The experimental finding that α-synuclein (αS) occurs physiologically as a helically folded tetramer begs the question: why
are helical tetramers the most populated multimers? While the helical tetramer is known to resist aggregation, the
assembly mechanism of αS peptides remains largely unknown. By rationally designing a series of helical multimers from
dimer to octamer, we characterized the free energy landscape of wild-type and mutated multimers using molecular
dynamics computer simulations. Competition between supramolecular packing and solvation results in well-hydrated
dimers and trimers, and more screened pentamers to octamers, with the helical tetramer possessing the most balanced
structure with the lowest activation energy. Our data suggest that familial mutants are very sensitive to alterations in
monomer packing that would in turn raise the energy barriers for multimerization. Finally, the hypothesis that the αS
tetramer forms a soluble, benign “dead end” to circumvent aggregation is supported by its computed very weak
association with negatively charged cell membranes.
History
Publication
Physical Chemistry Chemical Physics;21, pp. 12036-12043