From c4c0b06dd70555f7522d6eb163ea0f43d822617b Mon Sep 17 00:00:00 2001
From: wolf <wolf@0785d39b-7218-0410-832d-ea1e28bc413d>
Date: Fri, 2 May 2003 14:16:10 +0000
Subject: [PATCH] Appendix B was erroneously numbered Appendix A.

git-svn-id: https://svn.dealii.org/trunk@7546 0785d39b-7218-0410-832d-ea1e28bc413d
---
 deal.II/doc/reports/nedelec/nedelec.ps | 71 ++++++++++++++------------
 deal.II/doc/reports/nedelec/node1.html |  2 +-
 deal.II/doc/reports/nedelec/node6.html |  6 +--
 3 files changed, 42 insertions(+), 37 deletions(-)

diff --git a/deal.II/doc/reports/nedelec/nedelec.ps b/deal.II/doc/reports/nedelec/nedelec.ps
index 7ca06c5f8b..7d4dd9d8c8 100644
--- a/deal.II/doc/reports/nedelec/nedelec.ps
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@@ -2128,8 +2133,8 @@ TeXDict begin
 %%Page: 1 1
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+b(ed)m(\023)g(elec's)36 b(elemen)m(ts)h(of)h(\014rst)g(t)m(yp)s(e)1446
+933 y Fz(Anna)27 b(Sc)n(hneeb)r(eli,)h(Ma)n(y)f(2,)g(2003)28
 1223 y Fy(Abstract:)35 b Fz(The)23 b(aim)f(of)h(this)g(rep)r(ort)e(is)i
 (to)f(giv)n(e)g(an)h(in)n(tro)r(duction)f(to)g(N)n(\023)-39
 b(ed)n(\023)g(elec's)21 b Fx(H)7 b Fz(\(curl;)14 b(\012\)-conforming)21
@@ -2187,7 +2192,7 @@ b(The)29 b(b)r(oundary)g(condition)28 3825 y(\(2\))36
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+b(B.)28 4123 y(The)f(sub)5 b(ject)28 b(of)g(this)f(section)h(is)f(to)h
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 y(A)h(more)e(detailed)i(treatmen)n(t)f(of)h(the)g(follo)n(wing)e
@@ -7746,7 +7751,7 @@ Fm(on)h Fx(@)5 b Fz([)p Fs(\000)p Fz(1)p Fx(;)14 b Fz(1])3060
 4920 y(then)e Fx(')24 b Fz(=)e Fs(\000)p Fz(\001)p Fx(w)f
 Fz(+)d Fx(cw)r Fm(.)1949 5719 y Fk(22)p eop
 %%Page: 23 23
-23 22 bop 28 231 a Fw(A)134 b Fv(Time-harmonic)35 b(Maxw)m(ell's)i
+23 22 bop 28 231 a Fw(B)134 b Fv(Time-harmonic)35 b(Maxw)m(ell's)i
 (equations)h(with)e(lo)m(w-frequency)i(appro)m(ximation)28
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diff --git a/deal.II/doc/reports/nedelec/node1.html b/deal.II/doc/reports/nedelec/node1.html
index 169abda394..90e43cab6e 100644
--- a/deal.II/doc/reports/nedelec/node1.html
+++ b/deal.II/doc/reports/nedelec/node1.html
@@ -115,7 +115,7 @@ The coefficient <IMG
 <BR>
 This type of problem typically arises in particular settings of
 Maxwell`s equations. The boundary condition (<A HREF="node1.html#eq:_PCB">2</A>) then applies to a perfectly conducting boundary. 
-For a derivation of the model problem (<A HREF="node1.html#eq:model_problem">1</A>), refer to Appendix <A HREF="node6.html#appendix:_Maxwell_s_Eq.">A</A>.
+For a derivation of the model problem (<A HREF="node1.html#eq:model_problem">1</A>), refer to Appendix <A HREF="node6.html#appendix:_Maxwell_s_Eq.">B</A>.
 <BR></FONT>
 <P>
 <FONT SIZE="-1">The subject of this section is to give an appropriate setting for a variational formulation of (<A HREF="node1.html#eq:model_problem">1</A>).
diff --git a/deal.II/doc/reports/nedelec/node6.html b/deal.II/doc/reports/nedelec/node6.html
index 423df4c2fa..138058a02f 100644
--- a/deal.II/doc/reports/nedelec/node6.html
+++ b/deal.II/doc/reports/nedelec/node6.html
@@ -7,8 +7,8 @@ original version by:  Nikos Drakos, CBLU, University of Leeds
   Jens Lippmann, Marek Rouchal, Martin Wilck and others -->
 <HTML>
 <HEAD>
-<TITLE>A. Time-harmonic Maxwell's equations with low-frequency approximation</TITLE>
-<META NAME="description" CONTENT="A. Time-harmonic Maxwell's equations with low-frequency approximation">
+<TITLE>B. Time-harmonic Maxwell's equations with low-frequency approximation</TITLE>
+<META NAME="description" CONTENT="B. Time-harmonic Maxwell's equations with low-frequency approximation">
 <META NAME="keywords" CONTENT="main">
 <META NAME="resource-type" CONTENT="document">
 <META NAME="distribution" CONTENT="global">
@@ -35,7 +35,7 @@ original version by:  Nikos Drakos, CBLU, University of Leeds
 <H1><A NAME="SECTION00060000000000000000"></A> 
 <A NAME="appendix:_Maxwell_s_Eq."></A>
 <BR>
-A. <FONT SIZE="+1">Time-harmonic Maxwell's equations with low-frequency approximation</FONT>
+B. <FONT SIZE="+1">Time-harmonic Maxwell's equations with low-frequency approximation</FONT>
 </H1><FONT SIZE="-1">
 We show, how the model problem can be derived from the time-harmonic Maxwell's equations in the low-frequency case.
 We follow the outline of [<A
-- 
2.39.5