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+<!DOCTYPE HTML PUBLIC "-//W3C//DTD HTML 3.2 Final//EN">
+
+<!--Converted with LaTeX2HTML 99.1 release (March 30, 1999)
+original version by: Nikos Drakos, CBLU, University of Leeds
+* revised and updated by: Marcus Hennecke, Ross Moore, Herb Swan
+* with significant contributions from:
+ Jens Lippmann, Marek Rouchal, Martin Wilck and others -->
+<HTML>
+<HEAD>
+<TITLE>sampleMath</TITLE>
+<META NAME="description" CONTENT="sampleMath">
+<META NAME="keywords" CONTENT="sampleMath">
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+
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+
+<LINK REL="next" HREF="node1.html">
+<LINK REL="next" HREF="node1.html">
+</HEAD>
+
+<BODY >
+<!--Navigation Panel-->
+<A NAME="tex2html9"
+ HREF="node1.html">
+<IMG WIDTH="37" HEIGHT="24" ALIGN="BOTTOM" BORDER="0" ALT="next"
+ SRC="/afs/cern.ch/project/tex/new/latex2html/icons.gif/next_motif.gif"></A>
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+ SRC="/afs/cern.ch/project/tex/new/latex2html/icons.gif/previous_motif_gr.gif">
+<BR>
+<B> Next:</B> <A NAME="tex2html10"
+ HREF="node1.html">About this document ...</A>
+<BR>
+<BR>
+<!--End of Navigation Panel-->
+<P>
+<H2 ALIGN="center"><A NAME="SECTION00000000000000000000">
+Math examples</A>
+</H2>
+<BR>
+<DIV ALIGN="CENTER"><A NAME="xiEmax"></A>
+
+<!-- MATH
+ \begin{eqnarray}
+\phi(\lambda) & = & \frac{1} {2 \pi i}\int^{c+i\infty}_{c-i\infty}
+ \exp \left( u \ln u + \lambda u \right ) du \hspace{1cm}\mbox{for } c \geq 0 \\
+ \lambda & = & \frac{\epsilon -\bar{\epsilon} }{\xi}
+ - \gamma' - \beta^2 - \ln \frac{\xi} {E_{\rm max}}\\
+ \gamma & = & 0.577215\dots \mathrm{\hspace{5mm}(Euler's\ constant)} \\
+ \gamma' & = & 0.422784\dots = 1 - \gamma \\
+ \epsilon , \bar{\epsilon} & = & \mbox{actual/average energy loss}
+\end{eqnarray}
+ -->
+
+<TABLE ALIGN="CENTER" CELLPADDING="0" WIDTH="100%">
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="35" HEIGHT="31" ALIGN="MIDDLE" BORDER="0"
+ SRC="img1.gif"
+ ALT="$\displaystyle \phi(\lambda)$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="325" HEIGHT="58" ALIGN="MIDDLE" BORDER="0"
+ SRC="img3.gif"
+ ALT="$\displaystyle \frac{1} {2 \pi i}\int^{c+i\infty}_{c-i\infty}
+\exp \left( u \ln u + \lambda u \right ) du \hspace{1cm}\mbox{for } c \geq 0$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(1)</TD></TR>
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="13" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img4.gif"
+ ALT="$\displaystyle \lambda$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="185" HEIGHT="51" ALIGN="MIDDLE" BORDER="0"
+ SRC="img5.gif"
+ ALT="$\displaystyle \frac{\epsilon -\bar{\epsilon} }{\xi}
+- \gamma' - \beta^2 - \ln \frac{\xi} {E_{\rm max}}$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(2)</TD></TR>
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="13" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img6.gif"
+ ALT="$\displaystyle \gamma$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="235" HEIGHT="33" ALIGN="MIDDLE" BORDER="0"
+ SRC="img7.gif"
+ ALT="$\displaystyle 0.577215\dots \mathrm{\hspace{5mm}(Euler's\ constant)}$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(3)</TD></TR>
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="18" HEIGHT="33" ALIGN="MIDDLE" BORDER="0"
+ SRC="img8.gif"
+ ALT="$\displaystyle \gamma'$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="143" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img9.gif"
+ ALT="$\displaystyle 0.422784\dots = 1 - \gamma$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(4)</TD></TR>
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="24" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img10.gif"
+ ALT="$\displaystyle \epsilon , \bar{\epsilon}$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="187" HEIGHT="31" ALIGN="MIDDLE" BORDER="0"
+ SRC="img11.gif"
+ ALT="$\displaystyle \mbox{actual/average energy loss}$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(5)</TD></TR>
+</TABLE></DIV>
+<BR CLEAR="ALL"><P></P>
+
+<P>
+Since&nbsp;<A HREF="sampleMath.html#xiEmax">2</A> and <A HREF="sampleMath.html#eqn:stress-sr">6</A> hold for arbitrary
+<!-- MATH
+ $\delta\mathbf{c}$
+ -->
+<IMG
+ WIDTH="20" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img12.gif"
+ ALT="$\delta\mathbf{c}$">-vectors,
+it is clear that
+<!-- MATH
+ $\mathcal{N}(A) = \mathcal{R}(B)$
+ -->
+<IMG
+ WIDTH="104" HEIGHT="31" ALIGN="MIDDLE" BORDER="0"
+ SRC="img13.gif"
+ ALT="$\mathcal{N}(A) = \mathcal{R}(B)$"> and that when <IMG
+ WIDTH="68" HEIGHT="31" ALIGN="MIDDLE" BORDER="0"
+ SRC="img14.gif"
+ ALT="$y=B(x)$"> one has...
+<BR>
+...the <A NAME="tex2html4"
+ HREF="http://www-groups.dcs.st-and.ac.uk/~history/Mathematicians/Pythagoras.html">Pythagorians</A> knew infinitely many solutions in integers to <IMG
+ WIDTH="88" HEIGHT="33" ALIGN="MIDDLE" BORDER="0"
+ SRC="img15.gif"
+ ALT="$a^2+b^2=c^2$">.
+That no non-trivial integer solutions exist for <IMG
+ WIDTH="93" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img16.gif"
+ ALT="$a^n+b^n=c^n$"> with integers <IMG
+ WIDTH="43" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img17.gif"
+ ALT="$n&gt;2$"> has long
+been suspected (<A NAME="tex2html5"
+ HREF="http://www-groups.dcs.st-and.ac.uk/~history/HistTopics/Fermat's_last_theorem.html">Fermat, c.1637</A>). Only during the current decade has this been proved (<A NAME="tex2html6"
+ HREF="http://www.pbs.org:80/wgbh/nova/proof">Wiles, 1995</A>).
+
+<P>
+<BR>
+<DIV ALIGN="CENTER"><A NAME="eqn:stress-sr"></A>
+
+<!-- MATH
+ \begin{eqnarray}
+V \mathbf{\pi}^{sr} & = & \left< \sum_i M_i \mathbf{V}_i \mathbf{V}_i
+ + \sum_i \sum_{j>i} \mathbf{R}_{ij} \mathbf{F}_{ij}\right> \\\nonumber
+ & = & \left< \sum_i M_i \mathbf{V}_i \mathbf{V}_i
+ + \sum_{i}\sum_{j>i}\sum_\alpha\sum_\beta \mathbf{r}_{i\alpha j\beta}\mathbf{f}_{i\alpha j\beta}
+ - \sum_i \sum_\alpha \mathbf{p}_{i\alpha} \mathbf{f}_{i\alpha} \right>
+\end{eqnarray}
+ -->
+
+<TABLE ALIGN="CENTER" CELLPADDING="0" WIDTH="100%">
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT"><IMG
+ WIDTH="40" HEIGHT="30" ALIGN="MIDDLE" BORDER="0"
+ SRC="img18.gif"
+ ALT="$\displaystyle V \mathbf{\pi}^{sr}$"></TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="233" HEIGHT="63" ALIGN="MIDDLE" BORDER="0"
+ SRC="img19.gif"
+ ALT="$\displaystyle \left&lt; \sum_i M_i \mathbf{V}_i \mathbf{V}_i
++ \sum_i \sum_{j&gt;i} \mathbf{R}_{ij} \mathbf{F}_{ij}\right&gt;$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+(6)</TD></TR>
+<TR VALIGN="MIDDLE"><TD NOWRAP ALIGN="RIGHT">&nbsp;</TD>
+<TD ALIGN="CENTER" NOWRAP><IMG
+ WIDTH="16" HEIGHT="28" ALIGN="MIDDLE" BORDER="0"
+ SRC="img2.gif"
+ ALT="$\textstyle =$"></TD>
+<TD ALIGN="LEFT" NOWRAP><IMG
+ WIDTH="418" HEIGHT="63" ALIGN="MIDDLE" BORDER="0"
+ SRC="img20.gif"
+ ALT="$\displaystyle \left&lt; \sum_i M_i \mathbf{V}_i \mathbf{V}_i
++ \sum_{i}\sum_{j&gt;i}\...
+... j\beta}
+- \sum_i \sum_\alpha \mathbf{p}_{i\alpha} \mathbf{f}_{i\alpha} \right&gt;$"></TD>
+<TD WIDTH=10 ALIGN="RIGHT">
+&nbsp;</TD></TR>
+</TABLE></DIV>
+<BR CLEAR="ALL"><P></P>
+<BR><HR>
+<!--Table of Child-Links-->
+<A NAME="CHILD_LINKS"><STRONG>Subsections</STRONG></A>
+
+<UL>
+<LI><A NAME="tex2html11"
+ HREF="node1.html">About this document ...</A>
+</UL>
+<!--End of Table of Child-Links-->
+<BR><HR>
+<ADDRESS>
+<I>Michel Goossens</I>
+<BR><I>1999-03-30</I>
+</ADDRESS>
+</BODY>
+</HTML>