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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8 Chapter 1. <strong>Curves</strong>An important observation from a theoretical st<strong>and</strong>po<strong>in</strong>t is that any regular parametrized curvecan be reparametrized by arclength. For if α is regular, the arclength function s(t) =∫ ta‖α ′ (u)‖duis an <strong>in</strong>creas<strong>in</strong>g function (s<strong>in</strong>ce s ′ (t) =‖α ′ (t)‖ > 0 for all t), <strong>and</strong> therefore has an <strong>in</strong>verse functiont = t(s). Then we can consider the parametrizationNote that the cha<strong>in</strong> rule tells us thatβ(s) =α(t(s)).β ′ (s) =α ′ (t(s))t ′ (s) =α ′ (t(s))/s ′ (t(s)) = α ′ (t(s))/‖α ′ (t(s))‖is everywhere a unit vector; <strong>in</strong> other words, β moves with speed 1.EXERCISES 1.1*1. Parametrize the unit circle (less the po<strong>in</strong>t (−1, 0)) by the length t <strong>in</strong>dicated <strong>in</strong> Figure 1.11.(x,y)(−1,0)tFigure 1.11♯ 2.Consider the helix α(t) =(a cos t, a s<strong>in</strong> t, bt). Calculate α ′ (t), ‖α ′ (t)‖, <strong>and</strong> reparametrize α byarclength.3. Let α(t) = ( √3 1cos t + √ 1 12s<strong>in</strong> t, √3 1cos t, √3 cos t − √ 12s<strong>in</strong> t ) .reparametrize α by arclength.Calculate α ′ (t), ‖α ′ (t)‖, <strong>and</strong>*4. Parametrize the graph y = f(x), a ≤ x ≤ b, <strong>and</strong> show that its arclength is given by thetraditional formula∫ b √length = 1+ ( f ′ (x) ) 2 dx.a5. a. Show that the arclength of the catenary α(t) =(t, cosh t) for 0 ≤ t ≤ b is s<strong>in</strong>h b.b. Reparametrize the catenary by arclength. (H<strong>in</strong>t: F<strong>in</strong>d the <strong>in</strong>verse of s<strong>in</strong>h by us<strong>in</strong>g thequadratic formula.)*6. Consider the curve α(t) =(e t ,e −t , √ 2t). Calculate α ′ (t), ‖α ′ (t)‖, <strong>and</strong> reparametrize α byarclength, start<strong>in</strong>g at t =0.