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Liaison Hydrogene en Phase Liquide et Spectrometrie Raman. I: Alcools liquides purs
Author(s) -
Perchard C.,
Perchard J. P.
Publication year - 1975
Publication title -
journal of raman spectroscopy
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.748
H-Index - 110
eISSN - 1097-4555
pISSN - 0377-0486
DOI - 10.1002/jrs.1250030216
Subject(s) - chemistry , polarizability , intensity (physics) , analytical chemistry (journal) , depolarization ratio , atmospheric temperature range , phase (matter) , raman spectroscopy , melting point , thermodynamics , molecule , physics , organic chemistry , optics , aerosol
Abstract The v OH (OD) bands of some liquid alcohols (three primary, two secondary and one tertiary), have been studied over a wide temperature range with regard to: (i) band position as a function of temperature, (ii) band intensity and depolarization ratio as a function of temperature and physical state. From studies of (i), the long chain polymer structure is confirmed; and the diagonal and interaction force constants F OH and ƒ OH are calcualated between 295 K and the melting point. From studies of (ii), it is shown that the intensity in the liquid phase is temperature independent as long as autoassociation is preponderant: however from relative intensity measurements (gas to liquid) the scattering activity \documentclass{article}\pagestyle{empty}\begin{document}$ \left({45\bar \alpha ^{'2} + 7{\rm \gamma}^{{\rm '2}}} \right) $\end{document} is seen to increase by a factor of two as a result of autoassociation; and the depolarization ratio increases by a factor of two from dilute solution to pure liquid. These results are discussed in the light of the bond polarizability theory; it is concluded that the α′ l /α′ p ratio for the OH band changes considerably on formation of an hydrogen bond. This can be explained in terms of the Orville Thomas pulsed cloud model.