2016
DOI: 10.1098/rspa.2015.0629
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A curve shortening flow rule for closed embedded plane curves with a prescribed rate of change in enclosed area

Abstract: Motivated by a problem from fluid mechanics, we consider a generalization of the standard curve shortening flow problem for a closed embedded plane curve such that the area enclosed by the curve is forced to decrease at a prescribed rate. Using formal asymptotic and numerical techniques, we derive possible extinction shapes as the curve contracts to a point, dependent on the rate of decreasing area; we find there is a wider class of extinction shapes than for standard curve shortening, for which initially simp… Show more

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Cited by 21 publications
(27 citation statements)
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References 42 publications
(71 reference statements)
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“…All of these stability results are analogous to those for contracting bubbles in a Hele-Shaw cell for which the viscous fluid is of a power-law type [48,49] or for which there is a competition between surface tension and a kinetic-type boundary condition [50,51]. For these problems, there are also linear stability results that show a circular interface may be stable or unstable, depending on a parameter value, leading to the existence of noncircular selfsimilar solutions (that evolve to shapes which appear like k-sided polygons with rounded corners).…”
Section: Similarity Solutions With K-fold Symmetrymentioning
confidence: 62%
“…All of these stability results are analogous to those for contracting bubbles in a Hele-Shaw cell for which the viscous fluid is of a power-law type [48,49] or for which there is a competition between surface tension and a kinetic-type boundary condition [50,51]. For these problems, there are also linear stability results that show a circular interface may be stable or unstable, depending on a parameter value, leading to the existence of noncircular selfsimilar solutions (that evolve to shapes which appear like k-sided polygons with rounded corners).…”
Section: Similarity Solutions With K-fold Symmetrymentioning
confidence: 62%
“…self-similar shrinking interfaces such as those observed in [9,10] when a bubble is driven to extinction by the presence of a sink in a Hele-Shaw cell.…”
Section: 2mentioning
confidence: 83%
“…In particular, for the shrinking interface problem, we choose (1) the space scaling function R( \= t) so that the shrinking interface is always mapped back to its initial size, i.e., the interface does not shrink in the rescaled frame; (2) the time scaling function \rho ( \= t) to slow down the motion of the interface, especially at later times when the interface becomes very small and shrinks extremely rapidly. We note that an alternative time and space rescaling scheme was implemented in [9,10] to accurately simulate vanishing bubbles in a Hele-Shaw cell. Here, we use a semi-implicit, nonstiff time stepping method developed originally in [23] to remove the third order time step constraint.…”
Section: B1207mentioning
confidence: 99%
“…From a mathematical perspective, these issues are reminiscent of the differences between curve shortening flow and mean curvature flow in differential geometry [35,36]. Given that Hele-Shaw flow may be interpreted as a nonlocal version of curve shortening flow in the plane [21,37,38], a final reason to use (2) is that our three-dimensional moving boundary problem can be considered a nonlocal version of the mean curvature flow. Again, in this context we are interested in studying the effect of surface tension in (2) on the development of axially symmetric curvature singularities.…”
Section: Introductionmentioning
confidence: 99%