2000
DOI: 10.1103/physrevlett.85.4329
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Meniscus Instability in a Thin Elastic Film

Abstract: A new kind of meniscus instability leading to the formation of stationary fingers with a well-defined spacing has been observed in experiments with elastomeric films confined between a plane rigid glass and a thin curved glass plate. The wavelength of the instability increases linearly with the thickness of the confined film, but it is remarkably insensitive to the compliance and the energetics of the system. However, lateral amplitude (length) of the fingers depends on the compliance of the system and on the … Show more

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Cited by 187 publications
(244 citation statements)
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“…The peeling front shows a distinctive fingering pattern, which is reminiscent of Saffman-Taylor instabilities for liquids [16][17][18] or elastic instabilities for soft solids. 19,20 These fingering instabilities of the peel front are then associated with extensive deformation and orientation of the polymer chains in the direction of the motion of the shear device. This type of deformation is analogous although slightly different to what is observed in 908 peel tests of PSA, described as fibrillation.…”
Section: In-situ Visualization Of Failure Mechanisms Under Steady Stamentioning
confidence: 99%
“…The peeling front shows a distinctive fingering pattern, which is reminiscent of Saffman-Taylor instabilities for liquids [16][17][18] or elastic instabilities for soft solids. 19,20 These fingering instabilities of the peel front are then associated with extensive deformation and orientation of the polymer chains in the direction of the motion of the shear device. This type of deformation is analogous although slightly different to what is observed in 908 peel tests of PSA, described as fibrillation.…”
Section: In-situ Visualization Of Failure Mechanisms Under Steady Stamentioning
confidence: 99%
“…High aspect ratio of such systems is noteworthy as the lateral length scale far exceeds the thickness of the film resulting in high degree of confinement for the adhesive. As a result, adhesive stresses at the interface does not always result in uniform deformation through out the whole area of contact, rather spatially varying deformations (Gent et al 1958, Gent et al 1969, Ghatak et al 2000, Mönch et al 2001 attain lower energy for the system. Experimentally we see the existence of a critical thickness of the film or a critical curvature of the flexible plate below which the contact line between the film and the flexible plate does not remain straight, but turns undulatory with a characteristic wavelength which increases linearly with the thickness of the film (Ghatak et al 2003).…”
Section: Introductionmentioning
confidence: 99%
“…Concomitantly, bubbles are formed (Ghatak & Chaudhury 2003;Ghatak et al 2004) just behind the film edge (figure 1), which grow and coalesce to form two viable cracks. When one of these cracks is annihilated at the free edge of the film, the applied moment drops, as the other crack continues to propagate on the smooth part of the film accompanied with a wavy undulation (Ghatak et al 2000) of the contact line.…”
mentioning
confidence: 99%