Journal of the American Chemical Society, Vol.116, No.19, 8691-8704, 1994
Ligand-Field Effects in the Hydrated Divalent and Trivalent Metal-Ions of the First and 2nd Transition Periods
The influence of d-shell occupation on the structure of the first hydration sphere for a series of hydrated transition metal ions has been evaluated by using theoretical calculations to optimize the geometry and find the conformations with lowest energy. General trends in the properties reflecting the calculated metal-oxygen bond strength and energy are discussed and compared with experimental values. The metal-oxygen distances, calculated by ab initio SCF methods using large basis sets for high-spin hexaaqua complexes in the T-h symmetry of the di- and trivalent 3d metal ions, follow closely the trends found in crystal structure determinations of the isomorphous series of the 3d hexaaqua metal ions in Tutton and alum salts. The variation of the binding energies in a hexaaqua complex shows the double-humped features expected for a splitting of the d orbitals in an octahedral ligand field with the largest stabilization at formal d(3) and d(8) electron configurations of the metal ions. In cases with degenerate d-orbitals, an additional splitting of the energy levels by a lowering of the symmetry of the hexahydrated ion will in some cases significantly increase the binding energy. For the largest d(1) and d(6) metal ions an "all-vertical", and for some large d(2) ions an "air-horizontal", conformation of the hydrogen atoms of the planarly coordinated water ligands around the trifold axis in the D-3d symmetry is favored. For the hexahydrated d(9) ion Ag2+, the first-order Jahn-Teller effect leading to a tetragonal elongation of the octahedral coordination has been studied. The possibility that the nondistorted d(4) [Cr(H2O)(6)](2+) complex is forced into a low-spin state in its hexafluorosilicate salt due to compression in the lattice has been considered. The electrostatically dominated binding in the hexaaqua complexes shows an increasing covalent contribution to the right in the transition rows, especially for the trivalent ions. The ligand field effects are generally larger for the trivalent than for the divalent ions and also larger for the 4d(n) than for the 3d(n) elements, although the overall bond strength is lower due to the larger size of the 4d(n) ions. The high ligand field strength results in low-spin ground states for the hexahydrated Co3+, RU(2+), Rh3+ (d(6)), and RU(3+) (d(5)) ions in solution but, except for Rh3+, these high- to low-spin transitions proved to be difficult to reproduce by computations for the isolated hexaaqua clusters. Electron correlation was introduced, but the effect of the surroundings, which also may provide an additional important contribution to the stabilization of the low-spin state, was not accounted for. The low-spin square-planar configurations of the d(8) complexes [Pd(H2O)(4)](2+) and [Ag(H2O)(4)](3+) are discussed in terms of ligand field effects.
Keywords:NEUTRON-DIFFRACTION STRUCTURE;EFFECTIVE CORE POTENTIALS;CRYSTAL RAMAN-SPECTRA;TERVALENT AQUA IONS;AQUEOUS-SOLUTION;X-RAY;MOLECULAR CALCULATIONS;2ND-SPHERE HYDRATION;TITANIUM(III) ION;CESIUM ALUMS