Amyloids are fibrillary aggregates identified in over 40 human diseases, including
neurodegenerative diseases encompassing Alzheimer’s (AD), Parkinson’s (PD),
Huntington’s and Prion diseases. Amyloids form by spontaneous self-assembly of
monomeric precursor peptides known as intrinsically disordered proteins (IDPs).
Experiments suggest that soluble low molecular weight oligomers formed in the early
stages of assembly are toxic, and hence, most promising drug targets. However,
experiments are insufficient to characterize oligomers due to their inherent polymorphic
and short-lived nature. This thesis advances our mechanistic understanding of the
formation of amyloid oligomers by delineating signature features of IDP monomers and
‘profibrillar’ oligomers through predictive computational modelling techniques
employing atomic resolution molecular dynamics (MD) computer simulations. We
additionally predict the assembly of non-aggregating low molecular weight oligomers.
We first probe the molecular signatures of experimentally indicative non-aggregating
folded a-helical conformers, and aggregation-prone partially folded a-helices of
amyloid-b42 (Ab42) and a-synuclein (aS) IDPs implicated in AD and PD, respectively
across a broad spectrum of physical models. We predict a common intra-peptide route to
helix stabilization, showing that the terminal groups (N-terminal or NTR in Ab42 and C terminal or CTR in aS) frequently indulge in hydrophobic interactions with the central
hydrophobic domains (CHDs) and secondary salt bridges with other domains. Lack of
such short-range contacts during complete helix unfolding coupled with destabilized
helices in terminal-deleted variants confer the aggregation protective role by terminal
groups in folded helical conformers. Further, we reveal a shared feature of dynamic
coupling between the partially folded helical regions of the CHD and the charged terminal
ends (NTR in Ab42 and CTR in aS). Absence of such intra-peptide modulation in
helically folded and unfolded states confer long-range allosteric regulation of the CHD
by the termini that may render the partially folded helical states prone to initial
oligomerization. Next, we design structural assemblies of experimentally uncharacterized
aggregation-resistant low-weight aS tetramer. We model a de novo broken a-helical
tetramer by reconstructing loop motif that optimizes packing of aS helical monomers.
We show that monomers attain activated conformations during tetramer assembly, and
familial missense mutations double the energy barrier to tetramerization, thus preserving
the pool of aggregation-prone disordered monomers, and confirming the experimentally
observed low tetramer:monomer ratios with mutants. In order to investigate the effect of
helical continuity and periodicity, we model a de novo extended 11/3-helical tetramer.
Broken a-helical tetramers show a more favourable assembly than the extended 11/3-
helical tetramers, the ease of their interconversions diminishing with homologous E → K
mutations. Additionally, rationally designing a series of broken a-helical multimers from
dimers to octamers shows that tetramers have lowest activation energy, providing a
rationale for the experimental observation that tetramers are the most populated
oligomers. Finally, we investigate the molecular determinants of higher aggregation rate
of Ab42 over Ab40 by simulating their profibrillar oligomers (dodecamers) on graphene water interface. Our data reveals that Ab dodecamers may facilitate a single layer growth
along the graphene surface, with Ab42 presenting a more closed conformation with
possibilities of unidirectional growth in Ab40, but not in Ab42. Oligomer height profiles
on graphene indicate that dodecamers may be formed post mature fibril formation