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Handbook of Solvents - George Wypych - ChemTech - Ventech!

Handbook of Solvents - George Wypych - ChemTech - Ventech!

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28 Estanislao Silla, Arturo Arnau and Iñaki Tuñón<br />

ing superficially the influence that the solvent has on one <strong>of</strong> the equilibria <strong>of</strong> greatest relevance,<br />

the acid-base equilibrium.<br />

The solvent can alter an acid-base equilibrium not only through the acid or basic character<br />

<strong>of</strong> the solvent itself, but also by its dielectric effect and its capacity to solvate the different<br />

species which participate in the process. Whilst the acid or basic force <strong>of</strong> a substance<br />

in the gas phase is an intrinsic characteristic <strong>of</strong> the substance, in solution this force is also a<br />

reflection <strong>of</strong> the acid or basic character <strong>of</strong> the solvent and <strong>of</strong> the actual process <strong>of</strong> solvatation.<br />

For this reason the scales <strong>of</strong> acidity or basicity in solution are clearly different from<br />

those corresponding to the gas phase. Thus, toluene is more acid than water in the gas phase<br />

but less acid in solution. These differences between the scales <strong>of</strong> intrinsic acidity-basicity<br />

and in solution have an evident repercussion on the order <strong>of</strong> acidity <strong>of</strong> some series <strong>of</strong> chemical<br />

substances. Thus, the order <strong>of</strong> acidity <strong>of</strong> the aliphatic alcohols becomes inverted on passing<br />

from the gas phase to solution:<br />

R'<br />

R'<br />

in gas phase: R CH2 OH < R CH OH < R C OH<br />

R'<br />

R'<br />

in solution: R CH2 OH > R CH OH ><br />

R C OH<br />

The protonation free energies <strong>of</strong> MeOH to t-ButOH have been calculated in gas phase<br />

and with a continuum model <strong>of</strong> the solvent. 61 It has been shown that in this case continuum<br />

models gives solvation energies which are good enough to correctly predict the acidity ordering<br />

<strong>of</strong> alcohols in solution. Simple electrostatic arguments based on the charge<br />

delocalization concept, were used to rationalize the progressive acidity <strong>of</strong> the alcohols when<br />

hydrogen atoms are substituted by methyl groups in the gas phase, with the effect on the solution<br />

energies being just the opposite. Thus, both the methyl stabilizing effect and the electrostatic<br />

interaction with the solvent can explain the acid scale in solution. As both terms are<br />

related to the molecular size, this explanation could be generalized for acid and base equilibria<br />

<strong>of</strong> homologous series <strong>of</strong> organic compounds:<br />

AH ⇔ A - +H +<br />

B+H + ⇔BH +<br />

In vacuo, as the size becomes greater by adding methyl groups, displacement <strong>of</strong> the<br />

equilibria takes place toward the charged species. In solution, the electrostatic stabilization<br />

is lower when the size increases, favoring the displacement <strong>of</strong> the equilibria toward the neutral<br />

species. The balance between these two tendencies gives the final acidity or basicity ordering<br />

in solution. Irregular ordering in homologous series are thus not unexpected taking<br />

into account the delicate balance between these factors in some cases. 62<br />

2.1.4.2 Solvent effects on the rate <strong>of</strong> chemical reactions<br />

When a chemical reaction takes place in the midst <strong>of</strong> a solution this is because, prior to this,<br />

the molecules <strong>of</strong> the reactants have diffused throughout the medium until they have met.<br />

This prior step <strong>of</strong> the diffusion <strong>of</strong> the reactants can reach the point <strong>of</strong> conditioning the performance<br />

<strong>of</strong> the reaction, especially in particularly dense and/or viscous surroundings. This<br />

is the consequence <strong>of</strong> the liquid phase having a certain microscopic order which, although<br />

R''<br />

R''

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