dorsal/arxiv
View SchemaSelf-similar asymptotics for a class of Hele-Shaw flows driven solely by surface tension
| Authors | Baruch Meerson, Pavel V. Sasorov, Arkady Vilenkin |
|---|---|
| Categories | |
| ArXiv ID | physics/0610103 |
| URL | https://arxiv.org/abs/physics/0610103 |
| DOI | 10.1016/j.physd.2007.04.019 |
Abstract
We investigate the dynamics of relaxation, by surface tension, of a family of curved interfaces between an inviscid and viscous fluids in a Hele-Shaw cell. At t=0 the interface is assumed to be of the form |y|=A x^m, where A>0, m \geq 0, and x>0. The case of 0<m<1 corresponds to a smooth shape, m>1 corresponds to a cusp, whereas m=1 corresponds to a wedge. The inviscid fluid tip retreats in the process of relaxation, forming a lobe which size grows with time. Combining analytical and numerical methods we find that, for any m, the relaxation dynamics exhibit self-similar behavior. For m\neq 1 this behavior arises as an intermediate asymptotics: at late times for 0\leq m<1, and at early times for m>1. In both cases the retreat distance and the lobe size exhibit power law behaviors in time with different dynamic exponents, uniquely determined by the value of m. In the special case of m=1 (the wedge) the similarity is exact and holds for the whole interface at all times t>0, while the two dynamic exponents merge to become 1/3. Surprisingly, when m\neq 1, the interface shape, rescaled to the local maximum elevation of the interface, turns out to be universal (that is, independent of m) in the similarity region. Even more remarkably, the same rescaled interface shape emerges in the case of m=1 in the limit of zero wedge angle.
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"abstract": "We investigate the dynamics of relaxation, by surface tension, of a family of\ncurved interfaces between an inviscid and viscous fluids in a Hele-Shaw cell.\nAt t=0 the interface is assumed to be of the form |y|=A x^m, where A\u003e0, m \\geq\n0, and x\u003e0. The case of 0\u003cm\u003c1 corresponds to a smooth shape, m\u003e1 corresponds to\na cusp, whereas m=1 corresponds to a wedge. The inviscid fluid tip retreats in\nthe process of relaxation, forming a lobe which size grows with time. Combining\nanalytical and numerical methods we find that, for any m, the relaxation\ndynamics exhibit self-similar behavior. For m\\neq 1 this behavior arises as an\nintermediate asymptotics: at late times for 0\\leq m\u003c1, and at early times for\nm\u003e1. In both cases the retreat distance and the lobe size exhibit power law\nbehaviors in time with different dynamic exponents, uniquely determined by the\nvalue of m. In the special case of m=1 (the wedge) the similarity is exact and\nholds for the whole interface at all times t\u003e0, while the two dynamic exponents\nmerge to become 1/3. Surprisingly, when m\\neq 1, the interface shape, rescaled\nto the local maximum elevation of the interface, turns out to be universal\n(that is, independent of m) in the similarity region. Even more remarkably, the\nsame rescaled interface shape emerges in the case of m=1 in the limit of zero\nwedge angle.",
"arxiv_id": "physics/0610103",
"authors": [
"Baruch Meerson",
"Pavel V. Sasorov",
"Arkady Vilenkin"
],
"categories": [
"physics.flu-dyn",
"nlin.PS"
],
"doi": "10.1016/j.physd.2007.04.019",
"title": "Self-similar asymptotics for a class of Hele-Shaw flows driven solely by surface tension",
"url": "https://arxiv.org/abs/physics/0610103"
},
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