<?xml version="1.0" encoding="UTF-8"?>

<record version="16" id="1636">
 <title>Serret-Frenet equations</title>
 <name>SerretFrenetFormulas</name>
 <created>2002-02-02 01:46:12</created>
 <modified>2007-06-02 23:21:50</modified>
 <type>Theorem</type>
 <creator id="146" name="rmilson"/>
 <author id="13753" name="Mathprof"/>
 <author id="146" name="rmilson"/>
 <author id="78" name="slider142"/>
 <classification>
	<category scheme="msc" code="53A04"/>
 </classification>
 <synonyms>
	<synonym concept="Serret-Frenet equations" alias="Frenet equations"/>
	<synonym concept="Serret-Frenet equations" alias="Frenet-Serret equations"/>
	<synonym concept="Serret-Frenet equations" alias="Frenet-Serret formulas"/>
	<synonym concept="Serret-Frenet equations" alias="Serret-Frenet formulas"/>
	<synonym concept="Serret-Frenet equations" alias="Frenet formulas"/>
 </synonyms>
 <related>
	<object name="SpaceCurve"/>
	<object name="Torsion"/>
	<object name="CurvatureOfACurve"/>
 </related>
 <preamble>\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amssymb}
\newcommand{\reals}{\mathbb{R}}

\newcommand{\SO}{\operatorname{SO}}</preamble>
 <content>Let $I\subset\reals$ be an interval, and let $\gamma:I\to\reals^3$ be
an arclength parameterization of an oriented space curve, assumed to
be \PMlinkname{regular}{Curve}, and free of points of inflection.  Let $T(s)$, $N(s)$,
$B(s)$ denote the corresponding moving trihedron, and $\kappa(s),
\tau(s)$ the corresponding \PMlinkname{curvature}{CurvatureOfACurve}
and \PMlinkname{torsion functions}{Torsion}.  The following
differential relations, called the Serret-Frenet equations, hold
between these three vectors.
\begin{eqnarray}
\label{eq:dT}
T'(s) &amp;=&amp; \kappa(s) N(s);\\
\label{eq:dN}
N'(s) &amp;=&amp; -\kappa(s) T(s) + \tau(s)B(s); \\
\label{eq:dB}
B'(s) &amp;=&amp; -\tau(s) N(s).
\end{eqnarray}

Equation \eqref{eq:dT} follows directly from the \PMlinkname{definition of the
normal}{MovingFrame} $N(s)$ and from the \PMlinkname{definition of the
curvature}{CurvatureAndTorsion}, $\kappa(s)$. Taking the derivative of
the relation 
$$N(s)\cdot T(s) = 0,$$
gives
$$N'(s)\cdot T(s)  = - T'(s) \cdot N(s) = -\kappa(s).$$
Taking the derivative of the relation
$$N(s)\cdot N(s) = 1,$$
gives
$$N'(s) \cdot N(s) = 0.$$
By the \PMlinkname{definition of torsion}{CurvatureAndTorsion}, we have
$$N'(s)\cdot B(s) = \tau(s).$$
This proves equation \eqref{eq:dN}.
Finally,
taking derivatives of the relations
\begin{gather*}
T(s)\cdot B(s) = 0,\\
N(s)\cdot B(s) = 0,\\
B(s)\cdot B(s) =1,  
\end{gather*}
and making use of \eqref{eq:dT} and \eqref{eq:dN}
gives
\begin{gather*}
B'(s) \cdot T(s) = -T'(s)\cdot B(s) = 0,\\
B'(s) \cdot N(s) = -N'(s)\cdot B(s) = -\tau(s),\\
B'(s)\cdot B(s) = 0.  
\end{gather*}
This proves equation \eqref{eq:dB}.

It is also convenient to describe the Serret-Frenet equations by using
matrix notation.  Let $F:I \to \SO(3)$ (see - special orthogonal
group), the mapping defined by
$$F(s) = (T(s),N(s),B(s)),\quad s\in I$$
represent the Frenet frame as a $3\times 3$ orthonormal
matrix.  Equations \eqref{eq:dT} \eqref{eq:dN} \eqref{eq:dB} can be
succinctly given as
$$F(s)^{-1} F'(s) = 
\begin{pmatrix}
  0 &amp; \kappa(s) &amp; 0 \\
  -\kappa(s)  &amp; 0 &amp; \tau(s) \\
  0 &amp; -\tau(s) &amp; 0
\end{pmatrix}
$$
In this formulation, the above relation is also known as the structure
equations of an oriented space curve.</content>
</record>
