴不可能存在三相接触线,事实上,如果我们用针将液滴固定在表面上,就不会检测到变形,也不会检测到表面疏水性的降低。然而,如果我们通过将超疏水基底部分浸入水浴中来创建一个长的水平三相接触线,我们会看到在三相接触线曾经存在的区域,表面疏水性会局部降低。该区域的 SEM 扫描显示出一条狭窄的水平条纹,那里的纳米棒不再存在,取而代之的是只有一个比纳米棒高度低且类似于融合或去除的纳米棒的浅结构。在远离该区域的地方,无论是暴露于体相水的表面部分还是暴露于空气的表面部分,都没有观察到表面疏水性的变化,SEM 扫描证实纳米棒在这两个区域似乎都是完整的。