Pentaquadrupole (QqQqQ) mass spectrometry is used to explore the abilities of gaseous SF n + ( n = 1–5) ions to form adducts and dimers with three π-electron rich molecules—benzene, acetonitrile, and pyridine, whereas ab initio calculations estimate most feasible structures, bond dissociation energies (BDEs), and reaction enthalpies of the observed products. With benzene, SF + reacts by net H-by-SF +· replacement. As suggested by the calculations, this novel benzene reaction forms ionized benzenesulfenyl fluoride, C 6H 5–SF +·, via a Wheland-type intermediate that spontaneously loses a H atom. SF 3 + forms a rare, loosely bonded π complex with benzene, [Bz ⋯ SF 3] +, which is stable toward both H and HF loss. No dimer, Bz 2SF 3 +, is formed. According to calculations, an unsymmetrically bonded, π-coordinated Bz 2SF 3 + dimer exists, i.e. (Bz–SF 3 ⋯ Bz) +, but its formation from [Bz ⋯ SF 3] + is endothermic; hence, thermodynamically unfavorable. With acetonitrile, SF 2 +·, SF 3 +, and SF 5 + form both adducts and dimers. CH 3–C ·N–SF 2 + (a new distonic ion) and CH 3CN–SF 5 + are covalently bonded, but CH 3CN ⋯ SF 3 + is loosely bonded. The binding natures of the acetonitrile adducts are reflected in the dimers; [CH 3CN–SF 2 ⋯ NCCH 3] +· and [CH 3CN–SF 5 ⋯ NCCH 3] + are unsymmetrically bonded, whereas [CH 3CN ⋯ SF 3 ⋯ NCCH 3] + is symmetrically and loosely bonded. Such dimers as [CH 3CN ⋯ SF 3 ⋯ NCCH 3] + are ideal for measurements of ion affinity via the Cooks’ kinetic method. With pyridine, only SF 3 + forms adduct and dimer. Py–SF 3 + is covalently bonded through nitrogen; [Py ⋯ SF 3 ⋯ Py] + is loosely but unsymmetrically bonded. The unsymmetric 2.28 and 2.44 Å long N–S bonds in [Py ⋯ SF 3 ⋯ Py] +, which are expected to rapidly interconvert, result likely from steric hindrance that forces orthogonal alignment of the two pyridine rings. Most observed adducts and dimers display relatively high BDEs, i.e. they are formed in thermodynamically favorable reactions. The extents of dissociation of the adducts and dimers observed in MS 3 experiments reflect the structures and BDEs predicted by the calculations.
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