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

<record version="4" id="4059">
 <title>proof that normal distribution is a distribution</title>
 <name>ProofThatNormalDistributionIsADistribution</name>
 <created>2003-02-24 01:25:26</created>
 <modified>2008-04-19 15:18:30</modified>
 <type>Proof</type>
<parent id="527">normal random variable</parent>
 <selfproof>0</selfproof>
 <creator id="1863" name="Wkbj79"/>
 <author id="1863" name="Wkbj79"/>
 <author id="455" name="Henry"/>
 <classification>
	<category scheme="msc" code="62E15"/>
 </classification>
 <related>
	<object name="AreaUnderGaussianCurve"/>
 </related>
 <preamble>\usepackage{amssymb}
\usepackage{amsmath}
\usepackage{amsfonts}

\newcommand{\lint}{\int\limits}</preamble>
 <content>\begin{eqnarray*}
\lint_{-\infty}^\infty \frac{e^{-\frac{(x-\mu)^2}{2\sigma^2}}}{\sigma\sqrt{2\pi}} \, dx
&amp;=&amp; \sqrt{ \left( \lint_{-\infty}^\infty \frac{e^{-\frac{(x-\mu)^2}{2\sigma^2}}}{\sigma\sqrt{2\pi}} \, dx \right)^2} \\
&amp;=&amp; \sqrt{ \lint_{-\infty}^\infty \frac{e^{-\frac{(x-\mu)^2}{2\sigma^2}}}{\sigma\sqrt{2\pi}} \, dx
\lint_{-\infty}^\infty \frac{e^{-\frac{(y-\mu)^2}{2\sigma^2}}}{\sigma\sqrt{2\pi}} \, dy} \\
&amp;=&amp; \sqrt{ \lint_{-\infty}^\infty \lint_{-\infty}^\infty \frac{e^{-\frac{(x-\mu)^2+(y-\mu)^2}{2\sigma^2}}}{\sigma^2 2\pi} \, dx \, dy}
\end{eqnarray*}

Substitute $x^\prime=x-\mu$ and $y^\prime=y-\mu$.  Since the bounds are infinite, they do not change, and $dx^\prime=dx$ and $dy^\prime=dy$.  Thus, we have
\begin{eqnarray*}
\sqrt{\lint_{-\infty}^\infty \lint_{-\infty}^\infty \frac{e^{-\frac{(x-\mu)^2+(y-\mu)^2}{2\sigma^2}}}{\sigma^2 2\pi} \, dx \, dy}
&amp;=&amp; \sqrt{\lint_{-\infty}^\infty \lint_{-\infty}^\infty \frac{e^{-\frac{(x^\prime)^2+(y^\prime)^2}{2\sigma^2}}}{\sigma^2 2\pi} \, dx^\prime \, dy^\prime}.
\end{eqnarray*}

Converting to polar coordinates, we obtain
\begin{eqnarray*}
\sqrt{\lint_{-\infty}^\infty \lint_{-\infty}^\infty \frac{e^{-\frac{(x^\prime)^2+(y^\prime)^2}{2\sigma^2}}}{\sigma^2 2\pi} \, dx^\prime \, dy^\prime}
&amp;=&amp; \sqrt{\lint_0^\infty \lint_0^{2\pi} \frac{re^{-\frac{r^2}{2\sigma^2}}}{\sigma^2 2\pi} \, dr \, d\theta} \\
&amp;=&amp; \sqrt{\lint_0^{2\pi} \frac{d\theta}{2\pi}} \sqrt{\lint_0^\infty \frac{re^{-\frac{r^2}{2\sigma^2}}}{\sigma^2} \, dr} \\
&amp;=&amp; \sqrt{\frac{\theta}{2\pi}\bigg|_0^{2\pi}} \sqrt{\frac{1}{\sigma^2}\lint_{0}^\infty r e^{-\frac{r^2}{2\sigma^2}} \, dr} \\
&amp;=&amp; \sqrt{\frac{2\pi}{2\pi}} \sqrt{\frac{\sigma^2}{\sigma^2}\left( -e^{-\frac{r^2}{2\sigma^2}} \right)\bigg|_0^\infty} \\
&amp;=&amp; \sqrt{1} \sqrt{1}\\
&amp;=&amp; 1.
\end{eqnarray*}</content>
</record>
