P rotonation energetics of the naturally occurring amino acids (AA) is of current interest because of the importance of proton transfer (PT) reactions in biological systems [1]. Recently, the PAs of amino acids, small peptides, and their derivatives have been successfully used [2][3][4][5][6][7] to explain some fragment ion abundance relationships in the low-energy tandem mass spectra of protonated peptides. Considering appropriate PAs, one can often predict whether the N-or the C-terminal fragment remains charged upon dissociation of the respective parent ions [2]. These predictions require, however, good quality PA data for the fragments involved.The literature on the protonation chemistry of AAs and small peptides was reviewed by Harrison [8] who introduced the recently available, most consistent gasphase basicity (GB) and proton affinity (PA) scales for AAs. Harrison used the following strategy [8] to compile his list. First, he critically evaluated the available literature data on gas-phase basicities of AAs since most of the existing experimental techniques address primarily GBs and not PAs. Then eq 1,was used to convert GBs to PAs applying appropriate ⌬S values. Here, T is the temperature and ⌬S is the protonation entropy. The protonation entropy can be represented as a sum of three terms, involving entropy changes caused by loss of translational (⌬S trans ), rotational (⌬S rot ), and vibrational (⌬S vib ) degrees of freedom, whereby the ⌬S vib term is usually neglected (for more details, see reference [8]). Direct assessment of ⌬S is possible only if the GBs are determined from variable-temperature equilibrium measurements [8]. Such studies have been performed only for Gly, Ala, and Pro; the results suggest that the ⌬S term is dominated by the loss of translational entropy of the free proton for these AAs (⌬S Ϸ ⌬S trans ; ⌬S rot Ϸ 0) [9]. In other words, for those amino acids for which no extra strong H-bond is introduced in the protonated species, ⌬S resulting from changes of the rotational degrees of freedom is negligible (⌬S rot Ϸ 0). The term ⌬S trans can be readily approximated by the Sackur-Tetrode equation (for details see reference [8]), which gives T⌬S trans of Ϫ7.8 kcal mol Ϫ1 for T ϭ 298 K. The ⌬S rot Ϸ 0 approximation is definitely not valid for AAs containing strongly basic side chains like Lys or Arg, for which a strong intramolecular H-bond is introduced in the protonated species (for example, ϪH 2 N ϩ ϪH. . .NH 2 Ϫ for protonated Lys). These strong hydrogen bonds freeze rotational degrees of freedom in the protonated species that can be considered free in the neutral molecules, thus leading to a negative rotational entropy (⌬S rot Ͻ 0). The magnitude of ⌬S rot for AAs is mostly approximated by considering similar molecules for which data from variable temperature equilibrium experiments are available. For example, Harrison approximated ⌬S rot (Lys) using ⌬S rot (1,5-. Unfortunately, no experimental or theoretical information on ⌬S rot for Arg, Gln, Asn, etc. is available. Harrison assume...