ON THE PLANARITY OF STYRENE AND ITS DERIVATIVES - THE MOLECULAR-STRUCTURES OF STYRENE AND (Z)-BETA-BROMOSTYRENE AS DETERMINED BY AB-INITIO CALCULATIONS AND GAS-PHASE ELECTRON-DIFFRACTION
Jc. Cochran et al., ON THE PLANARITY OF STYRENE AND ITS DERIVATIVES - THE MOLECULAR-STRUCTURES OF STYRENE AND (Z)-BETA-BROMOSTYRENE AS DETERMINED BY AB-INITIO CALCULATIONS AND GAS-PHASE ELECTRON-DIFFRACTION, Journal of molecular structure, 413, 1997, pp. 313-326
The molecular structures of styrene and (Z)-beta-bromostyrene have bee
n studied in the pas phase at nozzle temperatures of 303 and 338 K res
pectively. For both molecules the electron diffraction data were consi
stent with the results from ab initio calculations which described the
vinyl torsional motion, near the planar configurations, in terms of a
double minimum potential function with barriers of 243 cal mol(-1) (s
tyrene) and 430 cal mol(-1) (bromostyrene) at the planar form, and wit
h the minimum energy forms 27 degrees (styrene) and 39 degrees (bromos
tyrene) away, The perpendicular barriers were calculated to 2.73 kcal
mol(-1) (styrene) and 1.10 kcal mol(-1) (bromostyrene). The important
distances (r(a)) and angles (angle(alpha)) obtained from least squares
refinements of the electron diffraction data are as follows: styrene,
r(C-H)(Av) = 1.102(7) Angstrom, r(C=C) = 1.355(16) Angstrom, r(C-C)(P
h) = 1.399(2) Angstrom, r(C-C=) = 1.475(23) Angstrom, angle C=C-C = 12
6.9(24)degrees; and bromostyrene, r(C-H)(Av) = 1.082(13) Angstrom, r(C
=C) = 1.331(20) Angstrom, r(C-C)(Ph) = 1.400(2) Angstrom, r(C-C=) = 1.
465(20) Angstrom, r(C-Br) = 1.893(8) Angstrom, angle C=C-C = 132.8(23)
degrees, angle Br-C=C = 125.7(15)degrees, angle C-2-C-1-C-7 = 123.9(33
). (C) 1997 Elsevier Science B.V.