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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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P <br />

<br />

7<br />

P , , P , ,, 1 ∂<br />

<br />

2 ∂ P<br />

, ,,<br />

1 6 <br />

∂<br />

∂ P<br />

, ,,<br />

…………………<br />

8<br />

where, the averages of fluctuation of the number of solvent particles are defined as<br />

<br />

P 0<br />

<br />

<br />

P for m 1<br />

<br />

9<br />

9<br />

In the homogeneous limit, one can write<br />

P , , <br />

g i(r,ω); P , ,, <br />

g i(r,ω)<br />

10<br />

where, ρ and ρ represent the ion and solvent density, respectively, and r r d r s .<br />

Approximating the average density (=/V) to be equal to the solvent density, Eq.(6 ) can<br />

be reduced to<br />

g , g , , 1 ρ ∂ <br />

2 n ∂ρ ρg , , <br />

1 <br />

6 <br />

ρ <br />

<br />

∂ <br />

∂ρ ρg , , .<br />

11<br />

The effect of a single ion on g , enters through the fluctuation of the number of<br />

solvent particles and pair distribution g , , for the finite system. For simplicity, the<br />

effect of a single ion on the fluctuation of the number of solvent particles is neglected.<br />

This approximation is a reasonably good one if the system contains an appreciable<br />

127

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