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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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140 Abraham Nitzan<br />

Figure 4.3.1. The electrostatic response potential <br />

induced by the solvent at the position <strong>of</strong> the solute ion,<br />

as a function <strong>of</strong> the solute charge. Dashed line - the<br />

Stockmayer-CH 3Cl model described in Section 4. Full<br />

and dotted lines, model polyether solvents described in<br />

the text. [From Ref. 11b].<br />

Figure 4.3.2. The linear response relaxation function<br />

C(t) (dashed and dotted lines] and the non-equilibrium<br />

solvation function S(t) (solid line) computed for the<br />

Stockmayer-CH 3Cl model described in Section 4. In<br />

the nonequilibrium simulation the ion charge is<br />

switched on att=0.Thedotted and dashed lines represent<br />

C(t) obtained from equilibrium simulations with<br />

uncharged and charged ion, respectively. [From Ref.<br />

11a].<br />

A typical timestep for these simulation is 3fs. In the absence <strong>of</strong> thermalization this<br />

gives energy conservation to within 10 -4 over ~80,000 time steps. After equilibrating the<br />

system at 240K, the equilibrium correlation function C(t) is evaluated from equilibrium trajectories<br />

with both a charged (q = e) and an uncharged (q = 0) impurity atom. The non-equilibrium<br />

solvation function S(t) can also be computed from trajectories that follow a step<br />

function change in the ion charge from q=0toq=e.These calculations are done for the<br />

CH 3Cl solvent model characterized by the above parameters and for similar models with<br />

different parameters. In particular, results are shown below for systems characterized by<br />

different values <strong>of</strong> the parameter 15<br />

2<br />

p′ = I /2Mσ<br />

[4.3.35]<br />

which measures the relative importance <strong>of</strong> rotational and translational solvent motions.<br />

4.3.5 NUMERICAL SIMULATIONS OF SOLVATION IN SIMPLE POLAR<br />

SOLVENTS: RESULTS AND DISCUSSION<br />

The dashed line <strong>of</strong> Figure 4.3.1 shows the equilibrium solvent induced electrostatic potential<br />

Φ at the position <strong>of</strong> the ion, as a function <strong>of</strong> the ion charge q obtained for the<br />

Stockmayer-CH3Cl model described in Section 4. Clearly the solvent response is linear with<br />

qallthewayuptoq=e,with slight deviations from linearity starting atq>e.Theslope (~4)<br />

<strong>of</strong> the linear dependence <strong>of</strong> the dashed line in Figure 1 (for q < e) is considerably smaller<br />

from that obtained from Φ=q/aε s (taking a = σA/2 gives a slope <strong>of</strong> 7.4) that is used to get<br />

Eq. [4.3.1]. A more advanced theory <strong>of</strong> solvation based on the mean spherical approximation<br />

predicts (using σA and σD for the diameters <strong>of</strong> the ion and the solvent, respectively) a<br />

slope <strong>of</strong> 4.6.<br />

The linearity <strong>of</strong> the response depends on the nature <strong>of</strong> the solvent. As examples Figure<br />

4.3.1 also shows results obtained for models <strong>of</strong> more complex solvents, H(CH2OCH2) nCH3

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