T. Sakaizumi et al., MICROWAVE-SPECTRUM, MOLECULAR-STRUCTURE, AND AB-INITIO CALCULATION OF(E)-CHLOROACETALDEHYDE OXIME, Journal of molecular structure, 413, 1997, pp. 107-119
The microwave spectra of (E)-(ClCH2CH)-Cl-35=NOH, (E)-(ClCH2CH)-Cl-37=
NOH, (E)-(ClCH2CH)-Cl-35=NOD, and (E)-(ClCH2CH)-Cl-37=NOD have been ob
served in the frequency range from 26.4 to 40.5 GHz. The rotational an
d centrifugal distortion constants of the four isotopic species in the
ground and excited vibrational states were determined, The values of
the Delta I(=I-f -I-a -I-b) obtained for the normal (Cl-35 and Cl-17)
and deuterated (Cl-35 and Cl-37) species in the ground vibrational sta
te were found to be -16.350(4), -16.36(4), -17.06(4), and -17.07(6) u
Angstrom(2), respectively. The molecular structure of this molecule wa
s determined to be the anticlinal form (phi(1):angle ClCCN = 121.4 deg
rees, phi(2):angle CNOH = 180.0 degrees), as shown in Fig. l(a). It wa
s found that ab initio calculation of MP2/6-31G* level can be used to
predict the most stable rotational conformer of (E)-ClCH2CH=NOH, The
seven structural parameters of the heavy atom skeleton of this molecul
e were fitted to the eight rotational constants (B and C) of the four
isotopic species. The obtained structural parameters (r(0)) are almost
the same as those (r(alpha)) Obtained previously by a gas-phase elect
ron diffraction study (K. Iijima, T. Miwa, T. Sakaizumi, O. Ohashi, J,
Mol. Struct. 352/353 (1995) 161), within the errors. The r(C=N) and a
ngle CCN obtained for (E)-ClCH2CH=NOH are slightly shorter and drastic
ally narrower than those of (Z)-ClCH2CH=NOH. The trend is consistent w
ith those of CH3CH=NOH and CH3CH2CH=NOH. (C) 1997 Elsevier Science B.V
.