r23066 - in /trunk/docs/latex: dispersion.tex model-free.tex -- May 07, 2014 - 18:37

Author: bugman
Date: Wed May  7 18:37:57 2014
New Revision: 23066

URL: http://svn.gna.org/viewcvs/relax?rev=23066&view=rev
Log:
Fixes for the HTML version of the relax manual.

The renewal of the \theequation command in the model-free and relaxation 
dispersion chapters was
causing all equation numbers in latex2html to be broken.  By placing these in 
a latexonly
environment, the problem is avoided in the HTML version at 
www.nmr-relax.com/manual/.


Modified:
    trunk/docs/latex/dispersion.tex
    trunk/docs/latex/model-free.tex

Modified: trunk/docs/latex/dispersion.tex
URL: 
http://svn.gna.org/viewcvs/relax/trunk/docs/latex/dispersion.tex?rev=23066&r1=23065&r2=23066&view=diff
==============================================================================
--- trunk/docs/latex/dispersion.tex     (original)
+++ trunk/docs/latex/dispersion.tex     Wed May  7 18:37:57 2014
@@ -708,6 +708,7 @@
 See the 
\module{lib\pysep{}dispersion\pysep{}ns\pyus{}cpmg\pyus{}2site\pyus{}expanded}
 module for more details including the original code.
 Further simplifications can be found in the code.
 
+\begin{latexonly}
 \begin{subequations}
 \renewcommand{\theequation}{\theparentequation .\arabic{equation}}
 \begin{align}
@@ -769,6 +770,7 @@
             & \qquad \qquad                   + (t_{120} t_{122} - t_{116} 
t_{120}) t_{113} t_{118} t_{127} \kAB \Big].
 \end{align}
 \end{subequations}
+\end{latexonly}
 
 The relative peak intensities, magnetisation, and effective $\Rtwo$ 
relaxation rate are calculated as
 \begin{subequations}

Modified: trunk/docs/latex/model-free.tex
URL: 
http://svn.gna.org/viewcvs/relax/trunk/docs/latex/model-free.tex?rev=23066&r1=23065&r2=23066&view=diff
==============================================================================
--- trunk/docs/latex/model-free.tex     (original)
+++ trunk/docs/latex/model-free.tex     Wed May  7 18:37:57 2014
@@ -278,6 +278,7 @@
 \subsection{The model-free models}
 
 Extending the list of models given in \citet{Mandel95, Fushman97, 
Orekhov99b, Korzhnev01, Zhuravleva04}, the models built into relax include
+\begin{latexonly}
 \begin{subequations}
 \renewcommand{\theequation}{\theparentequation .\arabic{equation}}
 \addtocounter{equation}{-1}
@@ -294,11 +295,27 @@
  m9 &= \{R_{ex}\}.                             \label{model: m9}
 \end{align}
 \end{subequations}
+\end{latexonly}
+\begin{htmlonly}
+\begin{eqnarray}
+ m0 &= \{\},                                   \label{model: m0} \\
+ m1 &= \{S^2\},                                \label{model: m1} \\
+ m2 &= \{S^2, \tau_e\},                        \label{model: m2} \\
+ m3 &= \{S^2, R_{ex}\},                        \label{model: m3} \\
+ m4 &= \{S^2, \tau_e, R_{ex}\},                \label{model: m4} \\
+ m5 &= \{S^2, S^2_f, \tau_s\},                 \label{model: m5} \\
+ m6 &= \{S^2, \tau_f, S^2_f, \tau_s\},         \label{model: m6} \\
+ m7 &= \{S^2, S^2_f, \tau_s, R_{ex}\},         \label{model: m7} \\
+ m8 &= \{S^2, \tau_f, S^2_f, \tau_s, R_{ex}\}, \label{model: m8} \\
+ m9 &= \{R_{ex}\}.                             \label{model: m9}
+\end{eqnarray}
+\end{htmlonly}
 
 \noindent The parameter $R_{ex}$ is scaled quadratically with field strength 
in these models as it is assumed to be fast.
 In the set theory notation, the model-free model for the spin system $i$ is 
represented by the symbol $\Mfset_i$.
 Through the addition of the local $\tau_m$ to each of these models, only the 
component of Brownian rotational diffusion experienced by the spin system is 
probed.
 These models, represented in set notation by the symbol $\Localset_i$, are
+\begin{latexonly}
 \begin{subequations}
 \renewcommand{\theequation}{\theparentequation .\arabic{equation}}
 \addtocounter{equation}{-1}
@@ -315,6 +332,21 @@
  tm9 &= \{\tau_m, R_{ex}\}.                             \label{model: tm9}
 \end{align}
 \end{subequations}
+\end{latexonly}
+\begin{htmlonly}
+\begin{eqnarray}
+ tm0 &=& \{\tau_m\},                                     \label{model: tm0} 
\\
+ tm1 &=& \{\tau_m, S^2\},                                \label{model: tm1} 
\\
+ tm2 &=& \{\tau_m, S^2, \tau_e\},                        \label{model: tm2} 
\\
+ tm3 &=& \{\tau_m, S^2, R_{ex}\},                        \label{model: tm3} 
\\
+ tm4 &=& \{\tau_m, S^2, \tau_e, R_{ex}\},                \label{model: tm4} 
\\
+ tm5 &=& \{\tau_m, S^2, S^2_f, \tau_s\},                 \label{model: tm5} 
\\
+ tm6 &=& \{\tau_m, S^2, \tau_f, S^2_f, \tau_s\},         \label{model: tm6} 
\\
+ tm7 &=& \{\tau_m, S^2, S^2_f, \tau_s, R_{ex}\},         \label{model: tm7} 
\\
+ tm8 &=& \{\tau_m, S^2, \tau_f, S^2_f, \tau_s, R_{ex}\}, \label{model: tm8} 
\\
+ tm9 &=& \{\tau_m, R_{ex}\}.                             \label{model: tm9}
+\end{eqnarray}
+\end{htmlonly}