Just for reference, the correct link here is
http://wiki.nmr-relax.com/Tutorial_for_adding_relaxation_dispersion_models_to_relax#The_relax_library.

Regards,

Edward



On 2 May 2014 11:57,  <[email protected]> wrote:
> Author: tlinnet
> Date: Fri May  2 11:57:07 2014
> New Revision: 22918
>
> URL: http://svn.gna.org/viewcvs/relax?rev=22918&view=rev
> Log:
> Python API documentation corrections for the model B14.
>
> 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#Adding_the_model_to_the_list";
>
> The B14 model is explained in: http://wiki.nmr-relax.com/B14.
>
> Modified:
>     trunk/lib/dispersion/b14.py
>
> Modified: trunk/lib/dispersion/b14.py
> URL: 
> http://svn.gna.org/viewcvs/relax/trunk/lib/dispersion/b14.py?rev=22918&r1=22917&r2=22918&view=diff
> ==============================================================================
> --- trunk/lib/dispersion/b14.py (original)
> +++ trunk/lib/dispersion/b14.py Fri May  2 11:57:07 2014
> @@ -41,6 +41,7 @@
>  =========
>
>  The equation used is::
> +
>              R2A0 + R2B0 + kex      Ncyc                      1      ( 1+y    
>         1-y                          )
>      R2eff = ------------------ -  ------ * cosh^-1 * v1c - ------ ln( --- + 
> ------------------ * (v2 + 2*kAB*pD ) )
>                    2                Trel                     Trel    (  2    
> 2*sqrt(v1c^2 -1 )                     )
> @@ -50,6 +51,7 @@
>                             Trel    (  2    2*sqrt(v1c^2 -1 )                 
>     )
>
>  Which have these following definitions::
> +
>      v1c = F0 * cosh(tauCP * E0)- F2 * cosh(tauCP * E2)
>      v1s = F0 * sinh(tauCP * E0)- F2 * sinh(tauCP * E2)
>      v2*N = v1s * (OB-OA) + 4OB * F1^a * sinh(tauCP * E1)
> @@ -57,23 +59,20 @@
>      v3 = ( v2^2 + 4 * kBA * kAB * pD^2 )^1/2
>      y = ( (v1c-v3)/(v1c+v3) )^NCYC
>
> -Note, E2 is complex. If |x| denotes the complex modulus:<br>
> +Note, E2 is complex. If |x| denotes the complex modulus::
> +
>      cosh(tauCP * E2) = cos(tauCP * |E2|)
>      sinh(tauCP * E2) = i sin(tauCP * |E2|)
>
>  The term pD is based on product of the off diagonal elements in the CPMG 
> propagator (Supplementary Section 3).
>
> -It is interesting to consider the region of validity of the Carver Richards 
> result.
> -The two results are equal when the correction is zero, which is true when
> +It is interesting to consider the region of validity of the Carver Richards 
> result.  The two results are equal when the correction is zero, which is true 
> when::
>
>      sqrt(v1c^2-1) ~ v2 + 2*kAB * pD
>
> -This occurs when 2*kAB * pD tends to zero, and so v2=v3.
> -Setting "kAB * pD" to zero, amounts to neglecting magnetisation that starts 
> on the ground state ensemble and end on the excited state ensemble and vice 
> versa.
> -This will be a good approximation when pA >> p_B.
> +This occurs when 2*kAB * pD tends to zero, and so v2=v3.  Setting "kAB * pD" 
> to zero, amounts to neglecting magnetisation that starts on the ground state 
> ensemble and end on the excited state ensemble and vice versa.  This will be 
> a good approximation when pA >> p_B.
>
> -In practise, significant deviations from the Carver Richards equation can be 
> incurred if pB > 1 %.
> -Incorporation of the correction term into equation (50), results in an 
> improved description of the CPMG experiment over the Carver Richards equation.
> +In practise, significant deviations from the Carver Richards equation can be 
> incurred if pB > 1 %.  Incorporation of the correction term into equation 
> (50), results in an improved description of the CPMG experiment over the 
> Carver Richards equation.
>
>  kex is the chemical exchange rate constant, pA and pB are the populations of 
> states A and B, and delta_omega is the chemical shift difference between the 
> two states in ppm.
>
>
>
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