V. Aleksa et al., STUDY OF THE CONFORMERS OF DICHLOROMETHYLMETHYLDIFLUOROSILANE BY VIBRATIONAL SPECTROSCOPY AND AB-INITIO METHODS, Journal of Raman spectroscopy, 29(7), 1998, pp. 627-643
Dichloromethylmethyldifluorosilane (CHCl2SiF2CH3) was synthesized for
the first time. Raman spectra of the liquid were obtained at various t
emperatures between 298 and 163 K, Spectra of the amorphous solid were
recorded at 85 K and spectra of crystalline solids cooled by differen
t techniques were obtained. The infrared spectra were recorded of the
vapor and of the amorphous and crystalline states at liquid nitrogen t
emperature. Two different crystals were observed after careful anneali
ng of the amorphous solid to 202 K (crystal I) and 208 K (crystal II).
Both the Raman and infrared spectra of these crystals were different,
interpreted as different conformers being present in the two crystal
lattices. When the liquid was cooled, crystal II was invariably formed
, suggesting this crystal to be stable, whereas crystal I appeared to
be metastable, Additional infrared spectra were obtained of the compou
nd trapped in argon and nitrogen matrices at 5 and 15 K. The compound
exists in two different conformations (anti and gauche) due to restric
ted rotation of the -CHCl2 group. Approximately 32 of the infrared and
/or Raman bands present in the vapor and liquid vanished in one or oth
er of the two crystals formed, giving 18 pairs of bands each belonging
to one conformer. The remaining vibrational bands were present in bot
h crystals, suggesting overlapping bands of the anti and gauche confor
mers, Raman temperature studies gave an enthalpy difference Delta H(co
nf)degrees = 0 +/- 0.2 kJ mol(-1) between the conformers in the liquid
. The bands vanishing in the infrared matrix isolation spectra upon an
nealing to ca, 31-34 It suggested that the anti conformer had lower en
ergy than gauche in both argon and nitrogen matrices, and the conforma
tional barrier was estimated to be 6-7 kJ mol(-1). Ab initio calculati
ons at the HF/6-311G level gave optimized geometries, infrared and Ra
man intensities and vibrational wavenumbers for the anti and gauche co
nformers. An assignment of the vibrational spectra into anti and gauch
e conformers was carried out and reasonably good agreement was obtaine
d between the experimental and scaled ab initio calculated wavenumbers
for the two conformers. (C) 1998 John Wiley & Sons, Led.