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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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§2. The Gauss Map <strong>and</strong> the Second Fundamental Form 47On a sphere, all normal slices have the same (nonzero) curvature. On the other h<strong>and</strong>, if we lookcarefully at Figure 2.2, we see that certa<strong>in</strong> normal slices of a saddle surface are true l<strong>in</strong>es. Thisleads us to make the follow<strong>in</strong>gDef<strong>in</strong>ition. If the normal slice <strong>in</strong> direction V has zero curvature, i.e., if II P (V, V) =0, thenwe call V an asymptotic direction. 2 A curve <strong>in</strong> M is called an asymptotic curve if its tangent vectorat each po<strong>in</strong>t is an asymptotic direction.Example 3. If a surface M conta<strong>in</strong>s a l<strong>in</strong>e, that l<strong>in</strong>e is an asymptotic curve. For the normalslice <strong>in</strong> the direction of the l<strong>in</strong>e conta<strong>in</strong>s the l<strong>in</strong>e (<strong>and</strong> perhaps other th<strong>in</strong>gs far away), which, ofcourse, has zero curvature. ▽Corollary 2.4. There is an asymptotic direction at P if <strong>and</strong> only if k 1 k 2 ≤ 0.Proof. k 2 =0if <strong>and</strong> only if e 2 is an asymptotic direction. Now suppose k 2 ≠0. IfV isa unit asymptotic vector mak<strong>in</strong>g angle θ with e 1 , then we have k 1 cos 2 θ + k 2 s<strong>in</strong> 2 θ =0,<strong>and</strong> sotan 2 θ = −k 1 /k 2 ,sok 1 k 2 ≤ 0. Conversely, if k 1 k 2 ≤ 0, take θ with tan θ = ± √ −k 1 /k 2 , <strong>and</strong> thenV is an asymptotic direction. □Example 4. We consider the helicoid, as pictured <strong>in</strong> Figure 1.2. It is a ruled surface <strong>and</strong> sothe rul<strong>in</strong>gs are asymptotic curves. What is quite less obvious is that the family of helices on thesurface are also asymptotic curves. But, as we see <strong>in</strong> Figure 2.4, the normal slice tangent to thePFigure 2.4helix at P has an <strong>in</strong>flection po<strong>in</strong>t at P , <strong>and</strong> therefore the helix is an asymptotic curve. We ask thereader to check this by calculation <strong>in</strong> Exercise 5. ▽It is also an immediate consequence of Proposition 2.3 that the pr<strong>in</strong>cipal curvatures are themaximum <strong>and</strong> m<strong>in</strong>imum (signed) curvatures of the various normal slices. Assume k 2 ≤ k 1 . Thenk 1 cos 2 θ + k 2 s<strong>in</strong> 2 θ = k 1 (1 − s<strong>in</strong> 2 θ)+k 2 s<strong>in</strong> 2 θ = k 1 +(k 2 − k 1 ) s<strong>in</strong> 2 θ ≤ k 12 Of course, V ̸=0 here. See Exercise 21 for an explanation of this term<strong>in</strong>ology.

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