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Introduction: Elucidation of the structure of PrPSc has opened the possibility to understand propagation of PrPSc (PrPSc-templated conversion of PrPC to PrPSc) at the atomistic level. However, PrPSc offers a flat, “dull” templating surface with little templating capability. Therefore, the folded domain (FD) of PrPC must unfold and stretch before it can be accommodated on the PrPSc surface.
Objectives: We modelled the very early steps of PrPC unfolding once its flexible N-terminal 90-120 domain has easily attached to the PrPSc surface and adopted the PrPSc conformation.
Methods: We used Molecular Dynamics simulations at 310 K and 400 K in explicit water of a molecular system consisting of a PrPSc tetramer and a PrPC(90-231) monomer with its 90-120 tail attached to it and having adoped the PrPSc conformation. Similar simulations of free PrPC(90-231) were also carried out.
Results/Discussion: The FD of PrPC(90-231) with its tail attached to PrPSc proved to be remarkably stable through 300 ns simulations. Even at 400 K it maintained its global fold and its 3 alpha-helices remained unscathed. Conformational fluctuations only affected significantly its internal coils and short β-strands. The N-terminal tail remained attached and the FD bounced into the PrPSc surface. In contrast, unfolding events were more conspicuous throughout simulations of free PrPC(90-231).
Conclusion: Our results highlight the “procrustean” predicament of PrPSc propagation, with a relatively stable FD facing a flat, relatively inert template. They also point to the relatively more flexible 121-143 N-terminal segment of the FD as a likely initiator of unfolding/refolding during conversion.
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