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

<record version="12" id="1660">
 <title>Frenet frame</title>
 <name>TNBFrame</name>
 <created>2002-02-02 17:02:19</created>
 <modified>2006-12-09 09:03:02</modified>
 <type>Definition</type>
 <creator id="146" name="rmilson"/>
 <author id="146" name="rmilson"/>
 <author id="78" name="slider142"/>
 <classification>
	<category scheme="msc" code="53A04"/>
 </classification>
 <defines>
	<concept> osculating plane</concept>
	<concept>normal plane</concept>
	<concept>rectifying plane</concept>
	<concept>unit normal</concept>
	<concept>unit tangent</concept>
	<concept>binormal</concept>
 </defines>
 <synonyms>
	<synonym concept="Frenet frame" alias="moving trihedron"/>
	<synonym concept="Frenet frame" alias="moving frame"/>
	<synonym concept="Frenet frame" alias="rep\`ere mobile"/>
	<synonym concept="Frenet frame" alias="Frenet trihedron"/>
 </synonyms>
 <related>
	<object name="SpaceCurve"/>
 </related>
 <preamble>\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amssymb}
\newcommand{\reals}{\mathbb{R}}</preamble>
 <content>Let $I\subset \reals$ be an interval and let $\gamma:I\to\reals^3$ be a
parameterized space curve, assumed to be
\PMlinkname{regular}{SpaceCurve} and free of points of inflection. We
interpret $\gamma(t)$ as the trajectory of a particle moving through
3-dimensional space.  The moving trihedron (also known as the Frenet
frame, the Frenet trihedron, the rep\`ere mobile, and the moving
frame) is an orthonormal basis of 3-vectors $T(t),N(t),B(t),$ defined
and named as follows:
\begin{align*}
  T(t) &amp;= \displaystyle \frac{\gamma'(t)}{\Vert \gamma'(t) \Vert}\, ,
  &amp;&amp;
  \text{the unit  tangent;}\\
  N(t) &amp;= \displaystyle \frac{T'(t)}{\Vert T'(t) \Vert} \, ,&amp;&amp;
  \text{the unit normal;}\\ \\
  B(t) &amp;= T(t)\times N(t)  \, ,&amp;&amp; \text{the unit binormal.}\\
\end{align*}
A straightforward application of the chain rule shows that these
definitions are covariant with respect to reparameterizations.  Hence,
the above three vectors should be conceived as being attached to the
point $\gamma(t)$ of the oriented space curve, rather than being
functions of the parameter $t$.

Corresponding to the above vectors are 3 planes, passing through each
point $\gamma(t)$ of the space curve.  The \emph{osculating plane} at
the point $\gamma(t)$ is the plane spanned by $T(t)$ and $N(t)$; the
\emph{normal plane} at $\gamma(t)$ is the plane spanned by $N(t)$ and
$B(t)$; the rectifying plane at $\gamma(t)$ is the plane spanned by
$T(t)$ and $B(t)$.</content>
</record>
