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首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >Adhesion-induced instability patterns in thin confined elastic film
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Adhesion-induced instability patterns in thin confined elastic film

机译:约束弹性薄膜中的粘附诱导的不稳定性模式

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Adhesion-induced instability has been observed at the interface of a flexible plate and a thin elastic film bonded to a rigid substrate. The surface of the confined film develops undulations almost instantaneously, and instability patterns appear in the form of fingers or bubbles at the interface. The characteristic wavelengths of these instabilities remain independent of all material and geometrical properties of the system except the thickness of the film. These observations contrast sharply with the Saffman-Taylortype phenomenon in which the length scale of the instability patterns depends on the viscous and surface tension forces in addition to the thickness of the liquid film. The analogy between the phenomenon reported here and the Rayleigh-Kelvin instability with curved liquid menisci is more pronounced, as, in both cases, surface force triggers the instability while not determining its wavelength. The instability also throws light on cavitation phenomena in confined adhesive layers. [References: 48]
机译:在柔性板和粘合到刚性基板上的弹性薄膜之间的界面处,观察到了粘合引起的不稳定性。密闭薄膜的表面几乎立即起伏,并且在界面处以手指或气泡的形式出现不稳定性图案。这些不稳定性的特征波长保持独立于系统的所有材料和几何特性,除了薄膜的厚度。这些观察结果与Saffman-Taylortype现象形成鲜明对比,在Saffman-Taylortype现象中,不稳定性图案的长度尺度除液膜的厚度外还取决于粘性和表面张力。此处报道的现象与弯曲液体半月板的Rayleigh-Kelvin不稳定性之间的类比更为明显,因为在两种情况下,表面力都会触发不稳定性,而无法确定其波长。这种不稳定性还揭示了密闭粘合剂层中的气穴现象。 [参考:48]

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