Abstract

Treatment of V­(N­[<sup><i>t</i></sup>Bu]­Ar)<sub>3</sub> (<b>1</b>) (Ar = 3,5-Me<sub>2</sub>C<sub>6</sub>H<sub>3</sub>) with O<sub>2</sub> was shown by stopped-flow kinetic studies to result in the rapid formation of (η<sup>1</sup>-O<sub>2</sub>)­V­(N­[<sup><i>t</i></sup>Bu]­Ar)<sub>3</sub> (<b>2</b>) (Δ<i>H</i><sup>⧧</sup> = 3.3 ± 0.2 kcal/mol and Δ<i>S</i><sup>⧧</sup> = −22 ± 1 cal mol<sup>–1</sup> K<sup>–1</sup>), which subsequently isomerizes to (η<sup>2</sup>-O<sub>2</sub>)­V­(N­[<sup><i>t</i></sup>Bu]­Ar)<sub>3</sub> (<b>3</b>) (Δ<i>H</i><sup>⧧</sup> = 10.3 ± 0.9 kcal/mol and Δ<i>S</i><sup>⧧</sup> = −6 ± 4 cal mol<sup>–1</sup> K<sup>–1</sup>). The enthalpy of binding of O<sub>2</sub> to form <b>3</b> is −75.0 ± 2.0 kcal/mol, as measured by solution calorimetry. The reaction of <b>3</b> and <b>1</b> to form 2 equiv of OV­(N­[<sup><i>t</i></sup>Bu]­Ar)<sub>3</sub> (<b>4</b>) occurs by initial isomerization of <b>3</b> to <b>2</b>. The results of computational studies of this rearrangement (Δ<i>H</i> = 4.2 kcal/mol; Δ<i>H</i><sup>⧧</sup> = 16 kcal/mol) are in accord with experimental data (Δ<i>H</i> = 4 ± 3 kcal/mol; Δ<i>H</i><sup>⧧</sup> = 14 ± 3 kcal/mol). With the aim of suppressing the formation of <b>4</b>, the reaction of O<sub>2</sub> with <b>1</b> in the presence of <sup><i>t</i></sup>BuCN was studied. At −45 °C, the principal products of this reaction are <b>3</b> and <sup><i>t</i></sup>BuC­(O)­NV­(N­[<sup><i>t</i></sup>Bu]­Ar)<sub>3</sub> (<b>5</b>), in which the bound nitrile has been oxidized. Crystal structures of <b>3</b> and <b>5</b> are reported

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