The C–H overtone absorption spectra of (CH3O)3B in liquid and gas phases are reported. The observed energies of the C–H stretching overtones corresponding to Δv=3, 4, 5, and 6 (liquid) are obtained by conventional spectroscopy. The C–H overtones Δv=5 and 6 (gas) are obtained by laser intracavity photoacoustic spectroscopy. Computer deconvolution of the gas-phase absorptions shows two bands at each overtone which are assigned as the overtones of nonequivalent C–H bonds. In general, for molecules in which a methyl group is directly attached to an oxygen atom, nonequivalent C–H bonds are produced due to the ‘‘trans effect.’’ A different mechanism seems to occur in the case of the methyl groups in trimethylborate even though they are adjacent to an oxygen atom. In order to interpret the experimental results, ab initio molecular-orbital calculations were performed on (CH3O)BH2, (CH3O)2BH, and (CH3O)3B. Equilibrium geometries, vibrational frequencies, and infrared intensities were calculated at the Hartree–Fock level using the 3-21G split valence basis set. In the three molecules studied, the equilibrium conformation is such that the methyl groups have one C–H bond (C–Ha ) in the plane of the molecule and cis to a B–O bond, and two equivalent C–H bonds located symmetrically above and below the plane of the molecule (C–Hb ). In (CH3O)BH2, the in-plane C–H bond C–Ha is longer than the out-of-plane C–H bonds C–Hb (1.082 Å vs 1.0795 Å). This trend is reversed in the case of (CH3O)3B, where the C–Ha and C–Hb bond lengths are 1.0792 and 1.0807 Å, respectively. The situation is more complicated in the case of the molecule (CH3O)2BH, where in one methyl group the C–Ha bond is shorter than the C–Hb bond (1.0794 Å vs 1.0802 Å), while in the other methyl group the corresponding C–Ha bond is longer than the C–Hb bond (1.0829 Å vs 1.0802 Å). The nature of the difference in the C–H bond lengths is studied and discussed in terms of group orbital interactions in both, the σ and π systems. In addition, a correlation between the C–H bond length, the corresponding C–H stretching force constant, and the vibrational frequency is discussed based on vibrational frequency calculations performed on the deuterated species (CHD2O)nBH3−n for n=1, 2, 3 in cases where the isolated C–H was considered to be the in-plane C–Ha or the out-of-plane C–Hb.
Read full abstract