Ml. Smythe et al., THE MOLTEN HELIX - EFFECTS OF SOLVATION ON THE ALPHA-HELICAL TO 3(10)-HELICAL TRANSITION, Journal of the American Chemical Society, 117(20), 1995, pp. 5445-5452
Free energy surfaces, or potentials of mean force, for the alpha- to 3
(10)-helical conformational transition in polypeptides have been calcu
lated in several solvents of different dielectric. The alpha- to 3(10)
-helical transition has been suggested as potentially important in var
ious biological processes, including protein folding, formation of vol
tage-gated ion channels, kinetics of substrate binding in proteins, an
d signal transduction mechanisms. This study investigates the thermody
namics of the alpha- to 3(10)-helical transition of a model peptide, t
he capped decamer of alpha-methylalanine, in order to assess the plaus
ibility of this transition in the mechanisms of such biological proces
ses. The free energy surfaces indicate that in each environment studie
d the alpha-helical conformation is the more stable of the two for the
decapeptide, The thermodynamic data suggest that the alpha-helix is e
nergetically stabilized and the 3(10)-helix is entropically favored. T
he inclusion of dichloromethane, acetonitrile, or water results in app
roximately 7 kcal/mol of relative conformational energy (favoring the
alpha-helix) and 3 kcal/mol of relative conformational entropy (favori
ng the 3(10)-helix) in comparison to the gas phase. In polar environme
nts, the alpha-helix is stabilized by its more favorable salute-solven
t electrostatic interactions, and solute-solute steric interactions. I
n addition, it was concluded that in polar solvents, especially water,
it is possible for the peptide to reduce some of the inherent strain
of the 3(10)-helix by widening psi, the resulting weaker intrasolute h
ydrogen bonds being compensated for by increased-hydrogen bonding to t
he solvent. Lower polarity environments are associated with a marginal
ly increased relative stability of the 3(10)-helix, which we suggest i
s largely due to the additional intrahelical hydrogen bond of this con
formation. The data suggest that, in environments such as membranes, t
he interior of proteins or crystals, the complete transition from an c
t-helix to a 3(10)-helix for this decapeptide would require less than
6 kcal/mol in free energy. Switching conformations for individual resi
dues is much more facile, and shorter 3(10)-helices may actually be en
ergetically favored, at least, in nonpolar environments. This study pr
imarily estimates the backbone contribution to the helical transition;
side chain interactions would be expected to play a significant role
in stabilizing one conformer relative to the other. It is, therefore,
quite feasible that the alpha- to 3(10)-helical transition could provi
de a possible mechanism for many biological processes. While there are
many factors, such as helix length and side chain packing, that contr
ibute to the selection of either the alpha- or the 3(10)-helical confo
rmation or a mixture of the two, this study focuses primarily on one o
f these effects, that of the polarity of the environment.