HYDROPHOBIC HYDRATION STRUCTURES OF TRIS(1,10-PHENANTHROLINE)METAL AND TRIS(2,2'-BIPYRIDINE)METAL COMPLEX-IONS AND EFFECT OF THE IONIC CHARGE - X-RAY-DIFFRACTION STUDY WITH ISOMORPHOUS SUBSTITUTION
H. Yokoyama et al., HYDROPHOBIC HYDRATION STRUCTURES OF TRIS(1,10-PHENANTHROLINE)METAL AND TRIS(2,2'-BIPYRIDINE)METAL COMPLEX-IONS AND EFFECT OF THE IONIC CHARGE - X-RAY-DIFFRACTION STUDY WITH ISOMORPHOUS SUBSTITUTION, Bulletin of the Chemical Society of Japan, 70(10), 1997, pp. 2357-2367
X-Ray diffraction measurements have been made for aqueous solutions of
sulfates or chlorides of [Ru(phen)(3)](2+), [Ni-(phen)(3)](2+), [Ru(b
py)(3)](2+), [Ni(bpy)(3)](2+), [Rh(bpy)(3)](3+), and [Cr(bpy)(3)](3+)
(phen = 1,10-phenanthroline, bpy = 2,2'-bipyridine), Radial distributi
on functions for the metal interactions were obtained by the isomorpho
us substitution between ruthenium(II) and nickel(II) complexes or betw
een rhodium(III) and chromium(III) complexes. Metal-nitrogen and metal
-carbon distances within the complex ions in solution were essentially
in agreement with those in the crystals. Regarding the divalent metal
complexes, about two water molecules seemed to exist at a distance of
3.5-3.6 Angstrom (1 Angstrom = 10(-10) m) from the central metal atom
and 10-11 water molecules existed in the region of 5.3 to 6.3 Angstro
m, probably in the vicinity of peripheral hollows along the C-3 axis o
f the complex. Further, large broad peaks with high electron density w
ere observed around 7.7 and 11.2 Angstrom for the [Ru(bpy)(3)](2+) ion
and around 8.0 and 11.5 Angstrom for the [Ru(phen)(3)](2+) ion, almos
t independent of salt concentration and kinds of counter ions. These w
ere attributed to the hydrophobic hydration shells having the hydrogen
-bonded network structure. The hydration structure of the trivalent me
tal complexes was significantly different from that observed for the d
ivalent ones: 14-15 water molecules existed in the range of 4.7 to 6.0
Angstrom, a part of them presumably in the hollows along the C-2 axes
of the complex, and only a single broad peak was observed around 7.7
Angstrom as the hydrophobic hydration shell. These results indicated t
hat the hydrophobic hydration structure was reduced by the increase of
the ionic charge, as predicted from a comparison of temperature coeff
icients of the Walden product obtained by the conductivity measurement
s of dilute solutions.