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Zinc(II) hydration in aqueous solution. A Raman spectroscopic investigation and an ab-initio molecular orbital study

118

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36

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1999

Year

Abstract

Raman spectra of aqueous Zn(II) perchlorate solutions were measured over a broad concentration (0.50-3.54 mol L<sup>-1</sup>) and temperature (25-120°C) range. The weak polarized band at 390 cm<sup>-1</sup> and two depolarized modes at 270 and 214 cm<sup>-1</sup> have been assigned to ν<sub>1</sub>(a<sub>1g</sub>), ν<sub>2</sub>(e<sub>g</sub>) and ν<sub>5</sub>(f<sub>2g</sub>) of the hexaaquazinc(II) ion, respectively. The infrared active mode at 365 cm<sup>-1</sup> has been assigned to ν<sub>3</sub>(f<sub>1u</sub>). The vibrational analysis of the species [Zn(OH<sub>2</sub>)<sub>6</sub><sup>2+</sup>] was done on the basis of <i>O</i><sub>h</sub> symmetry (OH<sub>2</sub> as point mass). The polarized mode ν<sub>1</sub>(a<sub>1g</sub>) ZnO<sub>6</sub> has been followed over the full temperature range and band parameters (band maximum, full width of half height and band intensity) have been examined. The position of the ν<sub>1</sub>(a<sub>1g</sub>) ZnO<sub>6</sub> mode shifts only about 4 cm<sup>-1</sup> to lower frequencies and broadens about 32 cm<sup>-1</sup> for a 95°C temperature increase. The Raman spectroscopic data suggest that the hexaaquazinc(II) ion is thermodynamically stable in perchlorate solution over the temperature and concentration range measured. <i>Ab</i><i>initio</i> geometry optimizations and frequency calculations of [Zn(OH<sub>2</sub>)<sub>6</sub><sup>2+</sup>] were carried out at the Hartree-Fock and second order Møller-Plesset levels of theory, using various basis sets up to 6-31+G*. The global minimum structure of the hexaaqua Zn(II) species corresponds with symmetry <i>T</i><sub>h</sub>. The unscaled vibrational frequencies of the [Zn(OH<sub>2</sub>)<sub>6</sub><sup>2+</sup>] were reported. The unscaled vibrational frequencies of the ZnO<sub>6</sub> unit are lower than the experimental frequencies (<i>ca</i>. 15%), but scaling the frequencies reproduces the measured frequencies. The theoretical binding enthalpy for [Zn(OH<sub>2</sub>)<sub>6</sub><sup>2+</sup>] was calculated and accounts for <i>ca</i>. 64% of the experimental single ion hydration enthalpy for Zn(II). <i>Ab</i><i>initio</i> geometry optimizations and frequency calculations are also reported for a [Zn(OH<sub>2</sub>)<sub>18</sub><sup>2+</sup>] (Zn[6+12]) cluster with 6 water molecules in the first sphere and 12 water molecules in the second sphere. The global minimum corresponds with <i>T</i> symmetry. Calculated frequencies of the zinc [6+12] cluster correspond well with the observed frequencies in solution. The ν<sub>1</sub> ZnO<sub>6</sub> (unscaled) mode occurs at 389 cm<sup>-1</sup> in good agreement with the experimental value. The theoretical binding enthalpy for [Zn(OH<sub>2</sub>)<sub>18</sub><sup>2+</sup>] was calculated and is very close to the experimental single ion hydration enthalpy for Zn(II). The water molecules of the first sphere form strong H-bonds with water molecules in the second hydration shell because of the strong polarizing effect of the Zn(II) ion. The importance of the second hydration sphere is discussed.

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