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Metrics of curves in shape optimization and analysis - Andrea Carlo ...

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CutΩ(The arrows represent the distance R(s) from y(s) ∈ ∂Ω to the cutlocus).Figure 9: Smooth contour <strong>and</strong> cutlocus.6.3.7 Pullback <strong>of</strong> the metric on smooth contoursIf Ω is smooth but not convex, then the above formula holds up to the cutlocus.Def<strong>in</strong>ition 6.22 The cutlocus ( a.k.a. the external skeleton) is the set <strong>of</strong>po<strong>in</strong>ts x ∉ Ω such that there are two (or more) different po<strong>in</strong>ts y 1 , y 2 ∈ Ω <strong>of</strong>m<strong>in</strong>imum distance from x to Ω, that is,|x − y 1 | = |x − y 2 | = u Ω (x) .We def<strong>in</strong>e a function R(s) : [0, L] → [0, ∞] that measures the distance from ∂Ωto the cutlocus Cut; <strong>in</strong> turn, we can parameterize Cut asCut = {ψ(R(s), s) | s ∈ [0, L], R(s) < ∞} ;R(s) is locally Lipschitz where it is f<strong>in</strong>ite (by results <strong>in</strong> Itoh <strong>and</strong> Tanaka [25], Li<strong>and</strong> Nirenberg [32]). The “polar” change <strong>of</strong> coord<strong>in</strong>ates ψ (def<strong>in</strong>ed <strong>in</strong> (6.3)) is adiffeomorphism between the sets{(ρ, s) s ∈ [0, L], 0 < ρ < R(s)} ↔ lR 2 \ (Ω ∪ Cut) .See fig. 9.The pullback metric for deformations <strong>of</strong> the contour ∂Ω is∫ [ ∫ ]R(s)〈h, k〉 =(ϕ ′ (ρ)) 2 (1 + ρκ(s)) dρ α(s)β(s) ds∂Ω06.3.8 ConclusionIn this case we have found (a posteriori) a Riemannian metric <strong>of</strong> closed embeddedplanar <strong>curves</strong>, <strong>and</strong> we know the structure <strong>of</strong> the completion, <strong>and</strong> the completionadmits m<strong>in</strong>imal geodesics. On the down side, the completion is not really “asmooth Riemannian manifold”. For example, it is difficult to study the m<strong>in</strong>imalgeodesics, <strong>and</strong> to prove any property about them. Anyway, the fact that N c islocally compact <strong>and</strong> the regularity property 6.18 <strong>of</strong> L p spaces suggest that itmay be possible to “shoot geodesics” (<strong>in</strong> some weak form). Unfortunately thetopology has too few open sets to be used for <strong>shape</strong> <strong>optimization</strong>: many simpleenergy functionals are not cont<strong>in</strong>uous.50

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