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. 2013 Jul 31;8(7):e70521.
doi: 10.1371/journal.pone.0070521. Print 2013.

Conformational stability of fibrillar amyloid-beta oligomers via protofilament pair formation - a systematic computational study

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Conformational stability of fibrillar amyloid-beta oligomers via protofilament pair formation - a systematic computational study

Anna Kahler et al. PLoS One. .

Abstract

Amyloid-[Formula: see text] (A[Formula: see text]) oligomers play a crucial role in Alzheimer's disease due to their neurotoxic aggregation properties. Fibrillar A[Formula: see text] oligomerization can lead to protofilaments and protofilament pairs via oligomer elongation and oligomer association, respectively. Small fibrillar oligomers adopt the protofilament topology, whereas fibrils contain at least protofilament pairs. To date, the underlying growth mechanism from oligomers to the mature fibril still remains to be elucidated. Here, we performed all-atom molecular dynamics simulations in explicit solvent on single layer-like protofilaments and fibril-like protofilament pairs of different size ranging from the tetramer to the 48-mer. We found that the initial U-shaped topology per monomer is maintained over time in all oligomers. The observed deviations of protofilaments from the starting structure increase significantly with size due to the twisting of the in-register parallel [Formula: see text]-sheets. This twist causes long protofilaments to be unstable and leads to a breakage. Protofilament pairs, which are stabilized by a hydrophobic interface, exhibit more fibril-like properties such as the overall structure and the twist angle. Thus, they can act as stable conformational templates for further fibril growth. Key properties like the twist angle, shape complementarity, and energetics show a size-dependent behavior so that small oligomers favor the protofilament topology, whereas large oligomers favor the protofilament pair topology. The region for this conformational transition is at the size of approximately twelve A[Formula: see text] monomers. From that, we propose the following growth mechanism from A[Formula: see text] oligomers to fibrils: (1) elongation of short protofilaments; (2) breakage of large protofilaments; (3) formation of short protofilament pairs; and (4) elongation of protofilament pairs.

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Conflict of interest statement

Competing Interests: HS serves as an academic editor for PLOS ONE. This does not alter the authors’ adherence to all the PLOS ONE policies on sharing data and materials.

Figures

Figure 1
Figure 1. Presentation of the system and explanation of calculations.
(A) The orientation of sidechains in the protofilament monomer with the salt bridge between residues D23 (red) and K28 (blue), and residue M35 (yellow) of the C-terminus pointing towards the surrounding solvent. (B) The 4-mer (Oformula image) as an example for the orientation of peptide chains within the protofilaments. (C) The interaction between hydrophobic residues around M35 (yellow) in the C-termini of two opposite protofilaments constitutes the interface in the protofilament pairs. (D) The 8-mer (Oformula image) as an example for the orientation of peptide chains in the protofilament pairs. (E) Two different angles were analyzed, the twist angle and the angle between adjacent monomers. (F) Two oligomers can either be combined to form a longer protofilament (elongation) or be merged via C-terminal contacts to form a protofilament pair (thickening). Therefore, two types of MM/GBSA calculations were performed: segmentation of protofilaments along the red plane and segmentation of protofilament pairs along the blue plane.
Figure 2
Figure 2. Rmsd values and twist angle for a small, medium,and large protofilament and its corresponding protofilament pair.
The rmsd values for the protofilaments (A) increase significantly with size of Aformula image oligomers. Upon formation of the C-terminal interface leading to protofilament pairs (B), the rmsd shows no difference between the small, medium or large system. Parallel in-register formula image-sheets reveal a general twist along the growth axis. The twist angle increases with size in the protofilaments (C) and is the reason for the rather high rmsd values (A). Upon formation of the C-terminal interface leading to protofilament pairs (D), the twist angle remains stable over time, indicating that addition of a second layer counteracts twisting of parallel formula image-sheets.
Figure 3
Figure 3. Final structures of the simulations of a small, medium, and large protofilament and its corresponding protofilament pair.
(A) The protofilament tetramer (O4) reveals a large twist angle and a flexible hinge region in the C-terminus. (B) The protofilament pair octamer (O2×4) shows a similar twist angle to the Oformula image, but the hydrophobic residues in the C-terminus are covered by the second layer. (C) The protofilament hexamer (Oformula image) displays the large twist of the parallel formula image-sheets. (D) The protofilament pair dodecamer (Oformula image) has a smaller twist angle than the protofilament hexamer due to the conteracting stabilization by the C-terminal interaction. (E) The protofilament 24-mer (Oformula image) shows a small angle between adjacent monomers but the large overall twist angle. (F) The protofilament pair 48-mer (Oformula image) shows that the overall twist angle is reduced upon C-terminal interaction.
Figure 4
Figure 4. Stability of -sheets in the protofilament pair 8-mer (O).
(A) Chains A and E are the terminal chains in growth-direction, chains D and H are the terminal chains on the other end of the oligomer; each chain consists of 35 residues. (B) Mean content of parallel formula image-sheets. N-terminal and C-terminal formula image-sheet of each monomer are separated by a turn region. See Figures S13–S22 in File SI for the results of all other oligomers.
Figure 5
Figure 5. Hydration of oligomers along the salt bridges between D23 and K28.
(A) Salt bridges along the 10-mer (Oformula image), the side chains of D23 and K28 are depicted as red and blue sticks, respectively. (B) Visualization of the water channel in the protofilament 12-mer (Oformula image, 50 ns); main entrance channel (green) and channel exits through neighboring turns (red).
Figure 6
Figure 6. Interaction energy analysis of the protofilaments and protofilament pairs from the 8-mer to the 48-mer.
The MM/GBSA interaction energy of the protofilament pairs decreases significantly with size, whereas longer protofilaments become increasingly unstable. Formation of protofilament pairs over formation of longer protofilaments becomes favored for oligomers consisting of 12 monomers. Further elongation of protofilaments increases instability.
Figure 7
Figure 7. Breakage of the protofilament 24-mer (O) and 48-mer (O).
Final snapshots of the MD simulation after 50 ns show that the overtwisting of parallel formula image-sheets initiates a breakage into oligomers of smaller size. Breakage points in the 24-mer (A) and the 48-mer (B) are indicated with red arrows.
Figure 8
Figure 8. Model for the growth mechanism of fibrillar oligomers.
Elongation of protofilaments and thickening to protofilament pairs can occur in the following steps: (1) aggregation of monomers forming small protofilaments; (2) and (3) elongation of protofilaments along the longitudinal growth axis; (4) fragmentation of large protofilaments into small protofilaments; (5) merging of two small protofilaments leading to a small protofilament pair; (6) addition of monomers elongating small protofilament pairs; (7) merging of two medium protofilaments leading to a medium protofilament pair; (8) addition of monomers elongating medium protofilament pairs; and (9) downstream aggregation of Aformula image via elongation of large protofilament pairs to fibrils and plaques.

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