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Lecture Notes for 120 - UCLA Department of Mathematics

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3.3. CLOSED SPACE CURVES 66<br />

(12) Prove that a unit speed curve q with non-zero curvature and torsion lies<br />

on a sphere if there are constants a, b such that<br />

✓ ✓ˆ ◆ ✓ˆ ◆◆<br />

apple a cos ⌧ds + b sin ⌧ds =1<br />

Hint: Show<br />

✓ ◆<br />

1 d 1<br />

⌧ ds apple<br />

✓ˆ<br />

= a sin<br />

◆ ✓ˆ<br />

⌧ds + b cos<br />

◆<br />

⌧ds<br />

and<br />

⌧<br />

apple = d ✓ ✓ˆ ◆ ✓ˆ ◆◆<br />

a sin ⌧ds + b cos ⌧ds<br />

ds<br />

and use the previous exercise.<br />

(13) Show that if a curve with constant curvature lies on a sphere then it is<br />

part <strong>of</strong> a circle, i.e., it is <strong>for</strong>ced to be planar.<br />

(14) Show that<br />

q ⇤ (s) =q + 1 apple N + 1 ✓ˆ ◆<br />

apple cot ⌧ds B<br />

defines an envelope <strong>for</strong> q.<br />

(15) Show that a planar curve has infinitely many Bertrand mates.<br />

(16) Let q, q ⇤ be two Bertrand mates.<br />

(a) (Schell) Show that<br />

⌧⌧ ⇤ = sin2 ✓<br />

r 2<br />

(b) (Mannheim) Show that<br />

(1 rapple)(1+rapple ⇤ ) = cos 2 ✓<br />

(17) Consider a curve q (s) parametrized by arclength with positive curvature<br />

and non-vanishing torsion such that<br />

appler + ⌧rcot ✓ =1<br />

i.e., there is a Bertrand mate.<br />

(a) Show that the Bertrand mate is uniquely determined by r.<br />

(b) Show that if q has two different Bertrand mates then it must be a<br />

generalized helix.<br />

(c) Show that if a generalized helix has a Bertrand mate then its curvature<br />

and torsion are constant, consequently it is a circular helix.<br />

(18) Investigate properties <strong>of</strong> a pair <strong>of</strong> curves that have the same normal planes<br />

at corresponding points, i.e., their tangent lines are parallel.<br />

(19) Investigate properties <strong>of</strong> a pair <strong>of</strong> curves that have the same binormal lines<br />

at corresponding points.<br />

3.3. Closed Space Curves<br />

We start by studying spherical curves. In fact any regular space curve generates<br />

a natural spherical curve, the unit tangent. We studied this <strong>for</strong> planar curves where<br />

the unit tangent became a curve on a circle. In that case the length <strong>of</strong> the unit<br />

tangent curve can be interpreted as an integral <strong>of</strong> the curvature and it also measures<br />

how much the curve turns. When the planar curve is closed this turning necessarily<br />

has to be a multiple <strong>of</strong> 2⇡.

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