1,3-Butadiene and its 2,3-digerma analogue H2C=HGe-GeH=CH2 are investi
gated through ab initio calculations. Geometries are determined at the
SCF-DZP level, and energies are refined at the MP4 level. Substitutio
n of carbon by germanium at positions 2,3 has two main effects. First,
the central bond conjugation is significantly decreased. Second, the
relatively long Ge-Ge central bond removes the steric hindrance that w
as causing the s-cis isomer of butadiene to distort into a nonplanar g
auche form. Therefore, 2,3-digermabutadiene has two stable planar conf
ormers, close in energy, corresponding to C-2h s-trans and C-2v s-cis
forms. The s-cis isomer is unfavored by 0.4 kcal/mol. The rotational b
arrier from the trans isomer is calculated at 1.6 kcal/mol. Due to pla
nar sigma repulsion, the coordinate corresponding to rotation around t
he central Ge-Ge bond in the s-cis isomer is very flat on the potentia
l surface and is associated with a very low-frequency normal mode. Var
ious approaches, based on geometry or energy criteria, are used to eva
luate the extent of pi conjugation in butadiene and 2,3-digermabutadie
ne. They suggest that the pi-conjugation in the latter is about half t
hat in butadiene.