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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

Figure 5.

Figure 5.

Correlation plots of experimental and back-predicted dipolar CCR rates based on four GB3 models. RDD(HNN)/DD(CβHβ) + RDD(HNCβ)/DD(NHβ) is abbreviated by R. The theoretical rates are calculated under the assumption of isotropic (red squares) and anisotropic overall tumbling (blue diamonds). The structural models are: RDC-refined X-ray structure 2OED[99], where the HN and Hα proton positions were subsequently re-optimized with RDCs[72,100] (top left); an eight-state ensemble calculated from RDCs, J couplings, 15N relaxation order parameters and crystallographic B-factors[103] (bottom left); single-state structures (top right) and four-state ensembles both from eNOEs, RDCs and J couplings[106,107] (bottom right). The most extreme outliers are indicated with red residue numbers, where i/j designate the residues of the HN-N and Hβ-Cβ vectors. The black lines indicate a slope of 1. Reprinted by permission from John Wiley and Sons: R.B. Fenwick, B. Vögeli, Detection of correlated protein backbone and side-chain angle fluctuations, ChemBioChem, 2017, 18, 2016–2021, copyright 2017.