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Evolution of protein interfaces in multimers and fibrils
A majority of cellular proteins function as part of multimeric complexes of two or more subunits. Multimer formation requires interactions between protein surfaces that lead to closed structures, such as dimers and tetramers. If proteins interact in an open-ended way, uncontrolled growth of fibrils...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
AIP Publishing LLC
2019
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6561775/ https://www.ncbi.nlm.nih.gov/pubmed/31202237 http://dx.doi.org/10.1063/1.5086042 |
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author | Zabel, W. Jeffrey Hagner, Kyle P. Livesey, Benjamin J. Marsh, Joseph A. Setayeshgar, Sima Lynch, Michael Higgs, Paul G. |
author_facet | Zabel, W. Jeffrey Hagner, Kyle P. Livesey, Benjamin J. Marsh, Joseph A. Setayeshgar, Sima Lynch, Michael Higgs, Paul G. |
author_sort | Zabel, W. Jeffrey |
collection | PubMed |
description | A majority of cellular proteins function as part of multimeric complexes of two or more subunits. Multimer formation requires interactions between protein surfaces that lead to closed structures, such as dimers and tetramers. If proteins interact in an open-ended way, uncontrolled growth of fibrils can occur, which is likely to be detrimental in most cases. We present a statistical physics model that allows aggregation of proteins as either closed dimers or open fibrils of all lengths. We use pairwise amino-acid contact energies to calculate the energies of interacting protein surfaces. The probabilities of all possible aggregate configurations can be calculated for any given sequence of surface amino acids. We link the statistical physics model to a population genetics model that describes the evolution of the surface residues. When proteins evolve neutrally, without selection for or against multimer formation, we find that a majority of proteins remain as monomers at moderate concentrations, but strong dimer-forming or fibril-forming sequences are also possible. If selection is applied in favor of dimers or in favor of fibrils, then it is easy to select either dimer-forming or fibril-forming sequences. It is also possible to select for oriented fibrils with protein subunits all aligned in the same direction. We measure the propensities of amino acids to occur at interfaces relative to noninteracting surfaces and show that the propensities in our model are strongly correlated with those that have been measured in real protein structures. We also show that there are significant differences between amino acid frequencies at isologous and heterologous interfaces in our model, and we observe that similar effects occur in real protein structures. |
format | Online Article Text |
id | pubmed-6561775 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | AIP Publishing LLC |
record_format | MEDLINE/PubMed |
spelling | pubmed-65617752019-06-20 Evolution of protein interfaces in multimers and fibrils Zabel, W. Jeffrey Hagner, Kyle P. Livesey, Benjamin J. Marsh, Joseph A. Setayeshgar, Sima Lynch, Michael Higgs, Paul G. J Chem Phys ARTICLES A majority of cellular proteins function as part of multimeric complexes of two or more subunits. Multimer formation requires interactions between protein surfaces that lead to closed structures, such as dimers and tetramers. If proteins interact in an open-ended way, uncontrolled growth of fibrils can occur, which is likely to be detrimental in most cases. We present a statistical physics model that allows aggregation of proteins as either closed dimers or open fibrils of all lengths. We use pairwise amino-acid contact energies to calculate the energies of interacting protein surfaces. The probabilities of all possible aggregate configurations can be calculated for any given sequence of surface amino acids. We link the statistical physics model to a population genetics model that describes the evolution of the surface residues. When proteins evolve neutrally, without selection for or against multimer formation, we find that a majority of proteins remain as monomers at moderate concentrations, but strong dimer-forming or fibril-forming sequences are also possible. If selection is applied in favor of dimers or in favor of fibrils, then it is easy to select either dimer-forming or fibril-forming sequences. It is also possible to select for oriented fibrils with protein subunits all aligned in the same direction. We measure the propensities of amino acids to occur at interfaces relative to noninteracting surfaces and show that the propensities in our model are strongly correlated with those that have been measured in real protein structures. We also show that there are significant differences between amino acid frequencies at isologous and heterologous interfaces in our model, and we observe that similar effects occur in real protein structures. AIP Publishing LLC 2019-06-14 2019-06-12 /pmc/articles/PMC6561775/ /pubmed/31202237 http://dx.doi.org/10.1063/1.5086042 Text en © 2019 Author(s). 0021-9606/2019/150(22)/225102/12/$0.00 All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | ARTICLES Zabel, W. Jeffrey Hagner, Kyle P. Livesey, Benjamin J. Marsh, Joseph A. Setayeshgar, Sima Lynch, Michael Higgs, Paul G. Evolution of protein interfaces in multimers and fibrils |
title | Evolution of protein interfaces in multimers and fibrils |
title_full | Evolution of protein interfaces in multimers and fibrils |
title_fullStr | Evolution of protein interfaces in multimers and fibrils |
title_full_unstemmed | Evolution of protein interfaces in multimers and fibrils |
title_short | Evolution of protein interfaces in multimers and fibrils |
title_sort | evolution of protein interfaces in multimers and fibrils |
topic | ARTICLES |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6561775/ https://www.ncbi.nlm.nih.gov/pubmed/31202237 http://dx.doi.org/10.1063/1.5086042 |
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