Topics in Current Chemistry

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Solid Sulfur Allotropes 33 Table 11 Molecular structure data of orthorhombic S11 at 163 Ka [38] Point symmetry Av. bond lengths (pm) Range Av. bond angles (􏰹) Range Av. torsion angles (􏰹)b Range 2–C2 (approximately) Molecule 1 205.7 203.7–211.0 106.0 103.8–108.4 97.1 70.5–140.5 Molecule 2 205.5 203.2–207.7 106.3 103.3–108.6 96.9 69.3–137.1 a Errors of bond lenghts 0.3–0.4 pm, of angles 0.1􏰹 b Absolute values (molecule 1) and 208 pm (molecule 2) with two adjacent short bonds (203– 204 pm). The related torsion angles of 141􏰹 (1) and 137􏰹 (2), respectively, are the largest ever observed in sulfur rings. However, crystalline S11 is of medi- um stability similar to S6, S9, S10, and S13. Both independent molecules of S11 in the crystal have the same conforma- tion, but the parameters of equivalent bonds show significant differences which are exceeded only in the case of solid S13 (Table 11). 2.2.1.8 Orthorhombic S12 Solid cyclo-dodecasulfur was first synthesized by Schmidt and Wilhelm in 1966 [98]. The authors obtained pale-yellowish, plate-like rectangular needles of solid S12 (from benzene solution). In the same year an X-ray structural analysis was reported by Kutoglu and Hellner [99]. A refined anal- ysis of crystalline S12 was performed by Steidel et al. in 1981, together with an examination of the molecular addition compound CS2·S12 [100]. Accord- ingly, S12 crystallizes in the orthorhombic space group Pnnm–D2h12 (no. 58) with a unit cell containing two molecules on sites of C2h symmetry. As was discussed in the case of cyclo-decasulfur S10, for the even-mem- bered S12 ring one might have expected a highly symmetrical molecular structure of D6d symmetry in analogy to S6 (D3d) and S8 (D4d). However, the X-ray single crystal analyses revealed an approximate D3d conformation of S12 (see Fig. 12) [99, 100]. By ab-initio quantum chemical calculations it has been shown that the D6d structure is about 226 kJ mol􏱐1 less stable than the D3d structure and, moreover, that it is not even a minimum on the potential energy surface [68]. In the S12 molecule the atoms are located in three parallel planes: six atoms in the median plane and three atoms each in an upper and in a lower plane. An arrangement in which the atoms would be located in two planes (D6d structure) would yield torsion angles of 129􏰹 being far from the opti- mum value of about 90􏰹. As a result, the bond lengths would be larger as a consequence of bond weakening due to the large torsion angles. In the D3d

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