Author: bugman Date: Fri May 9 12:58:37 2014 New Revision: 23130 URL: http://svn.gna.org/viewcvs/relax?rev=23130&view=rev Log: Shifted the model-free model equations for the HTML manual to the subequations environment. This is for the relax manual at http://www.nmr-relax.com/manual/index.html This is to preserve the equation numbering so that the HTML and PDF equation numbers match as closely as possible. Modified: trunk/docs/latex/model-free.tex Modified: trunk/docs/latex/model-free.tex URL: http://svn.gna.org/viewcvs/relax/trunk/docs/latex/model-free.tex?rev=23130&r1=23129&r2=23130&view=diff ============================================================================== --- trunk/docs/latex/model-free.tex (original) +++ trunk/docs/latex/model-free.tex Fri May 9 12:58:37 2014 @@ -297,18 +297,20 @@ \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} +\begin{subequations} +\begin{align} + 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{align} +\end{subequations} \end{htmlonly} \noindent The parameter $R_{ex}$ is scaled quadratically with field strength in these models as it is assumed to be fast. @@ -334,18 +336,20 @@ \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} +\begin{subequations} +\begin{align} + 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{align} +\end{subequations} \end{htmlonly}