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Chapter 4: Geometry

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esults hold at point f´Øµ of :<br />

x¼¼ ¢ x ¼ <br />

x ¼ <br />

¿ x¼ ¡ ´x ¼¼ ¢ x ¼¼¼ µ<br />

x ¼ ¢ x ¼¼ (4.20.3)<br />

¾<br />

The vectors of the moving trihedron satisfy the Serret–Frenet equations<br />

t n n t · b b n (4.20.4)<br />

For any plane curve represented parametrically by x f´Øµ ´Ø ´Øµ ¼µ,<br />

<br />

<br />

¬<br />

¬ ¾ Ü ¬¬<br />

Ø ¾ ¡ ¾<br />

¿¾<br />

(4.20.5)<br />

½· Ü<br />

Ø<br />

Expressions for the curvature vector and curvature of a plane curve corresponding to<br />

different representations are given in the following table:<br />

Representation Curvature vector k Curvature, ½<br />

Ü ´Øµ<br />

Ý ´Øµ<br />

Ý ´Üµ<br />

Ö ´µ<br />

´ÜĐÝ ÝĐܵ<br />

´Ü ¾ · Ý ¾ µ ¾ ´ Ý ÜĐÝ ÝĐÜ<br />

ܵ<br />

´Ü ¾ · Ý ¾ µ ¿¾<br />

Ý ¼¼<br />

Ý ¼¼ <br />

´½ · Ý ¼¾ µ ´ ݼ ½µ<br />

¾ ´½ · Ý ¼¾ µ ¿¾<br />

´Ö ¾ ·¾Ö ¼ ¾<br />

ÖÖ ¼¼ µ ´ Ö ×Ò Ö Ó× Ö ¾ ·¾Ö ¼ ¾<br />

ÖÖ ¼¼<br />

´Ö ¾ · Ö ¼ ¾ µ<br />

¾ Ö Ó× Ö ×Ò µ ´Ö ¾ · Ö ¼ ¾ µ<br />

¿¾<br />

The equation of the osculating circle of a plane curve is given by<br />

where c x · ¾ k is the center of curvature.<br />

´y cµ ¡ ´y cµ ¾ (4.20.6)<br />

THEOREM 4.20.1<br />

(Fundamental existence and uniqueness theorem)<br />

Let ´×µ and ´×µ be any continuous functions de ne d for all × ¾ ℄. Then there<br />

exists, up to a congruence, a unique space curve for which is the curvature<br />

function, is the torsion function, and × an arc length parameter along .<br />

4.20.1.3 Example<br />

A regular parametric representation of the circular helix is given by x f´Øµ <br />

´ Ó× Ø ×Ò Ø Øµ, for all Ø ¾ Ê, where ¼ and ¼are constant. By successive<br />

differentiation,<br />

x ¼ ´ ×Ò Ø Ó× Ø µ<br />

x ¼¼ ´ Ó× Ø ×Ò Ø ¼µ<br />

x ¼¼¼ ´<br />

so that ×<br />

Ø x¼ <br />

Ô<br />

¾ · ¾ . Hence,<br />

×Ò Ø Ó× Ø ¼µ<br />

1. Arc length parameter: × «´Øµ Ø´ ¾ · ¾ µ ¾<br />

½<br />

2. Curvature vector: k t<br />

× Ø t<br />

× Ø ´¾ · ¾ µ ½´ Ó× Ø ×Ò Ø ¼µ<br />

(4.20.7)<br />

© 2003 by CRC Press LLC

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