CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
CHEM01200604005 A. K. Pathak - Homi Bhabha National Institute
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However, these calculations do not lead to any significant change in the structural<br />
parameters of these hydrated clusters.<br />
2.3.2. Solvent Stabilization and Interaction Energy<br />
where E I<br />
The stabilzation energy of I 2 •− .nH 2 O clusters can be expressed as<br />
solv<br />
E = E . − − ( nE E<br />
I nH O HO+<br />
. −),<br />
. I<br />
. −<br />
2 2<br />
. nH O<br />
2 2 2 2<br />
, E HO 2<br />
and E<br />
I2<br />
.− refer to the total energy of the cluster I 2 •− .nH 2 O, the<br />
energy of a single H 2 O molecule and the energy of the bare I 2 •− system, respectively.<br />
Thus, E solv essentially refers to the total interaction energy of the solute with n solvent<br />
H 2 O units around it in the hydrated cluster of size n. A number of minimum energy<br />
configurations are obtained in these hydrated clusters and it is increasing with the size (n)<br />
of the cluster. It is understood that at a particular temperature there will be a statistical<br />
contribution of the conformers of a particular size to the overall property. So the<br />
weighted average solvent stabilization energy ( E w<br />
solv<br />
) values are calculated and provided<br />
in Table 1. The plot for the variation of E w<br />
solv<br />
vs. n is shown in Fig. 2.5(a). The weight<br />
factor of a conformer within a particular size (n) of the cluster is calculated based on the<br />
Boltzmann statistical population of the conformer at 150 K. It is observed that E w<br />
solv<br />
varies linearly with n, the number of water molecules in the hydrated clusters and the<br />
variation of E w<br />
solv<br />
is best fitted as<br />
E w<br />
solv<br />
= -0.83 + 11.25 n,<br />
When, E w<br />
solv<br />
is expressed in kcal/mol and n is the number of water molecules. This linear<br />
fitted plot has correlation coefficient ~ 0.999 promising the power of prediction of<br />
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