Structure of the High-Energy Conformer of 1,3-Butadiene

The experimental vibrational frequencies of s-trans -1,3-butadiene, for which the assignments are well-established, are used to determine the scale factors for its quantum mechanical force field obtained at the MP2/6-31G*//MP2/6-31G* level of theory. The scale factors are then transferred to the MP2/6-31G*//MP2/6-31G* force fields of the s-cis and s-gauche rotamers and their theoretical frequencies calculated. Comparison of the vibrational frequencies of these three species indicates a special region of the IR spectrum of 1,3-butadiene in the gas phase (720−790 cm -1 ) in which only a band attributable to the s-gauche rotamer should be present; i.e., it should be free both of the observed IR bands of the s-trans and of the calculated vibrational frequencies of the s-cis conformer. Investigation of the medium- and high-resolution IR spectra of 1,3-butadiene in the gas phase reveals the presence of a band at 749.22(20) cm -1 possessing the typical B contour (consistent with A symmetry, C 2 group). Rotational analysis of the medium-resolution spectrum of this band yields the rotational constants A ‘‘ − B̄ ‘‘ = 0.4478(27) cm -1 and A ‘ − B̄ ‘ = 0.4455(25) cm -1, only about one-third of the experimental values for s-trans -1,3-butadiene. This identifies the band as belonging to the high-energy conformer of 1,3-butadiene. The agreement between the experimental and theoretical values of the band center (749 vs 735 cm -1 ), the clear B type contour, and the extremely complicated character of the high-resolution spectrum of the band at 749.22 cm -1 strongly suggest that the geometry of the high-energy conformer of 1,3-butadiene in the gas phase is nonplanar s-gauche and not planar s-cis .