The amide III region of the peptide infrared and Raman spectra has been used to determine the relative populations of the three major backbone conformations (P II , β, and α R ) in 19 amino acid dipeptides. The results provide a benchmark for force field or other methods of predicting backbone conformations in flexible peptides. There are three resolvable backbone bands in the amide III region. The major population is either P II or β for all dipeptides except Gly, whereas the α R population is measurable but always minor (≤10%) for 18 dipeptides. (The Gly φ,ψ map is complex and so is the interpretation of the amide III bands of Gly.) There are substantial differences in the relative β and P II populations among the 19 dipeptides. The band frequencies have been assigned as P II , 1,317-1,306 cm −1 ; α R , 1,304-1,294 cm −1 ; and β, 1,294-1,270 cm −1 . The three bands were measured by both attenuated total reflection spectroscopy and by Raman spectroscopy. Consistent results, both for band frequency and relative population, were obtained by both spectroscopic methods. The β and P II bands were assigned from the dependence of the 3 JðH N ,H α Þ coupling constant (known for all 19 dipeptides) on the relative β population. The P II band assignment agrees with one made earlier from Raman optical activity data. The temperature dependences of the relative β and P II populations fit the standard model with Boltzmann-weighted energies for alanine and leucine between 30 and 60°C.vibrational spectroscopy | backbone conformations | spectral populations | aqueous solution A basic unsolved problem in protein folding is making accurate calculations of the folding energetics of flexible peptides. Accurate experimental results for the major backbone conformations are needed to test prediction methods. Even the simple problem of calculating the φ,ψ map of the alanine dipeptide is beyond the reach of standard force fields used in molecular dynamics simulations (1). There are two probable reasons: one is that the energy differences between the major backbone conformations are small, and the second is that standard force fields contain so many parameters that errors cannot be found readily by comparing simulations with experimental results. The ability to calculate accurately the relative energies of the various backbone conformations is needed for simulating early stages of the protein folding process, which is an important current problem in molecular biophysics.When simulated by standard force fields, the φ,ψ map of the alanine dipeptide has three major conformational basins, P II , β, and α R . Different force fields agree on this point but give widely varying results for the populations in the three basins (1). The φ,ψ maps of the 19 amino acid residues (Pro excluded) from the protein structure database show the same three basins and are similar in outline for the various residues if data for Gly and Pre-Pro are excluded in addition to Pro (2). The three basins are centered approximately at P II (−75°, 145°), β (−120°, 120°), a...