1986
DOI: 10.1107/s0108768186097689
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Propellanes LXXIX. Comparison of the geometries of dithia[n.3.3]propellanes (n = 1, 2, 3) and dithia(and oxathia)[4.3.3]propellanes. Study of the influence of complexation with HgCl2, I2, CdCl2 and PdCl2 and of formation of sulfoxides on some of these compounds. Demonstration of the 'Klammer' effect. Structures of eighteen crystals

Abstract: The room-temperature crystal structures of eighteen compounds are reported. (2) symmetry. There are only three exceptions to this non-mixing rule among thirty-odd of the many propellane structures reported in the literature. The considerable deviations found from ideal conformations are ascribed to crystal packing effects and, for molecules with n = 1 and 2, to the deviations from tetrahedrality at the bridgehead atoms; this serves to explain the 'Klammer' effect. The lowest-energy conformations from molecul… Show more

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Cited by 36 publications
(16 citation statements)
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“…In 7, the Hg±S distance and the distance between the mercury and non-bridging Cl atom are slightly shorter than in complexes of mercury chloride with N,S-didentate [26] or N,N,S-tridentate [24,25,27] thiosemicarbazones, but are similar to those found in other dimeric mercury chloride complexes with S-monodentate thiosemicarbazone ligands [28,29]. Of the distances between the mercury atom and bridging chlorine atoms, the shortest two are significantly shorter than in other chloro-bridged Hg dimers with S-monodentate ligands [28,32], while the longest two are at least 0.2 A Ê longer than in any other known dimer of this kind [28,30,31] (in those with long Hg±Cl br distances most closely approaching those of 7 the mercury atoms have coordination number five, like 7 [32]). …”
Section: Molecular Structuresmentioning
confidence: 74%
“…In 7, the Hg±S distance and the distance between the mercury and non-bridging Cl atom are slightly shorter than in complexes of mercury chloride with N,S-didentate [26] or N,N,S-tridentate [24,25,27] thiosemicarbazones, but are similar to those found in other dimeric mercury chloride complexes with S-monodentate thiosemicarbazone ligands [28,29]. Of the distances between the mercury atom and bridging chlorine atoms, the shortest two are significantly shorter than in other chloro-bridged Hg dimers with S-monodentate ligands [28,32], while the longest two are at least 0.2 A Ê longer than in any other known dimer of this kind [28,30,31] (in those with long Hg±Cl br distances most closely approaching those of 7 the mercury atoms have coordination number five, like 7 [32]). …”
Section: Molecular Structuresmentioning
confidence: 74%
“…The length of the conjoining bond, C(5)-C(6), with the value of 1.580(5) Å, is significantly longer than that of a typical single C-C bond, but comparable to average (C) 3 -C(sp 3 )-C(sp 3 )-(C) 3 (1.588 Å, [99]). Among the known dithia-and oxathia [4.3.3] propellanes only those with the rigid conformations: boat for 6-membered rings and envelope for 5-membered rings, show such an elongated conjoining bond (1.570-1.588 Å) [8,9].…”
Section: Resultsmentioning
confidence: 99%
“…Dithia-and oxathiapropellanes were also a subject of structural investigations, both propellanes themselves and their complexes with Cl 2 Á4H 2 O, I 2 , HgCl 2 , CdCl 2 and PdCl 2 [8]. One example of oxathia propellane, obtained by Diels-Alder reaction, was also described by Kaftory [9].…”
Section: Introductionmentioning
confidence: 96%
“…For and adducts, which are strong adducts according to the above classifications, much less structural and FT-Raman data are available, therefore generalizations are less reliable. adducts with both - and -donors show one main peak in their FT-Raman spectra in the range 190–140 cm −1 [16, 59, 60, 6267, 81] at a lower frequency with respect to solid [216 cm −1 , d (I−Br) = 2.521(4) Å] [98], and it is assignable to a stretching vibration of the E−I−Br three-body system having a major contribution from the ν (I−Br) vibration [63]. adducts (only four out of seven are both structurally and vibrationally characterized) [60, 67, 68] generally show in their FT-Raman spectra two main peaks: one in the range 240–180 cm −1 presumably due to the antisymmetric ( ν 3 ) stretching vibration of the E−I−Cl three body-system ( = , ), and the other at about 130 cm −1 due to the symmetric ( ν 1 ) stretching vibration (solid is characterized by a single peak at 283 cm −1 in its FT-Raman spectrum with a d (I−Cl) = 2.446(6) Å) [99].…”
Section: Discussionmentioning
confidence: 99%