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14. Estimation of Distance between the Metal Complex Ion and the Closest Solvent Water Molecules from Density Data
Katsumi Kurotaki
Keywords: aqueous solution, metal complex, density
Contrary to Archimedes' principle, the level of water in a test tube drops when electrolytes such as CuSO4 are dissolved in the water and dissociate into ions. This is due to the interaction between ions and water molecules around the ions; water molecules in the hydrogen-bonded network of water are oriented toward an ion by the strong electrostatic force of the ion leading to an increase of packing fraction of water molecules and an abnormal negative V0 calculated from density data for these ions, where V0 is the molar volume of ion at infinite dilution in water. Electrolyte solution theory predicted the magnitude of the electrostatic effect on V0. However, the V0 of multivalent metal ion deviates from the theoretical one because multivalent metal ions interact with water molecules by coordination bond formation as well as electrostatic force. On the other hand, the metal complex ions and peroxyanions, [MLn]z± whose M have no electrons for a bond with water molecules, interact with water in a purely electrostatic way (where M is metal ion of all kinds, L is NH3, diamine/2, F-, Cl-, CN-, NO2- and O, 1
z
4). Then the V0 of [MLn]z ± was analyzed on the basis of electrolyte solution theory and scaled particle theory (SPT). For a series of [MLn]z ± having an identical L, linear relationships are observed between the M-X bond distance, rMX and the intrinsic volume, Vcav(MLn) which is equal to the volume of water displaced by them, where X is the coordination atom. The value of dVcav(MLn)/drMX increased with increasing rMX. These data were analyzed with the model of an MXn core where the sphere M* (radius rM*) is overlapped by n spheres (radii rX) which are apart by rMX from M. Assuming that rM* = (rMX + rX)cos
, a self-consistent set of rM* and
is determined from the experimental value of dVcav(MLn)/drMX which is equal to cos
dVcav(M*sphere)/drM*, where
is the angle between the MX bond and the closest water molecules in contact with M*. The sum of rM* and the radius of water molecule (155 pm), rw is equal to the distance between M and the closest water molecules, rMw'2. Table 2 shows the values of rMw'2, nw'2 and dVcav(MLn)/drMX, where nw'2 is the hydration number. These data are consistent with the structural data determined by X-ray diffraction. This is the first evidence that there is a clear relationship between thermodynamic and structure data for aqueous electrolyte solution.
| dVcav (MLn) /dr MX / cm3 mol-1 pm-1 |
rM w'2, pm-1 |
n w'2 |
|
| [MF6]z- | 0.54 | 393 | 13-14 |
| [M(am)6]z+ [M(CN)6]z- [M(ox)3]z- |
0.62 | 407 | 13-14 |
| [MCl6]z- |
0.83 | 461 | 13-14 |
| MO4z- |
0.32 | 359 | 11 |
Publications:
Kurotaki, K. and Kawamura, S.: J. Chem. Soc. Faraday Trans., 94, 2939- 2943, 1998.