Jk. Wolken et F. Turecek, Heterocyclic radicals in the gas phase. An experimental and computational study of 3-hydroxypyridinium radicals and cations, J AM CHEM S, 121(25), 1999, pp. 6010-6018
Radicals 3-hydroxy-(1H)-pyridinium (1H) through 3-hydroxy-(6H)-pyridinium (
6H) and 3-pyridylhydroxonium (7H) were studied as models of hydrogen atom a
dducts to nitrogen heterocycles. Radical 1H was generated in the gas phase
by femtosecond collisional electron transfer to stable 3-hydroxy-(1H)-pyrid
inium cations (1H(+)). The fractions of nondissociating 1H decreased with i
ncreasing internal energies of the precursor cations as determined by the g
as-phase protonation energetics. Radical 1H dissociated unimolecularly by l
oss of the N-bound hydrogen atom to produce 3-hydroxypyridine (1). The diss
ociation showed large isotope effects that depended on the radical's intern
al energy. Other dissociations of 1H were loss of OH., ring contraction for
ming C-OH and pyrrole, and ring cleavages leading to C3Hx and C2HxN fragmen
ts, Combined MP2 and B3LYP/6-311G(2d,p) calculations yielded topical proton
affinities in 1 as 938 (N-1), 757 (C-2), 649 (C-3), 721 (OH), 727 (C-4), 7
14 (C-5), and 763 (C-6) kJ mol(-1). 1H+ was the most stable ion isomer form
ed by protonation of 1. Radical 1H was the most stable isomer whereas 2H, 3
H, 4H, 5H, and 6H were calculated to be 9, 48, 16, 18, and 22 kJ mol(-1) le
ss stable than 1H, respectively. The 3-pyridylhydrosonium radical 7H dissoc
iated without barrier by cleavage of the O-H bond. N-H bond dissociation in
1H was 102 kJ mol(-1) endothermic at 298 K and required an activation ener
gy of 126 kJ mol(-1). Deuterium isotope effects on the N-(H,D) bond dissoci
ations were modeled by RRKM calculations and used to estimate the internal
energy distribution in 1H. Isomerizations of 1H to 2H and 2H to 3H required
activation energies of 174 and 130 kJ mol(-1), respectively. Ring-cleavage
dissociations of 18 were >220 kJ mol(-1) endothermic. The occurrence of co
mpetitive ring cleavage dissociations pointed to a bimodal internal energy
distribution in 1H due to the formation of excited electronic states upon e
lectron transfer. The electronic properties and excited states of heterocyc
lic radicals are discussed.