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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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766 Roland Schmid<br />

E r = E i + E s [13.1.25]<br />

where:<br />

Ei inner-sphere reorganization energy<br />

Es solvent reorganization energy<br />

For outer-sphere ET the solvent component Es <strong>of</strong> the reorganization energy<br />

E s = e 2 c og [13.1.26]<br />

is the product <strong>of</strong> the medium-dependent Pekar factor c o =1/ε ∞ -1/ε sand a reactant-dependent<br />

(but solvent independent) geometrical factor<br />

g = 1/2R a + 1/2R d -1/R [13.1.27]<br />

where:<br />

R the donor-acceptor separation<br />

e the electron charge<br />

Further advancements included calculations <strong>of</strong> the rate constant preexponent for<br />

nonadiabatic ET, 132 an account <strong>of</strong> inner-sphere 133 and quantum intramolecular 134-136 vibrations<br />

<strong>of</strong> reactants and quantum solvent modes. 137,138 The main results were the formulation<br />

<strong>of</strong> the dependencies <strong>of</strong> the activation energy on the solvent dielectric properties and reactant<br />

sizes, as well as the bell-shaped relationship between ΔF and ΔFo. The predicted activation<br />

energy dependence on both the solvent dielectric properties 139,140 and the donor-acceptor<br />

distance 141 has, at least qualitatively, been supported by experiment. A bell-shaped plot <strong>of</strong><br />

ΔF vs ΔFowas obtained for ET in exciplexes, 142 ion pairs, 143 intramolecular 144 and<br />

outer-sphere 145 charge shift reactions. However, the symmetric dependence predicted by eq.<br />

[13.1.24] has not yet been detected experimentally. Instead, always asymmetric plots <strong>of</strong> ΔF<br />

against ΔFo are obtained or else, in the inverted region (ΔFo

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