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Optimization of the methods for small peptide solution structure determination by NMR spectroscopy

NMR spectroscopy was recognized as a method of protein structure determination in solution. However, determination of the conformation of small peptides, which undergo fast molecular motions, remains a challenge. This is mainly caused by the impossibility to collect the required quantity of the dist...

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Bibliographic Details
Published in:Molecular biology (New York) 2010-12, Vol.44 (6), p.958-967
Main Authors: Istrate, A. N, Mantsyzov, A. B, Kozin, S. A, Polshakov, V. I
Format: Article
Language:English
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Summary:NMR spectroscopy was recognized as a method of protein structure determination in solution. However, determination of the conformation of small peptides, which undergo fast molecular motions, remains a challenge. This is mainly caused by the impossibility to collect the required quantity of the distance and dihedral angle restraints from NMR spectra. At the same time, short charged peptides play an important role in a number of biological processes, in particular in pathogenesis of neurodegenerative diseases including Alzheimer's disease. Therefore, development of a method for structure simulation of small peptides in aqueous environment using the most realistic force fields seems to be of current importance. Such algorithm has been developed using the Amber-03 force field and Gromacs program after modification of its code. Calculation algorithm has been verified on a model peptide with a known solution structure and a metal-binding fragment of rat β-amyloid, whose structure has been determined by alternative methods. The developed algorithm substantially increases structure quality, in particular Ramachandran plot statistics, and decreases RMSD of atomic coordinates inside the calculated family. The described protocol can be used for determination of conformation of short peptides, and also for optimization of structure of larger proteins containing poorly structured fragments.
ISSN:0026-8933
1608-3245
DOI:10.1134/S0026893310060130