CYANA Command: enoe spindiff: Difference between revisions

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; b0field =''real'': (default: ''none'')
; b0field =''real'': (default: ''none'')
; tauc =''real'': (default: ''none'')
; tauc =''real'': (default: ''none'')
; maxdist =''real'': (default: ''none'')
; maxdist =''real'': (default: ''6.5A'')
; mode =''integer'': (default: ''1'')
; mode =''integer'': (default: ''1'')
; rmode =''integer'': (default: ''1'')
; rmode =''integer'': (default: ''1'')
Line 12: Line 12:
This command performs the spin diffusion calculations within the eNORA routine.
This command performs the spin diffusion calculations within the eNORA routine.


The parameter '''b0field'''
The parameter '''b0field''' is the field strength [MHz].
The parameter '''tauc''' is the correlation time [s].
The parameter '''maxdist''' is the correlation time [Angstroem].


There are two different approaches to determine spin-diffusion contributions to cross-peak buildups, both of which require PDB coordinates of a previously determined structure (a conventional NMR structure or an X-ray structure):
The parameter '''rmode'''


For the full-matrix (FRM) approach to spin-diffusion approximation we use the multi-spin Solomon equation to express the mixing time-dependence of the NOESY intensities. In the FRM approach, the buildup intensities containing spin-diffusion are calculated for all spins within the spheres centered at spins i and j (Orts et al. 2012).
There are two different approaches to determine spin-diffusion contributions to cross-peak buildups, both of which require PDB coordinates of a previously determined structure (a conventional NMR structure or an X-ray structure). Usually the lowest energy model of structure bundles is used for spin-diffusion calculation; however, averaging of spin-diffusion over individual conformers is possible, depending on how many structures were read, see


The parameter '''mode''' is used to select the spin diffusion correction method (FRM:1, TSS: 2).
For the full-matrix (FRM, mode=1) approach to spin-diffusion approximation we use the multi-spin Solomon equation to express the mixing time-dependence of the NOESY intensities. In the FRM approach, the buildup intensities containing spin-diffusion are calculated for all spins within the spheres centered at spins i and j (Orts et al. 2012).


In the TSS approach, we follow a strategy in which spin-diffusion contributions are obtained from the summed contributions of the exact solutions of three-spin systems ijk (Vögeli et al. 2010) for all neighboring spins k within the cross section of the spheres centered at spin i and j. Importantly, scaling the contribution to spin-diffusion from spin k by its protonation level allows the setting of individual, spin specific deuteration levels in sample specific manner corresponding i.e. to methyl-group specific labeling schemes, see


 
In the TSS (TSS, mode=2) approach, we follow a strategy in which spin-diffusion contributions are obtained from the summed contributions of the exact solutions of three-spin systems ijk (Vögeli et al. 2010) for all neighboring spins k within the cross section of the spheres centered at spin i and j. Importantly, scaling the contribution to spin-diffusion from spin k by its protonation level allows the setting of individual, spin specific deuteration levels in sample specific manner corresponding i.e. to methyl-group specific labeling schemes, see
 
 
 
Usually the lowest energy model of structure bundles is used for spin-diffusion calculation; however, averaging of spin-diffusion over individual conformers is possible.

Revision as of 15:37, 17 January 2019

Parameters

b0field =real
(default: none)
tauc =real
(default: none)
maxdist =real
(default: 6.5A)
mode =integer
(default: 1)
rmode =integer
(default: 1)

Description

This command performs the spin diffusion calculations within the eNORA routine.

The parameter b0field is the field strength [MHz]. The parameter tauc is the correlation time [s]. The parameter maxdist is the correlation time [Angstroem].

The parameter rmode

There are two different approaches to determine spin-diffusion contributions to cross-peak buildups, both of which require PDB coordinates of a previously determined structure (a conventional NMR structure or an X-ray structure). Usually the lowest energy model of structure bundles is used for spin-diffusion calculation; however, averaging of spin-diffusion over individual conformers is possible, depending on how many structures were read, see

The parameter mode is used to select the spin diffusion correction method (FRM:1, TSS: 2). For the full-matrix (FRM, mode=1) approach to spin-diffusion approximation we use the multi-spin Solomon equation to express the mixing time-dependence of the NOESY intensities. In the FRM approach, the buildup intensities containing spin-diffusion are calculated for all spins within the spheres centered at spins i and j (Orts et al. 2012).


In the TSS (TSS, mode=2) approach, we follow a strategy in which spin-diffusion contributions are obtained from the summed contributions of the exact solutions of three-spin systems ijk (Vögeli et al. 2010) for all neighboring spins k within the cross section of the spheres centered at spin i and j. Importantly, scaling the contribution to spin-diffusion from spin k by its protonation level allows the setting of individual, spin specific deuteration levels in sample specific manner corresponding i.e. to methyl-group specific labeling schemes, see