THEORETICAL-STUDY OF THE LOW-BARRIER HYDROGEN-BOND IN THE HYDROGEN MALEATE ANION IN THE GAS-PHASE - COMPARISON WITH NORMAL HYDROGEN-BONDS

Citation
M. Garciaviloca et al., THEORETICAL-STUDY OF THE LOW-BARRIER HYDROGEN-BOND IN THE HYDROGEN MALEATE ANION IN THE GAS-PHASE - COMPARISON WITH NORMAL HYDROGEN-BONDS, Journal of the American Chemical Society, 119(5), 1997, pp. 1081-1086
Citations number
42
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
119
Issue
5
Year of publication
1997
Pages
1081 - 1086
Database
ISI
SICI code
0002-7863(1997)119:5<1081:TOTLHI>2.0.ZU;2-G
Abstract
Relative strengths of normal and low-barrier hydrogen bonds (LBHBs) in the gas phase were analyzed by means of quantum-mechanical and thermo dynamic calculations on the mesaconic/citraconic and several maleic/fu maric cis/trans isomerization equilibria. All geometries were fully op timized with correlation effects included via second-order Moller-Ples set perturbation theory. The cis isomer of the maleic monoanion (also known as hydrogen maleate) is greatly stabilized in the gas phase owin g to the formation of an intramolecular low-barrier hydrogen bond more than 20 kcal/mol stronger, in free energy terms, than the correspondi ng normal intramolecular hydrogen bond in maleic diacid. The very shor t internuclear distance (2.41 Angstrom) obtained at the MP2 level betw een the hydrogen donor and the hydrogen acceptor in hydrogen maleate, as well as the high value of the NMR chemical shift for the participat ing proton, are two other characteristics experimentally attributed to the formation of an LBHB. The transition state structure for proton e xchange in the maleic monoanion is symmetrical. In this structure, the interactions of the central hydrogen atom with the acceptor and the d onor atoms are classified as covalent by Bader's theory of molecular s tructure. In any case, our calculations indicate that the zero-point e nergy for maleate monoanion is above the energy barrier for proton tra nsfer. This fact allows free motion of the hydrogen atom lying on the ground vibrational state in accordance with the single symmetrical min imum experimentally predicted in nonpolar solvents.