Folding of Polyalanine into Helical Hairpins

Structure and mechanism of maximum stability of isolated alpha-helical protein domains at a critical length scale

The stability of alpha helices is important in protein folding, bioinspired materials design, and controls many biological properties under physiological and disease conditions. Here we show that a naturally favored alpha helix length of 9 to 17 amino acids exists at which the propensity towards the formation of this secondary structure is maximized. We use a combination of thermodynamical analysis, well-tempered metadynamics molecular simulation and statistical analyses of experimental alpha helix length distributions and find that the favored alpha helix length is caused by a competition between alpha helix folding, unfolding into a random coil and formation of higher-order tertiary structures. The theoretical result is suggested to be used to explain the statistical distribution of the length of alpha helices observed in natural protein structures. Our study provides mechanistic insight into fundamental controlling parameters in alpha helix structure formation and potentially other biopolymers or synthetic materials. The result advances our fundamental understanding of size effects in the stability of protein structures and may enable the design of de novo alpha-helical protein materials.

Molecular dynamics simulations of the folding of poly(alanine) peptides

The secondary structures and the shapes of long-chain polyalanine (PA) molecules were investigated by all-atom molecular dynamics simulations using a modified Amber force field. Homopolymers of polyaminoacids such as PA are convenient models to study the mechanism of protein folding. It was found that the conformational structures of PA peptides are highly sensitive to the chain length. In the absence of solvent, straight α-helices dominate in short (n ∼ 20) peptides at room temperature. A shape transition occurs at a chain length n of 40-45; the compact helix-turn-helix structure (the double-leg hairpin) becomes favored over a straight α-helix. For n=60, double-leg and the triple-leg hairpins are the only structures present in PA molecules. An exploration of a chain organization in a cubic cavity revealed a clear predisposition of PA molecules for additional breaks in α-helices and the formation of multifolded hairpins. Furthermore, under confinement the hairpin structure becomes much looser, the antiparallel positions of helical stems are disturbed, and a sizeable proportion of the helical stems are transformed from α-helices into 3(10)-helices.