CYANA Command: enoe spindiff: Difference between revisions

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== Parameters ==
== Parameters ==
; mode =''integer'': (default: ''1'')


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


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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''' 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  
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  
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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
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
The parameter '''b0field''' is the field strength [MHz].
The parameter '''tauc''' is the correlation time [s].
The parameter '''maxdist''' is the size of the spheres centered at spin i and j.
The parameter '''rmode''' is used to specify if experimental or simulated auto-relaxation (rho) values are used.

Revision as of 16:40, 17 January 2019

Parameters

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

Description

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

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

The parameter b0field is the field strength [MHz]. The parameter tauc is the correlation time [s]. The parameter maxdist is the size of the spheres centered at spin i and j.

The parameter rmode is used to specify if experimental or simulated auto-relaxation (rho) values are used.