r22957 - /trunk/docs/latex/dispersion.tex -- May 05, 2014 - 14:08

Author: bugman
Date: Mon May  5 14:08:44 2014
New Revision: 22957

URL: http://svn.gna.org/viewcvs/relax?rev=22957&view=rev
Log:
Expanded the 'CR72 full' dispersion model description in the manual to 
explain its origin.

This was discussed at 
http://thread.gmane.org/gmane.science.nmr.relax.devel/5410.

The equations used the Davis et al., 1994 simplified form, and this is now 
explained.


Modified:
    trunk/docs/latex/dispersion.tex

Modified: trunk/docs/latex/dispersion.tex
URL: 
http://svn.gna.org/viewcvs/relax/trunk/docs/latex/dispersion.tex?rev=22957&r1=22956&r2=22957&view=diff
==============================================================================
--- trunk/docs/latex/dispersion.tex     (original)
+++ trunk/docs/latex/dispersion.tex     Mon May  5 14:08:44 2014
@@ -431,6 +431,8 @@
     \Psi     &= \left( \RtwozeroA - \RtwozeroB - \pA\kex + \pB\kex \right)^2 
- \dw^2 + 4\pA\pB\kex^2 , \\
     \zeta    &= 2\dw \left( \RtwozeroA - \RtwozeroB - \pA\kex + \pB\kex 
\right).
 \end{align}
+
+Note that these equations use the numerically simplified form derived in the 
appendix of \citet{Davis94}.
 
 This model is not accurate when the motional process is very slow.
 In that case, the `TSMFK01' model in Section~\ref{sect: dispersion: TSMFK01 
model} on page~\pageref{sect: dispersion: TSMFK01 model} should be used 
instead.