Structural and conformational properties of 2-propynylphosphine (propargylphosphine) as studied by microwave spectroscopy supplemented by quantum chemical calculations
J. Demaison et al., Structural and conformational properties of 2-propynylphosphine (propargylphosphine) as studied by microwave spectroscopy supplemented by quantum chemical calculations, INORG CHEM, 40(15), 2001, pp. 3719-3724
The microwave spectrum of 2-propynylphosphine (propargylphosphine); H-C dro
pC-CH2-PH2, has been investigated in the 18-26.5 and 32-48 GHz spectral reg
ions sit about -50 degreesC. Two conformers with different orientation:of t
he phosphino-group, denoted conformer I-and conformer Il, respectively, wer
e: assigned. Conformer I has a symmetry plane (C-s symmetry) with both hydr
ogen atoms of the phosphino group pointing toward the triple bond (C-C-P-H
dihedral angles approximately 47 degrees from syn-periplanar (0 degrees)).
The C-C-P-H dihedral angles are 73 and 167 degrees, respectively, from syn-
periplanar in,conformer II.,Only one of the hydrogen atoms of the phosphino
group points toward the triple bond in this rotamer. Conformer I is 1.5(20
) kJ/mol more stable than II. The dipole moment of LI was determined to be
tin units of 10(-30) C m) mu (a) = 0 (assumed), mu (b) = 3.05(7), mu (c) =
1.60(9), and mu (tot) = 3.44(9) [mu (tot) = 1.03(3) D]. Two vibrationally e
xcited states were assigned for each of the two rotamers I and II. Their fr
equencies were determined by relative intensity measurements. Many of the t
ransitions of conformer II were split into two components presumably becaus
e of tunneling of the phosphino group. The tunneling frequency was determin
ed to-be 0.814(42) MHz for the ground vibrational state and 11.49(18) MHz f
or the first excited state of the C-P torsional vibration. Quantum chemical
calculations at the B3LYP and MP2 levels of theory using the 6-311++G(3df,
2pd) basis set reproduced experimental rotational constants, quartic centri
fugal distortion constants, and dipole moment components within a few perce
nt. The energy difference between the two conformers was calculated using t
he Gaussian-2 theory, and conformer I was found to be more stable than conf
ormer II by 2.1 kJ/mol.