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Solid Sulfur Allotropes 53 S12 S13 S14: S15 endo-S18 (a-S18) S20 Sm 148 􏰹C at heating rate 10 K min􏱐1, 141 􏰹C at 5 K min􏱐1, 135 􏰹C at 2.5 K min􏱐1 [55] Polymerizes at ca. 90 􏰹C prior to melting at 114 􏰹C [55] 117 􏰹C [46] No melting point has been reported for this allotrope 126–128 􏰹C [104] 121 􏰹C [55] (124–125 􏰹C [104], 120–130 􏰹C [43]) ca. 110 􏰹C [55] In this context it should be mentioned that the heat conductivity of ele- mental sulfur is extremely low. Therefore, heating rates should not be chosen too high. Obviously, melting temperatures also depend on the external pressure, a phenomenon which has been most extensively studied in the case of S8 [156]; see below. 2.3.2 Thermal Behavior The thermal decomposition of the sulfur allotropes has been studied exten- sively by Steudel et al. [55]. S6: pure solid cyclo-hexasulfur decomposes only slowly at 20 􏰹C [157] and even at 50 􏰹C the reaction is still slow. Storage at 20 􏰹C in diffuse daylight for 10 days resulted in a decomposition of only 3% of the original S6 and the only decomposition product was Sm. Storage at 50 􏰹C (in an oven) for 5 days gave 8% Sm and 2% S8 [106]. At 120 􏰹C, in the liquid state, the decomposition is complete within 1 min yielding S7, S8 and Sm. DSC diagrams show the melting of pure S6 to begin at 88 􏰹C (endothermic melting peak centered at 100 􏰹C) followed by the exothermic polymerization to S1 (peak centered at 110 􏰹C) and its exothermic depolymerization to mainly S8 and some S7 [55]. S7: cyclo-heptasulfur is the least stable of all sulfur allotropes. After 2 h at 20 􏰹C a sample of g-S7 had decomposed to a mixture of S8 and Sm containing only trace amounts of S7. After 4 days at 20 􏰹C (in the dark) the decomposi- tion was complete and yielded 81% Sm and 19% S8 [106]. The melting of g-S7 at 39 􏰹C is reversible, but on further heating the melt polymerizes exother- mically at 70–110 􏰹C followed by the exothermic depolymerization of S1 to the equilibrium melt in the region above 115 􏰹C [55]. S8: below 96 􏰹C, cyclo-octasulfur is stable as orthorhombic a-S8. However, the conversion to monoclinic b-S8 at temperatures just above the triple point of 96 􏰹C is kinetically hindered and requires lattice defects or imperfections as present in a powder but usually not in a single-crystal [158]. Therefore, single-crystals of a-S8 usually melt at 115 􏰹C without prior conversion to the b-form. For the same reason the temperature at which the transition a!b is observed by DSC measurements depends on the heating rate and is often found well above 100 􏰹C, even if a powder-like sample is used. The activation energy for the a!b transition is approximately identical to the enthalpy of sublimation of a-S8 (100 kJ mol􏱐1) [158]. Heating of S8 to 90–110 􏰹C, just be-

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