The dynamics and spectroscopy of N-methyl-acetamide (NMA) and trialanine in solution is characterized from molecular dynamics (MD) simulations using different energy functions, including a conventional point charge (PC)-based force field, one based on a multipolar (MTP) representation of the electrostatics, and a semiempirical DFT method. For the 1-d infrared spectra, the frequency splitting between the two amide-I groups is 10 cm −1 from the PC, 13 cm −1 from the MTP, and 47 cm −1 from SCC-DFTB simulations, compared with 25 cm −1 from experiment. The frequency trajectory required for determining the frequency fluctuation correlation function (FFCF) is determined from individual (INM) and full normal mode (FNM) analyses of the amide-I vibrations. The spectroscopy, time-zero magnitude of the FFCF C(t = 0), and the static component ∆ 2 0 from simulations using MTP and analysis based on FNM are all consistent with experiments for (Ala) 3 . Contrary to that, for the analysis excluding mode-mode coupling (INM) the FFCF decays to zero too rapidly and for simulations with a PC-based force field the ∆ 2 0 is too small by a factor of two compared with experiments. Simulations with SCC-DFTB agree better with experiment for these observables than those from PC-based simulations. The conformational ensemble sampled from simulations using PCs is consistent with the literature (including P II , β, α R , and α L ), whereas that covered by the MTP-based simulations is dominated by P II with some contributions from β, α R . This agrees with and confirms recently reported, Bayesian-refined populations based on 1-dimensional infrared experiments. Full normal mode analysis together with a MTP representation provides a meaningful model to correctly describe the dynamics of hydrated trialanine.