MOLECULAR-DYNAMICS SIMULATION STUDY OF LANTHANIDE IONS LN(3-SOLUTION - ANALYSIS OF THE STRUCTURE OF THE FIRST HYDRATION SHELL AND OF THE ORIGIN OF SYMMETRY FLUCTUATIONS() IN AQUEOUS)
T. Kowall et al., MOLECULAR-DYNAMICS SIMULATION STUDY OF LANTHANIDE IONS LN(3-SOLUTION - ANALYSIS OF THE STRUCTURE OF THE FIRST HYDRATION SHELL AND OF THE ORIGIN OF SYMMETRY FLUCTUATIONS() IN AQUEOUS), Journal of physical chemistry, 99(35), 1995, pp. 13078-13087
We have analyzed molecular dynamics simulations of tripositive lanthan
ide ions Ln(3+) in aqueous solution. Combining a variety of new approa
ches for the analysis and the visualization of the first hydration she
lls, we were able to extract in detail their angular structure and the
ir dynamic behavior along the series of Ln(3+) ions. For a heavy lanth
anide ion (Yb3+) the eight water molecules of the first hydration shel
l form a well-defined square antiprism, whereas for a nine-coordinate
light lanthanide ion (Nd3+) the first hydration shell adopts the trica
pped trigonal prism geometry. In the middle of the series both geometr
ies coexist. Both the square antiprism and the tricapped trigonal pris
m rearrange via 90 degrees pseudorotations of the main symmetry axis.
The pertaining transition state of lowered symmetry is a dodecahedron
for the Yb3+ octaaqua complex and a capped square antiprism for the Nd
3+ enneaaqua complex. The lifetime of a square antiprism between two p
seudorotations is 11 ps but amounts to only 2 ps for a tricapped trigo
nal prism. The Lifetime of a square antiprism from the simulation of Y
b3+ (CN = 8) is in quantitative agreement with the correlation time fo
r the fluctuation of the zero-field splitting from experimental EPR sp
ectra of the Gd3+ octaaqua complex. This correlation time, of relevanc
e for the understanding of the mechanism of the H-1 relaxation of Gd3-based MRI contrast agents, is linked to transient distorsions of the
Gd3+ aqua complex from perfect symmetry that were so far assumed to be
due to random impacts of solvent molecules. On the basis of our MD-si
mulations we can go beyond these general notions and propose a model w
ith 90 degrees pseudorotations of the coordination polyhedron as the p
rincipal mechanism for distorsions of the first hydration shell.