Contribution of hydrogen bonds to equilibrium alpha beta transition of resorcinol

Citation
M. Yoshino et al., Contribution of hydrogen bonds to equilibrium alpha beta transition of resorcinol, J PHYS CH A, 103(15), 1999, pp. 2775-2783
Citations number
18
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF PHYSICAL CHEMISTRY A
ISSN journal
10895639 → ACNP
Volume
103
Issue
15
Year of publication
1999
Pages
2775 - 2783
Database
ISI
SICI code
1089-5639(19990415)103:15<2775:COHBTE>2.0.ZU;2-M
Abstract
The equilibrium alpha beta transition temperature, T-alpha beta, between th e alpha crystalline phase and the beta crystalline phase of resorcinol has been determined when both supercooling and superheating effects vanished. T he latent volume and dT(alpha beta)/dP have been determined by use of a pre cision pycnometer, and the thermodynamic characteristics of the alpha beta transition are presented. The P-V-T relations of each phase have also been obtained. All of the thermal expansion coefficient, the isothermal compress ibility, and the internal pressure for the higher-temperature, higher-densi ty polymorph, the beta crystal, are much larger than those for the lower-te mperature, lower-density polymorph, the a crystal. Contributions of the hyd rogen bonds and the van der Waals energy to the internal energy have semiqu antitatively been analyzed by use of a simple potential model. When the a c rystal transforms to the beta crystal, the energy of hydrogen bonds decreas es due to the breakdown of the hydrogen bonds, whereas the van der Waals en ergy increases with the contraction in volume. Since the latter cancels the most of the former, we observe the small latent heat. The breakdown of the hydrogen bonds induces a significant change in the potential depths of the covalent structure O-H ... O and ionic, proton-transferred structure O-... H-O+ in each hydrogen bond. In consequence, the distribution of the proton s between the covalent structure and the ionic structure changes with the t ransition. The increase in the entropy produced from the redistribution of the protons is the same order of magnitude as the latent entropy.