THE EXISTENCE OF 2ND, 3RD AND 4TH ROW ANOMERIC INTERACTIONS - AN AB-INITIO STUDY OF THE TORSIONAL BEHAVIOR IN HSCH2SH, HSECH2SEH, HSCH2SEH,HTECH2TEH, HSCH2TEH AND HSECH2TEH
Sd. Kahn et al., THE EXISTENCE OF 2ND, 3RD AND 4TH ROW ANOMERIC INTERACTIONS - AN AB-INITIO STUDY OF THE TORSIONAL BEHAVIOR IN HSCH2SH, HSECH2SEH, HSCH2SEH,HTECH2TEH, HSCH2TEH AND HSECH2TEH, Journal of molecular structure. Theochem, 109, 1994, pp. 163-176
The torsional behaviour in the title compounds has been probed by ab i
nitio calculations of the gauche, gauche (g,g), gauche,anti (g,a), ant
i,gauche (a,g) and anti,anti (a,a) conformations at the MINI-1, 3-21G
() and 3-21G* levels. In the case of HSCH2SH, results at the 6-31G* l
evel have also been obtained. Although the trends in relative energies
and geometrical changes computed with the 3-21G and MINI-1* basis se
ts are similar for the different conformations, the C-X and C-Y bond l
engths are overestimated in the latter case. For the conformations of
HSCH2SH, good correspondence is obtained for the relative energies and
geometrical parameters with the 3-21G and 6-31G* basis sets. The exi
stence of putative anomeric interactions in the HXCH2YH molecules has
been evaluated by examination of the relative energies and geometrical
variations of the different conformers and also by the group separati
on energies obtained from the isodesmic reaction HXCH2YH + CH4 --> CH3
XH + CH3YH. In general, the a,a conformers either relax without barrie
r to another conformer or are not true minima. The stabilization of th
e g,g relative to the a,g conformation (the anomeric effect) decreases
for the heavier chalcogens and the trend even reverses for HTeCH2YH (
Y = Te, S, Se). The group separation energies (3-21G()) including zer
o-point energy corrections indicate anomeric stabilizations of about 1
kcal mol-1 for the most stable conformers (g,g) of XCH2YH (X, Y = S,
Se). The g,g and a,g forms are stabilized to the same extent in HSeCH2
SeH vis-a-vis the isodesmic reaction. For HTeCH2TeH, a stabilization e
nergy of only 0.17 kcal mol-1 is observed for the most stable conforme
r (a,g). We conclude that at the 3.21G level of computation even anom
eric interactions with tellurium are small but nonetheless present. We
propose also that with the heavier chalcogens the energy difference b
etween the a,g and a,a conformations may provide a better measure of a
nomeric stabilization in diheterosubstituted methanes.