We study atomic models of the thermodynamics of the structural transition of peptides that form ␣-helices. The effect of sequence variation on ␣-helix formation for alanine-rich peptides, Ac-Ala21-methyl amide (A21) and Ac-A5 (AAARA)3A-methyl amide (Fs peptide), is investigated by atomic simulation studies of the thermodynamics of the helix-coil transition in explicit water. The simulations show that the guanidinium group in the Arg side chains in the Fs peptide interacts with the carbonyl group four amino acids upstream in the chain and desolvates backbone hydrogen bonds. This desolvation can be directly correlated with a higher probability of hydrogen bond formation. We find that Fs has higher helical content than A21 at all temperatures. A small modification in the AMBER force field reproduces the experimental helical content and helix-coil transition temperatures for the Fs peptide.D etailed all-atom molecular simulation of protein folding has been limited by the inadequacy of sampling and possible inaccuracies of the semiempirical force fields used in classical simulations. The development of techniques for efficient sampling and the refinement of semiempirical force fields are crucial for modeling protein folding, structure prediction, and complex formation. Small peptides have many of the complexities associated with the energy landscape of proteins (1) and are ideal systems to understand the role of competing interactions in determining protein structures. In this work, we study the thermodynamics of the helix-coil transition of short peptides for which ample experimental data exist. We use highly parallel algorithms that enable the efficient sampling of configurational space. We validate our results through comparison with experimental data and test the sensitivity of our results to small changes in the semiempirical force field.The elucidation of ␣-helical formation energetics is relevant for understanding protein folding mechanisms. In spite of the large number of experimental studies conducted in peptides, there is still much debate concerning the propensity of Ala residues to stabilize ␣-helices. Ingwall et al. (2) studied runs of Ala n , with n ϭ 10-1,000, flanked by Lys runs, and concluded that short (n ϳ 10) sequences of Ala peptides do not form helices in water (2, 3). Similar conclusions were drawn from studies of Ala-rich random sequences. However, short (13-21) Ala-rich peptides containing interior charged amino acid side chains are found to form helices with 70-90% helical content (4-7), and short runs of Ala n (n ϭ 13) flanked by two ornithine charged amino acid are found to be about 40% helical in water (8, 9). These data have been interpreted in terms of a large intrinsic propensity of Ala residues to form helices in water. Within the Lifson-Roig (10, 11) and Zimm-Bragg (12) models for the helix-coil transition, the intrinsic propensity of an amino acid to form a helix is a measure of the interactions of the amino acid with its own and nearest-neighbor amino acid backbone (11, 13). Theore...