Reaction of guanine with H2O3 in the absence and presence of a water molecule leading to the formation of 8-oxoguanine (8-oxoG) was investigated. Initial calculations were performed using imidazole (Im) as a model for the five-membered ring of guanine. The reactant, intermediate, and product complexes as well as transition states were obtained in gas phase at the B3LYP/6-31+G* and B3LYP/AUG-cc-pVDZ levels of theory. In all the cases, except for the reactions involving imidazole, single-point energy calculations were performed in gas phase at the MP2/AUG-cc-pVDZ level of theory. Solvation calculations in aqueous media were carried out using the polarizable continuum model (PCM) of the self-consistent reaction field (SCRF) theory. Vibrational frequency analysis and intrinsic reaction coordinate (IRC) calculations were performed to ensure that the transition states connected the reactant and product complexes properly. Zero-point energy (ZPE)-corrected total energies and Gibbs free energies at 298.15 K in gas phase and aqueous media were obtained. When a reaction of H2O3 in place of H2O2 with guanine is considered, the major barrier energy which is encountered at the first step is almost halved showing that H2O3 would be much more reactive than H2O2. Considering the reaction schemes investigated here and the observed fact that H2O3 is dissociated easily under ambient conditions, it appears that H2O3 would serve as an effective reactive oxygen species.
Modification in DNA or protein structure can severely affect DNA-protein interactions and the functioning of biological systems. Some new insights into radiation-induced effects of guanine-lysine interactions have been obtained here by theoretical investigations. Geometries of zwitterionic and non-zwitterionic lysine in different charge states (neutral, radical cation, and protonated cation) were optimized employing the B3LYP/6-31G** and B3LYP/AUG-cc-pVDZ levels of hybrid density functional theory (DFT) and using the second-order Møller-Plesset perturbation theory along with the 6-31G** basis set. In the case of neutral lysine in the gas phase, no zwitterionic structure was obtained. The non-zwitterionic structures of lysine in radical and protonated cationic forms are appreciably more stable than the corresponding zwitterionic structures in the gas phase as obtained at all levels of theory employed here. Binding of guanine and different dehydrogenated guanine radicals with lysine in different charge states was studied at the B3LYP/6-31G** level of DFT. When guanine makes a complex with the lysine radical cation, large amounts of spin and positive charge densities are transferred from the lysine radical cation to guanine and the guanine is thus converted from its normal form to the radical cationic form. Complexation of the lysine radical cation with the H1-hydrogen-abstracted guanine radical leads to CO2 liberation and proton transfer from lysine. These results are compared with the available experimental ones.
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