Abstract

We combine the total variation flow suitable for crystal modeling and image analysis with the dynamic boundary conditions. We analyze the behavior of facets at the parts of the boundary where these conditions are imposed. We devote particular attention to the radially symmetric data. We observe that the boundary layer detachment actually can happen at concave parts of the boundary.

Highlights

  • We consider the total variation flow with the dynamic boundary condition, possibly mixed with the Neumann boundary condition, which can be formally written as follows, ut = div ∇u |∇u| τ vt = − · ν∂u ∂ν u(x, 0) = u0(x) for (x, t) ∈ Ω × (0, T ) =: QT ; for (y, t) ∈ Γ × (0, T ) =: ST ; for (y, t) ∈ (∂Ω \ Γ) × (0, T ); for x ∈ Ω; (1.1)v(y, 0) = v0(y) for y ∈ Γ.Here Ω ⊂ RN is a bounded spatial domain of dimension N ∈ N, and when N > 1, the boundary ∂Ω is supposed to be sufficiently smooth

  • Even though the total variation flow with the Dirichlet boundary conditions was studied by a number of authors, see [4, 13, 41, 42], the details of the boundary behavior were not extensively discussed

  • We introduce a family of evolution problems with dynamic boundary condition indexed by parameter τ ∈ (0, ∞)

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Summary

Introduction

Even though the total variation flow with the Dirichlet boundary conditions was studied by a number of authors, see [4, 13, 41, 42], the details of the boundary behavior were not extensively discussed In particular this applies to the evolution of facets touching the boundary. The authors showed there that a boundary layer may detach from the solution in the bulk This phenomenon is attributed to the lack of uniform parabolicity of the mean curvature flow for graphs. Our goal in this paper is to study instances of occurrence of the “boundary layer detachment phenomenon” in the case of the total variation flow under the dynamic boundary condition on a part of the boundary called Γ. In this case we pinpoint the situation of the boundary layer detachment

Preliminaries
Energy and its lower semi-continuity
The evolution problem and the Comparison Principle
The subdifferential and its canonical section
The representation of the subdifferential
The canonical section
Scaling out parameter τ
Calibrability and coherence
Instant facet formation in the one-dimensional problem
A boundary layer behavior in the radial case in two dimensions
A ball
An annulus case
Facet evolution
Full Text
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