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

<record version="1" id="641">
 <title>position vector</title>
 <name>PositionVector</name>
 <created>2009-04-17 18:54:19</created>
 <modified>2009-04-17 18:54:19</modified>
 <type>Definition</type>
<parent id="208">vector</parent>
 <creator id="21" name="pahio"/>
 <modifier id="441" name="bci1"/>
 <author id="21" name="pahio"/>
 <classification>
	<category scheme="msc" code="02.30.-f"/>
 </classification>
 <synonyms>
	<synonym concept="position vector" alias="radius vector"/>
 </synonyms>
 <related>
	<object name="FunctorialAlgebraicGeometry"/>
 </related>
 <preamble>% this is the default PlanetPhysics preamble.  as your knowledge
% of TeX increases, you will probably want to edit this, but
% it should be fine as is for beginners.

% almost certainly you want these
\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}

% used for TeXing text within eps files
%\usepackage{psfrag}
% need this for including graphics (\includegraphics)
%\usepackage{graphicx}
% for neatly defining theorems and propositions
%\usepackage{amsthm}
% making logically defined graphics
%\usepackage{xypic}

% there are many more packages, add them here as you need them

% define commands here</preamble>
 <content>In the space $\mathbb{R}^3$, the vector 
$$\vec{r} \;:=\; (x,\,y,\,z) \;=\; x\vec{i}+y\vec{j}+z\vec{k}$$
directed from the origin to a point \,$(x,\,y,\,z)$\, is the {\em position vector} of this point.\, When the point is \PMlinkescapetext{variable}, $\vec{r}$ \PMlinkescapetext{represents} a vector field and its \PMlinkescapetext{length}
$$r \;:=\; \sqrt{x^2+y^2+z^2}$$
a scalar \PMlinkescapetext{field}.

The \PMlinkescapetext{simple formulae}
\begin{itemize}
\item $\nabla\!\cdot\vec{r} = 3$
\item $\nabla\!\times\!\vec{r} = \vec{0}$
\item $\displaystyle\nabla r = \frac{\vec{r}}{r} = \vec{r}^0$
\item $\displaystyle\nabla\frac{1}{r} = -\frac{\vec{r}}{r^3} = -\frac{\vec{r}^0}{r^2}$
\item $\displaystyle\nabla^2\frac{1}{r} = 0$
\end{itemize}
are valid, where $\vec{r}^0$ is the unit vector having the direction of $\vec{r}$.

If\, $\vec{c}$\, is a \PMlinkescapetext{constant} vector,\, $\vec{U}\!\!:\mathbb{R}^3\to\mathbb{R}^3$\, a vector function and\, $f\!\!:\mathbb{R}\to\mathbb{R}$\, is a twice differentiable function, then the formulae
\begin{itemize}
\item $\nabla(\vec{c}\cdot\!\vec{r}) = \vec{c}$
\item $\nabla\cdot(\vec{c}\times\vec{r}) = 0$
\item $(\vec{U}\!\cdot\!\nabla)\vec{r} = \vec{U}$
\item $(\vec{U}\!\times\!\nabla)\!\cdot\!\vec{r} = 0$
\item $(\vec{U}\!\times\!\nabla)\!\times\!\vec{r} = -2\vec{U}$
\item $\nabla f(r) = f'(r)\,\vec{r}^0$
\item $\displaystyle\nabla^2f(r) = f''(r)\!+\frac{2}{r}f'(r)$
\end{itemize}
hold.

\begin{thebibliography}{9}
\bibitem{VV}{\sc K. V\"ais\"al\"a:} {\em Vektorianalyysi}. \,Werner S\"oderstr\"om Osakeyhti\"o, Helsinki (1961).
\end{thebibliography}</content>
</record>
