Hamamoto-Kurosaki M, Okumura K
Department of Physics, Graduate School of Ochanomizu University, 2-1-1 Otsuka, 112-8610 Bunkyo-ku, Tokyo, Japan.
Eur Phys J E Soft Matter. 2009 Nov;30(3):283-90. doi: 10.1140/epje/i2009-10526-3. Epub 2009 Oct 24.
Recently, two regimes of viscous friction on textured surfaces were proposed in the context of penetration of liquid film into the texture (EPL 79, 56005 (2007)): the Poiseuille and Stokes regimes. With this idea on viscous friction, we theoretically discuss instabilities on a liquid film on textured surfaces when the film is forced to move with external forces. When a film recedes due to a pressure drop, we find scaling laws for instabilities to be checked in future experiments. When a circular film expands due to centrifugal force we find that the expanding film is stable against rim fluctuations (within the linear stability analysis) with its radius determined by a simple equation. Our discussion sheds light on the curvature of the front of the moving liquid film on textured surfaces and how the film thickness is kept fixed to the texture height on textured surfaces, aspects which have not been discussed in previous studies.
最近,在液膜渗入纹理的背景下(《欧洲物理快报》79, 56005 (2007)),提出了纹理表面上粘性摩擦的两种机制:泊肃叶机制和斯托克斯机制。基于这种粘性摩擦的观点,我们从理论上讨论了纹理表面上液膜在受到外力作用而移动时的不稳定性。当液膜由于压力降而后退时,我们找到了未来实验中有待检验的不稳定性标度律。当圆形液膜由于离心力而膨胀时,我们发现膨胀的液膜对于边缘波动是稳定的(在线性稳定性分析范围内),其半径由一个简单方程确定。我们的讨论揭示了纹理表面上移动液膜前沿的曲率,以及液膜厚度如何保持与纹理表面的纹理高度固定,这些方面在以前的研究中尚未讨论过。