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DIFFERENTIAL GEOMETRY: A First Course in Curves and Surfaces

DIFFERENTIAL GEOMETRY: A First Course in Curves and Surfaces

DIFFERENTIAL GEOMETRY: A First Course in Curves and Surfaces

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§1. Holonomy <strong>and</strong> the Gauss-Bonnet Theorem 85EXERCISES 3.11. Compute the holonomy around a parallel on*a. a torusb. the paraboloid x(u, v) =(u cos v, u s<strong>in</strong> v, u 2 )c. the catenoid x(u, v) =(cosh u cos v, cosh u s<strong>in</strong> v, u)2. Determ<strong>in</strong>e whether there can be a (smooth) closed geodesic on a surface whena. K>0b. K =0c. K0b. K =0c. K0 that is topologically a cyl<strong>in</strong>der. Prove that there cannot betwo disjo<strong>in</strong>t simple closed geodesics both go<strong>in</strong>g around the neck of the surface.9. Consider the paraboloid M parametrized by x(u, v) =(u cos v, u s<strong>in</strong> v, u 2 ), 0 ≤ u, 0≤ v ≤ 2π.Denote by M r that portion of the paraboloid def<strong>in</strong>ed by 0 ≤ u ≤ r. ∫a. Calculate the geodesic curvature of the boundary circle <strong>and</strong> compute κ g ds.∂M rb. Calculate χ(M r ).∫∫c. Use the Gauss-Bonnet Theorem to compute KdA. F<strong>in</strong>d the limit as r →∞. (ThisM ris the total curvature of the paraboloid.)∫∫d. Calculate K directly (however you wish) <strong>and</strong> compute KdA explicitly.e. Expla<strong>in</strong> the relation between the total curvature <strong>and</strong> the image of the Gauss map of M.10. Consider the pseudosphere (with boundary) M parametrized as <strong>in</strong> Example 6 of Chapter 2,Section 2, but here we take u ≥ 0. Denote by M r that portion def<strong>in</strong>ed by 0 ≤ u ≤ r. (Notethat we are <strong>in</strong>clud<strong>in</strong>g the boundary circle u = 0.)M

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