The structure of 1,1,2,2-tetramethyl-1,2-disilacyclobutane
(1) has been investigated by experimental means, by Raman
and
IR spectra, and by quantum-chemical calculations at various levels
of theory. All the data obtained show that the four-membered ring
of 1 is puckered, the ring puckering mode being 80 cm–1 and the barrier to planarity 1.76 kcal/mol (617 cm–1). Temperature investigations of the Raman spectrum
have shown that the liquid 1 solidifies into a plastic
mesophase at ∼210 K and crystallizes below ∼110 K. Strain
energies (SEs) for 1, the parent molecule 1,2-disilacyclobutane
(2), and, for comparison, their 1,3-isomers (3 and 4) were estimated as enthalpies of corresponding
homodesmic reactions taken with a reversed sign. These values (in
kcal/mol) for 1 (8.6) and 2 (12.4) appeared
lower than those for 3 (18.3) and 4 (19.6).
To rationalize these results, a QTAIM topological analysis of electron
density distribution was carried out for 1–4. Examination of the molecular graphs has demonstrated that
the Si–Si bond paths (BPs) in 1 and 2 are significantly bent (“banana” bonds), thus decreasing
the SE of these molecules. The corresponding Si–Si BP lengths
are increased by Δ ≈ 0.03 Å in comparison to the
corresponding endocyclic Si–Si interatomic distances, while
the Si–C BPs in all four molecules are nearly straight lines
(Δ ≈ 0.002 Å). Monitoring of the process of 1 polymerization on heating to room temperature has revealed
that this process is not spontaneous, as was supposed previously,
but is initiated by minor radical impurities. Indeed, the value of
the ring-opening enthalpy for 1 was calculated as 70
kcal/mol, too high for spontaneous thermal polymerization to occur.