Pnicogen-Bonded Complexes H<sub><i>n</i></sub>F<sub>5–<i>n</i></sub>P:N-Base, for <i>n</i> = 0–5

Abstract

Ab initio MP2/aug′-cc-pVTZ calculations have been carried out on the pnicogen-bonded complexes H<sub><i>n</i></sub>F<sub>5–<i>n</i></sub>P:N-base, for <i>n</i> = 0–5 and nitrogen bases NC<sup>–</sup>, NCLi, NP, NCH, and NCF. The structures of these complexes have either <i>C</i><sub>4<i>v</i></sub> or <i>C</i><sub>2<i>v</i></sub> symmetry with one exception. P–N distances and interaction energies vary dramatically in these complexes, while F<sub>ax</sub>–P–F<sub>eq</sub> angles in complexes with PF<sub>5</sub> vary from 91° at short P–N distances to 100° at long distances. The value of this angle approaches the F<sub>ax</sub>–P–F<sub>eq</sub> angle of 102° computed for the Berry pseudorotation transition structure which interconverts axial and equatorial F atoms of PF<sub>5</sub>. The computed distances and F<sub>ax</sub>–P–F<sub>eq</sub> angles in complexes F<sub>5</sub>P:N-base are consistent with experimental CSD data. For a fixed acid, interaction energies decrease in the order NC<sup>–</sup> > NCLi > NP > NCH > NCF. In contrast, for a fixed base, there is no single pattern for the variations in distances and interaction energies as a function of the acid. This suggests that there are multiple factors that influence these properties. The dominant factor appears to be the number of F atoms in equatorial positions, and then a linear F<sub>ax</sub>–P···N rather than H<sub>ax</sub>–P···N alignment. The acids may be grouped into pairs (PF<sub>5</sub>, PHF<sub>4</sub>) with four equatorial F atoms, then (PH<sub>4</sub>F, PH<sub>2</sub>F<sub>3</sub>) with F<sub>ax</sub>–P···N linear, and then (PH<sub>3</sub>F<sub>2</sub> and PH<sub>5</sub>) with H<sub>ax</sub>–P···N linear. The electron-donating ability of the base is also a factor in determining the structures and interaction energies of these complexes. Charge transfer from the N lone pair to the σ* P–A<sub>ax</sub> orbital stabilizes H<sub><i>n</i></sub>F<sub>5–<i>n</i></sub>P:N-base complexes, with A<sub>ax</sub> either F<sub>ax</sub> or H<sub>ax</sub>. The total charge-transfer energies correlate with the interaction energies of these complexes. Spin–spin coupling constants <sup>1p</sup><i>J</i>(P–N) for (PF<sub>5</sub>, PHF<sub>4</sub>) complexes with nitrogen bases are negative with the strongest bases NC<sup>–</sup> and NCLi but positive for the remaining bases. Complexes of (PH<sub>4</sub>F, PH<sub>2</sub>F<sub>3</sub>) with these same two strong bases and H<sub>4</sub>FP:NP have positive <sup>1p</sup><i>J</i>(P–N) values but negative values for the remaining bases. (PH<sub>5</sub>, PH<sub>3</sub>F<sub>2</sub>) have negative values of <sup>1p</sup><i>J</i>(P–N) only for complexes with NC<sup>–</sup>. Values of <sup>1</sup><i>J</i>(P–F<sub>ax</sub>) and <sup>1</sup><i>J</i>(P–H<sub>ax</sub>) correlate with the P–F<sub>ax</sub> and P–H<sub>ax</sub> distances, respectively

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