Effect of skeletal relaxation on the methyl torsion potential in acetaldehyde

Fully‐relaxed model ab initio calculations at Hartree–Fock/6–31G(d,p) and Mo/ller–Plesset (MP2)/6–31G(d,p) levels for acetaldehyde methyl conformers indicate significant skeletal flexing (e.g., the CH3 –C bond length changes by 0.006 A) and methyl hydrogen folding. Thirteen methyl conformer energies at 15° intervals are used to assess the magnitudes of the torsional potential function expansion terms. Only two terms V3=373.8 and V6=3.4 cm−1 (both significantly different from those obtained from microwave and infrared analyses) are found to be important. These calculations clearly show that relaxation during methyl rotation (i.e., skeletal flexing and methyl hydrogen folding) is an important determinant of the torsional potential. Energy levels obtained from internal rotation potentials which include flexing simulate infrared torsional fundamental frequencies in CH3CHO and CD3CHO to within 1–2 cm−1 of the experimental values. In the absence of relaxation infrared torsional fundamental frequencies are poorl...

[1]  S. Bell,et al.  Structure and potential energy functions for acetaldehyde: Ab initio calculations of X̃1A′, Ã1A″, and B̃1A′ states , 1985 .

[2]  C. Lin,et al.  Calculation of Energy Levels for Internal Torsion and Over‐All Rotation. II. CH3CHO Type Molecules; Acetaldehyde Spectra , 1957 .

[3]  Henry F. Schaefer,et al.  Applications of electronic structure theory , 1977 .

[4]  Ali G. Ozkabak,et al.  Methyl Torsional Interactions in Acetone , 1990 .

[5]  E. Martin,et al.  Barriers to rotation adjacent to double bonds , 1985 .

[6]  Kenneth B. Wiberg,et al.  Origin of rotation and inversion barriers , 1990 .

[7]  N. L. Allinger,et al.  The effect of electronegative atoms on the structures of hydrocarbons. ab initio calculations on molecules containing fluorine or (carbonyl) oxygen , 1985 .

[8]  P. Pulay,et al.  Critical comparison of the ab initio and spectroscopic methyl‐CH bond length difference in acetyl compounds, CH3C(O) X , 1984 .

[9]  H. Günthard,et al.  Internal rotation in acetaldehyde , 1976 .

[10]  F. Winther,et al.  K-structure analysis of the A and E components of the torsional fundamental of acetaldehyde and investigation of torsional combination bands , 1978 .

[11]  Kenneth B. Wiberg,et al.  Barriers to rotation adjacent to double bonds. 3. The carbon-oxygen barrier in formic acid, methyl formate, acetic acid, and methyl acetate. The origin of ester and amide resonance , 1987 .

[12]  L. Goodman,et al.  The acetone a2 torsional vibration , 1990 .

[13]  J. Hougen,et al.  The ground torsional state of acetaldehyde , 1991 .

[14]  D. C. Mckean CH stretching frequencies, bond lengths and strengths in acetone, acetaldehyde, propene and isobutene , 1975 .

[15]  T. Iijima,et al.  Zero-point average structure of a molecule containing a symmetric internal rotor , 1972 .

[16]  M. Herman,et al.  The fundamental torsion band in acetaldehyde , 1990 .

[17]  A. G. Ozkabak,et al.  Skeletal flexing during methyl rotation in small dimethyl molecules , 1991 .

[18]  E. Herbst,et al.  The millimeter-wave spectrum of acetaldehyde in its two lowest torsional states , 1986 .

[19]  H. Günthard,et al.  A versatile method for molecular structure determinations from ground state rotational constants , 1973 .

[20]  J. Wood,et al.  Combined Infrared and Microwave Determination of Torsional Parameters , 1970 .

[21]  H. Günthard,et al.  Solid state and gas infrared spectra and normal coordinate analysis of 5 isotopic species of acetaldehyde , 1971 .

[22]  D. Herschbach Calculation of Energy Levels for Internal Torsion and Over-All Rotation. III , 1959 .