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

<record version="1" id="655">
 <title>vector potential</title>
 <name>VectorPotential</name>
 <created>2009-04-18 06:55:21</created>
 <modified>2009-04-18 06:55:21</modified>
 <type>Definition</type>
 <creator id="21" name="pahio"/>
 <modifier id="21" name="pahio"/>
 <author id="21" name="pahio"/>
 <classification>
	<category scheme="msc" code="02.30.-f"/>
	<category scheme="msc" code="02.40.Hw"/>
 </classification>
 <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}

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%\usepackage{psfrag}
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%\usepackage{graphicx}
% for neatly defining theorems and propositions
%\usepackage{amsthm}
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%\usepackage{xypic}

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% define commands here</preamble>
 <content>Let\, $\vec{U} = \vec{U}(x,\,y,\,z)$\, be a vector field in $\mathbb{R}^3$ with continuous partial derivatives.\, Then the following three conditions are \PMlinkname{equivalent}{Equivalent3}:
\begin{itemize}
 \item The surface integrals of $\vec{U}$ over all contractible \PMlinkname{closed surfaces}{Sphere} $S$ vanish:
$$\oint_S\vec{U}\cdot d\vec{S} = 0$$
 \item The divergence of $\vec{U}$ vanishes everywhere in the \PMlinkname{field}{VectorField}:
$$\nabla\!\cdot\!\vec{U} = 0$$
 \item There exists the {\em vector potential}\, $\vec{A} = \vec{A}(x,\,y,\,z)$\, of $\vec{U}$:
$$\nabla\!\times\!\vec{A} = \vec{U}$$
\end{itemize}

\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>
