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    Quantum Mechanical Analysis of Nonenzymatic Nucleotidyl Transfer Reactions: Kinetic and Thermodynamic Effects of β–γ Bridging Groups of dNTP Substrates

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    Rate (<i>k</i>) and equilibrium (<i>K</i>) constants for the reaction of tetrahydrofuranol with a series of Mg<sup>2+</sup> complexes of methyl triphosphate analogues, CH<sub>3</sub>O-P­(O<sub>2</sub>)-O-P­(O<sub>2</sub>)-X-PO<sub>3</sub><sup>4–</sup>, X = O, CH<sub>2</sub>, CHCH<sub>3</sub>, C­(CH<sub>3</sub>)<sub>2</sub>, CFCH<sub>3</sub>, CHF, CHCl, CHBr, CFCl, CF<sub>2</sub>, CCl<sub>2</sub>, and CBr<sub>2</sub>, forming phosphate diester and pyrophosphate or bisphosphonate in aqueous solution were evaluated by B3LYP/TZVP//HF/6-31G* quantum chemical calculations and Langevin dipoles and polarized continuum solvation models. The calculated log <i>k</i> and log <i>K</i> values were found to depend linearly on the experimental p<i>K</i><sub>a4</sub> of the conjugate acid of the corresponding pyrophosphate or bisphosphonate leaving group. The calculated slopes of these Brønsted linear free energy relationships were β<sub>lg</sub> = −0.89 and β<sub>eq</sub> = −0.93, respectively. The studied compounds also followed the linear relationship Δlog <i>k</i> = 0.8Δlog <i>K</i>, which became less steep, Δlog <i>k</i> = 0.6Δlog <i>K</i>, after the range of studied compounds was extended to include analogues that were doubly protonated on γ-phosphate, CH<sub>3</sub>O-P­(O<sub>2</sub>)-O-P­(O<sub>2</sub>)-X-PO<sub>3</sub>H<sub>2</sub><sup>2–</sup>. The scissile P<sub>α</sub>–O<sub>lg</sub> bond length in studied methyl triphosphate analogues slightly increases with decreasing p<i>K</i><sub>a</sub> of the leaving group; concomitantly, the CH<sub>3</sub>OP<sub>α</sub>(O<sub>2</sub>) moiety becomes more positive. These structural effects indicate that substituents with low p<i>K</i><sub>a</sub> can facilitate both P<sub>α</sub>–O<sub>lg</sub> bond breaking and the P<sub>α</sub>–O<sub>nuc</sub> bond forming process, thus explaining the large negative β<sub>lg</sub> calculated for the transition state geometry that has significantly longer P<sub>α</sub>–O<sub>nuc</sub> distance than the P<sub>α</sub>–O<sub>lg</sub> distance
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