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Conformational analysis of the type II and type III collagen α-1 chain N-telopeptides by 1H-NMR spectroscopy and restrained molecular mechanics calculations
Authors:Albin Otter  Paul G Scott  George Kotovych
Abstract:The type II and type III collagen α-1 chain N-telopeptides are a nonadecamer with the sequence pEMAGGFDEKAGGAQLGVMQ-NH2 and a tetradecamer with the sequence pEYEAYDVKSGVAGG-NH2, respectively. Their conformations have been studied in CD3OH/H2O (60/40) solution by means of two-dimensional proton nmr spectroscopy. Based on double quantum filtered correlation spectroscopy, total correlation spectroscopy, rotating frame nuclear Overhauser enhancement (ROE) spectroscopy, and nuclear Over-hauser enhancement (NOE) spectroscopy experiments, all resonances were assigned and the conformational properties were analyzed in terms of vicinal NH-Hα coupling constants, sequential and medium-range NOEs (ROEs), and amide proton temperature coefficients. The NOE distance constraints as well as dihedral constraints based on the vicinal NH-Hα coupling constants were used as input parameters for restrained molecular mechanics, consisting of restrained molecular dynamics and restrained energy minimization calculations. The type II N-telopeptide's conformation is dominated by a fused βγ-turn between Phe6 and Ala10, stabilized by three hydrogen bonds and a salt bridge between the side-chain end groups of Glu8 and Lys9. The first 5 amino acids are extended with a much higher degree of conformational freedom. The 2 Gly residues following the turns were found to be highly flexible (hinge-like), leaving the spatial position of the second half of the molecule relative to the fused βγ-turn undefined. In the type III telopeptide, a series of sequential NH(i)-NH(i + 1) ROEs were observed between the amino acids Tyr2 and Ser9, indicating that a fraction of the conformational space is helical. However, the absence of medium-range ROEs and the lack of regularity of the effects associated with α-helices suggest the presence of a nascent rather than a complete helix. © 1993 John Wiley & Sons, Inc.
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