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. Author manuscript; available in PMC: 2022 Jun 19.
Published in final edited form as: Chemphyschem. 2018 Sep 3;20(2):178–196. doi: 10.1002/cphc.201800602

Table 3.

Validation of ensembles and single structures with CCR and 3J coupling data.

structure CCR rate r.m.s.d. [s−1] a 3J coupling r.m.s.d. [s−1] b
HNN/HNN CαHα/CαHα HNN/CαHα CαHα/HNN HN-Hα C’-C’ HN-C’ HN-Cβ
Single structures
2OEDc 1.12 4.71 1.68 1.67 0.98 0.41 0.44 1.07
CCR1d 0.65 4.11 0.98 1.23 0.87 0.62 0.63 1.12
Ensembles
ENS8e 0.78 3.99 1.61 1.28 0.75 0.33 0.40 1.02
CCR16d 0.15 2.02 0.25 0.29 0.55 0.25 0.39 0.72
a

Bond lengths of 1.041 and 1.117 Å were used to calculate CCRs from structures to account for libration motions not present in static structures

b

Karplus parameters used were those for the fits to Ace-Ala-NMe,[111] experimental data[112,113]

c

Coordinates from RDC-refined X-ray structure,[99] where HN and Hα proton positions were subsequently optimized with RDCs[72,100]

d

Ensemble generated using the CCR data and both 6 sets of HN-N and Hα-Cα RDCs[72,100]

e

Previously determined dynamic ensemble[103]