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Experimentally based model of a complex between a snake toxin and the α7 nicotinic receptor

Authors :
Carole Fruchart-Gaillard
Pierre-Jean Corringer
Bernard Gilquin
Stéphanie Antil-Delbeke
André Ménez
Jean-Pierre Changeux
Denis Servent
Nicolas Le Novère
Toru Tamiya
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)
Récepteurs et Cognition (RC)
Collège de France (CdF (institution))-Institut Pasteur [Paris]-Centre National de la Recherche Scientifique (CNRS)
Sophia University [Tokyo]
We thank Morgane Boutillon for technical assistance in the cycle-mutant experiments, Isabelle Krimm for help preparing the structural figures, and Pascal Kessler and Thomas Grutter for fruitful discussions.
Collège de France (CdF (institution))-Institut Pasteur [Paris] (IP)-Centre National de la Recherche Scientifique (CNRS)
Source :
Proceedings of the National Academy of Sciences of the United States of America, Proceedings of the National Academy of Sciences of the United States of America, National Academy of Sciences, 2002, 99 (5), pp.3216-3221. ⟨10.1073/pnas.042699899⟩, Proceedings of the National Academy of Sciences of the United States of America, 2002, 99 (5), pp.3216-3221. ⟨10.1073/pnas.042699899⟩
Publication Year :
2002
Publisher :
Proceedings of the National Academy of Sciences, 2002.

Abstract

To understand how snake neurotoxins interact with nicotinic acetylcholine receptors, we have elaborated an experimentally based model of the α–cobratoxin–α7 receptor complex. This model was achieved by using ( i ) a three-dimensional model of the α7 extracellular domain derived from the crystallographic structure of the homologous acetylcholine-binding protein, ( ii ) the previously solved x-ray structure of the toxin, and ( iii ) nine pairs of residues identified by cycle-mutant experiments to make contacts between the α-cobratoxin and α7 receptor. Because the receptor loop F occludes entrance of the toxin binding pocket, we submitted this loop to a dynamics simulation and selected a conformation that allowed the toxin to reach its binding site. The three-dimensional structure of the toxin–receptor complex model was validated a posteriori by an additional double-mutant experiment. The model shows that the toxin interacts perpendicularly to the receptor axis, in an equatorial position of the extracellular domain. The tip of the toxin central loop plugs into the receptor between two subunits, just below the functional receptor loop C, the C-terminal tail of the toxin making adjacent additional interactions at the receptor surface. The receptor establishes major contacts with the toxin by its loop C, which is assisted by principal (loops A and B) and complementary (loops D, F, and 1) functional regions. This model explains the antagonistic properties of the toxin toward the neuronal receptor and opens the way to the design of new antagonists.

Details

ISSN :
10916490 and 00278424
Volume :
99
Database :
OpenAIRE
Journal :
Proceedings of the National Academy of Sciences
Accession number :
edsair.doi.dedup.....2e33f29aafe2ed9e326ce0e9081163d5
Full Text :
https://doi.org/10.1073/pnas.042699899