Re: r23030 - /trunk/docs/latex/dispersion.tex -- May 07, 2014 - 10:30

There is also one "\nonumber" left that you may wish to remove in the
second equation block.  You may also need a "\nonumber" on the first
R2eff line for the multi-line equation to work.

Cheers,

Edward



On 7 May 2014 10:27, Edward d'Auvergne <edward@xxxxxxxxxxxxx> wrote:
> Hi Troels,
>
> One more LaTeX tip here ;)  If you change:
>
> +                     & - \frac{1}{T_{\textrm{rel}}}\ln{\left(
> \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2 \kAB p_D
> )\right)} \\
>
> to:
>
> +                     & \qquad - \frac{1}{T_{\textrm{rel}}}\ln{\left(
> \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2 \kAB p_D
> )\right)} \\
>
> see how that looks for you.  Or there is the phantom trick I added to
> http://wiki.nmr-relax.com/CR72 and http://wiki.nmr-relax.com/CR72_full
> pages 
> (http://wiki.nmr-relax.com/index.php?title=CR72&curid=300&diff=2403&oldid=2402
> and 
> http://wiki.nmr-relax.com/index.php?title=CR72_full&curid=317&diff=2404&oldid=2399).
>  In this case:
>
> +                     & \phantom{=} -
> \frac{1}{T_{\textrm{rel}}}\ln{\left( \frac{1+y}{2} +
> \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2 \kAB p_D )\right)} \\
>
> The formatting idea is that the multi-line maths should align to the
> right of the equal sign.
>
> Regards,
>
> Edward
>
>
>
> On 7 May 2014 10:14,  <tlinnet@xxxxxxxxxxxxx> wrote:
> > Author: tlinnet
> > Date: Wed May  7 10:14:09 2014
> > New Revision: 23030
> >
> > URL: http://svn.gna.org/viewcvs/relax?rev=23030&view=rev
> > Log:
> > Used LaTeX subequations instead, and using  R2eff parameter is defined in 
> > the relax.tex
> >
> > Using the defined \Rtwoeff, \RtwozeroA, \RtwozeroB, \kAB, \kBA, \kex.
> >
> > sr #3154: (https://gna.org/support/?3154) Implementation of Baldwin (2014) 
> > B14 model - 2-site exact solution model for all time scales.
> >
> > This follows the tutorial for adding relaxation dispersion models at:
> > http://wiki.nmr-relax.com/Tutorial_for_adding_relaxation_dispersion_models_to_relax#The_relax_manual
> >
> > 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=23030&r1=23029&r2=23030&view=diff
> > ==============================================================================
> > --- trunk/docs/latex/dispersion.tex     (original)
> > +++ trunk/docs/latex/dispersion.tex     Wed May  7 10:14:09 2014
> > @@ -565,21 +565,26 @@
> >  This is the model for 2-site exchange exact analytical derivation on all 
> > time scales (with the constraint that $\pA > \pB$), named after 
> > \citet{Baldwin2014}.
> >  It is selected by setting the model to `B14 full'.
> >  The equation is
> > -\begin{eqnarray}
> > -  R_{2,\textrm{eff}} & = & 
> > \frac{R_2^A+R_2^B+k_{\textrm{EX}}}{2}-\frac{N_{\textrm{CYC}}}{T_{\textrm{rel}}}\cosh{}^{-1}(v_{1c})
> >  \nonumber \\
> > -                     & - &  \frac{1}{T_{\textrm{rel}}}\ln{\left( 
> > \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2k_{\textrm{AB}}p_D 
> > )\right)} \nonumber \\
> > -    & = & R_{2,\textrm{eff}}^{\textrm{CR72}} - 
> > \frac{1}{T_{\textrm{rel}}}\ln{\left( \frac{1+y}{2} + 
> > \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2k_{\textrm{AB}}p_D )\right)} ,
> > -\end{eqnarray}
> > +\begin{subequations}
> > +\begin{align}
> > +  \Rtwoeff & = \frac{\RtwozeroA + \RtwozeroB + \kex }{2}-\frac{ 
> > N_{\textrm{CYC}} }{ T_{\textrm{rel}} } \cosh{}^{-1}(v_{1c}) \\
> > +                     & - \frac{1}{T_{\textrm{rel}}}\ln{\left( 
> > \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2 \kAB p_D )\right)} 
> > \\
> > +    & = \Rtwoeff^{\textrm{CR72}} - \frac{1}{T_{\textrm{rel}}}\ln{\left( 
> > \frac{1+y}{2} + \frac{1-y}{2\sqrt{v_{1c}^2-1}}(v_2 + 2\kAB p_D )\right)} ,
> > +\end{align}
> > +\end{subequations}
> > +
> >
> >  where
> > -\begin{eqnarray}
> > -    v_{1c} & = & 
> > F_0\cosh{\left(\tau_{\textrm{CP}}E_0\right)}-F_2\cosh{\left(\tau_{\textrm{CP}}E_2\right)}
> >  \nonumber \\
> > -    v_{1s} & = & 
> > F_0\sinh{\left(\tau_{\textrm{CP}}E_0\right)}-F_2\sinh{\left(\tau_{\textrm{CP}}E_2\right)}
> >  \nonumber \\
> > -    v_{2}N & = & v_{1s}\left(O_B-O_A\right)+4O_B F_1^a 
> > \sinh{\left(\tau_{\textrm{CP}}E_1\right)} \nonumber \\
> > -    p_D N & = & v_{1s} + 
> > \left(F_1^a+F_1^b\right)\sinh{\left(\tau_{\textrm{CP}}E_1\right)} 
> > \nonumber \\
> > -    v_3 & = & \left( v_2^2 + 4 k_{\textrm{BA}} k_{\textrm{AB}} p_D^2 
> > \right)^{1/2} \nonumber \\
> > -    y & = & \left( \frac{v_{1c}-v_3}{v_{1c}+v_3} 
> > \right)^{N_{\textrm{CYC}}}
> > -\end{eqnarray}
> > +\begin{subequations}
> > +\begin{align}
> > +    v_{1c} & = 
> > F_0\cosh{\left(\tau_{\textrm{CP}}E_0\right)}-F_2\cosh{\left(\tau_{\textrm{CP}}E_2\right)}
> >  \\
> > +    v_{1s} & = 
> > F_0\sinh{\left(\tau_{\textrm{CP}}E_0\right)}-F_2\sinh{\left(\tau_{\textrm{CP}}E_2\right)}
> >   \\
> > +    v_{2}N & = v_{1s}\left(O_B-O_A\right)+4O_B F_1^a 
> > \sinh{\left(\tau_{\textrm{CP}}E_1\right)} \nonumber \\
> > +    p_D N & = v_{1s} + 
> > \left(F_1^a+F_1^b\right)\sinh{\left(\tau_{\textrm{CP}}E_1\right)} \\
> > +    v_3 & = \left( v_2^2 + 4 \kBA \kAB p_D^2 \right)^{1/2} \\
> > +    y & = \left( \frac{v_{1c}-v_3}{v_{1c}+v_3} \right)^{N_{\textrm{CYC}}}
> > +\end{align}
> > +\end{subequations}
> >
> >  The advantage of this code will be that you will always get the right 
> > answer provided you got 2-site exchange, in-phase magnetisation and 
> > on-resonance pulses.
> >
> >
> >
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> >
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