Evolving Plane Curves by Curvature in Relative Geometries
Evolving Plane Curves by Curvature in Relative Geometries
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DOI:
10.1215/s0012-7094-93-07216-x
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发表时间:
1993-11
影响因子:
2.5
通讯作者:
M. Gage;Yi A. Li
中科院分区:
文献类型:
--
作者:
M. Gage;Yi A. Li
In (0.1) X :S × [0, ω) → IR is the position vector of a family of closed convex plane curves, kN is the curvature vector, with k being the curvature and N the inward pointing normal given by N = −(cos θ, sin θ). The weight function γ(θ) = γ(N) is a function of the normal vector to the curve at each point but does not depend on position in the plane. Equation (0.1) has two significant interpretations. It can be seen as the generalization of the “curve shortening” problem ([Ga8]) to Minkowski geometry or as a simplified model of the motion of the interface of a metal crystal as it melts ([AnGu],[Ta1] and [Ga8]). The proof illustrates most of the techniques that have been used recently in understanding geometric evolution equations as described in [Ha3]. It is not hard to show that the self-similar solutions correspond to positive, 2π periodic solutions of the equation