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

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y eqn. (11.3), where the terms RHS are evaluated at (t, ϕ(t, ·)); s<strong>in</strong>ce G ⊥ iscurve-wise parameterization <strong>in</strong>variant, then‖∂ t ˜C(t, ·)‖G ⊥ = ‖∂ t C(t, ·)‖ G ⊥ .Consequently,Corollary 11.15 G is homotopy-wise parameterization <strong>in</strong>variant if <strong>and</strong> only iffor all b.‖h‖ G = ‖h + bc ′ ‖ GSummariz<strong>in</strong>g all above theory, we obta<strong>in</strong> a method to underst<strong>and</strong>/study/designthe metric G on B, follow<strong>in</strong>g these steps:1. choose a metric G on M that is curve-wise parameterization <strong>in</strong>variant2. G generates the horizontal space W = V ⊥3. project G on W to def<strong>in</strong>e G ⊥ that is homotopy-wise parameterization<strong>in</strong>variant.11.8.1 Horizontal G ⊥ as length m<strong>in</strong>imizerAs we def<strong>in</strong>ed <strong>in</strong> 11.9, to def<strong>in</strong>e the distance we m<strong>in</strong>imize the length <strong>of</strong> the pathsγ : [0, 1] → M that connect a curve c 0 to a reparameterization c 1 ◦ φ <strong>of</strong> the curvec 1 . Consider the follow<strong>in</strong>g sketchy example.Example 11.16 Consider two paths γ 1 <strong>and</strong> γ 2 connect<strong>in</strong>gc 0 to reparameterizations <strong>of</strong> c 1 . Recall that the spaceW c is orthogonal to the orbits, the space V c is tangent tothe orbits. The path γ 1 (that moves <strong>in</strong> some tracts alongthe orbits, with ˙γ 1 ∈ V γ ) is longer than the path γ 2 .The above example expla<strong>in</strong>s the follow<strong>in</strong>g lemma.W cc 0cVcγγ12Lemma 11.17 Let us choose G to be a curve-wise parameterization <strong>in</strong>variantmetric (so, by Prop. 11.8, it cannot be homotopy-wise parameterization<strong>in</strong>variant).1. Let ˜C(t, θ) = C(t, ϕ(t, θ)) where ϕ(t, ·) is a diffeomorphism for all fixed t.M<strong>in</strong>imizem<strong>in</strong> E G ( ˜C)ϕThen at the m<strong>in</strong>imum ˜C ∗ , ∂ t ˜C∗ is horizontal at every po<strong>in</strong>t, <strong>and</strong>E G ( ˜C ∗ ) = E G ⊥( ˜C ∗ ) .O ccc 11 o φo φ’96

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