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DIFFERENTIAL GEOMETRY: A First Course in Curves and Surfaces

DIFFERENTIAL GEOMETRY: A First Course in Curves and Surfaces

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§3. Some Global Results 25Apply<strong>in</strong>g this to the case of the tangent <strong>in</strong>dicatrix of a closed space curve, we deduce thefollow<strong>in</strong>g classical result.Theorem 3.3 (Fenchel). The total curvature of any closed space curve is at least 2π, <strong>and</strong>equality holds if <strong>and</strong> only if the curve is a convex, planar curve.Proof. Let Γ be the tangent <strong>in</strong>dicatrix of our space curve. ∫ For almost every ξ ∈ Σwehave#(Γ ∩ ξ ⊥ ) ≥ 2, <strong>and</strong> so it follows from Proposition 3.2 that κds = length(Γ) ≥ 1 (2)(4π) =2π.4Now, we claim that if Γ is a connected, closed curve <strong>in</strong> Σ of length ≤ 2π, then Γ lies <strong>in</strong> a closedhemisphere. It will follow, then, that if Γ is a tangent <strong>in</strong>dicatrix of length 2π, itmust be a greatcircle. (For if Γ lies <strong>in</strong> the hemisphere A · x ≥ 0,∫ Lgreat circle A · x = 0.) It follows that the curve is planar.0T(s) · Ads =0forces T · A =0,soΓis thePNQΓ 1Γ 1Figure 3.2To prove the claim, we proceed as follows. Suppose length(Γ) ≤ 2π. Choose P <strong>and</strong> Q <strong>in</strong> Γso that the arcs Γ 1 = PQ ⌢<strong>and</strong> Γ 2 = QP ⌢have the same length. Choose N bisect<strong>in</strong>g the shortergreat circle arc from P to Q, asshown <strong>in</strong> Figure 3.2. For convenience, we rotate the picture sothat N is the north pole of the sphere. Suppose now that the curve Γ 1 were to enter the southernhemisphere; let Γ 1 denote the reflection of Γ 1 across the north pole (follow<strong>in</strong>g arcs of great circlethrough N). Now, Γ 1 ∪ Γ 1 is a closed curve conta<strong>in</strong><strong>in</strong>g a pair of antipodal po<strong>in</strong>ts <strong>and</strong> therefore islonger than a great circle. (See Exercise 1.) S<strong>in</strong>ce Γ 1 ∪ Γ 1 has the same length as Γ, we see thatlength(Γ) > 2π, which is a contradiction. Therefore Γ <strong>in</strong>deed lies <strong>in</strong> the northern hemisphere. □We now sketch the proof of a result that has led to many <strong>in</strong>terest<strong>in</strong>g questions <strong>in</strong> higherdimensions. We say a simple closed space curve is knotted if we cannot fill it <strong>in</strong> with a disk.Theorem 3.4 (Fary-Milnor). If a simple closed space curve is knotted, then its total curvatureis at least 4π.Sketch of proof. Suppose the total curvature of C is less than 4π. Then the average number#(Γ∩ξ ⊥ ) < 4. S<strong>in</strong>ce this is generically an even number ≥ 2 (whenever the great circle isn’t tangentto Γ), there must be an open set of ξ’s for which we have #(Γ∩ξ ⊥ )=2. Choose one such, ξ 0 . Thismeans that the tangent vector to C is only perpendicular to ξ 0 twice, so the function f(x) =x · ξ 0has only two critical po<strong>in</strong>ts. That is, the planes perpendicular to ξ 0 will (by Rolle’s Theorem)

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