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

<record version="15" id="4642">
 <title>Clairaut's theorem</title>
 <name>ClairautsTheorem</name>
 <created>2003-08-22 03:21:04</created>
 <modified>2006-11-13 15:21:39</modified>
 <type>Theorem</type>
 <creator id="13753" name="Mathprof"/>
 <author id="13753" name="Mathprof"/>
 <author id="2760" name="yark"/>
 <author id="2947" name="flynnheiss"/>
 <classification>
	<category scheme="msc" code="26B12"/>
 </classification>
 <synonyms>
	<synonym concept="Clairaut's theorem" alias="equality of mixed partials"/>
 </synonyms>
 <preamble>\usepackage{amsmath}
\usepackage{amsfonts}
\usepackage{amssymb}

\usepackage{amsthm}

\newtheorem*{cthm*}{Clairaut's Theorem}</preamble>
 <content>\begin{cthm*}
If $\mathbf{f}\colon\mathbb{R}^n \to \mathbb{R}^m$ is a function whose second partial derivatives exist and are continuous on a set $S \subseteq \mathbb{R}^n$, then
\[
   \frac{\partial^2 f}{\partial x_i \partial x_j}
  =\frac{\partial^2 f}{\partial x_j \partial x_i}
\]
on $S$, where $1 \leq i,j \leq n$.
\end{cthm*}

This theorem is commonly referred to as \emph{the equality of mixed partials}.
It is usually first presented in a vector calculus course,
and is useful in this context for proving basic properties of the interrelations of gradient, divergence, and curl.
For example, if $\mathbf{F}\colon \mathbb{R}^3 \to \mathbb{R}^3$ is a function satisfying the hypothesis, then $\nabla \cdot (\nabla \times \mathbf{F}) =0$.
Or, if $f\colon\mathbb{R}^3 \to \mathbb{R}$ is a function satisfying the hypothesis, then $\nabla \times \nabla f= \mathbf{0}$.</content>
</record>
