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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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10.2 Effect <strong>of</strong> polymer/solvent acid-base interactions 575<br />

The principle states that hard acid prefers to interact with a hard base, and vice versa, a<br />

s<strong>of</strong>t acid with a s<strong>of</strong>t base. A hard-hard interaction is fast because <strong>of</strong> large Coulombic attraction,<br />

a s<strong>of</strong>t-s<strong>of</strong>t interaction is fast because <strong>of</strong> large orbital overlap between HOMO and<br />

LUMO. However the problem is, what is the physical meaning <strong>of</strong> hardness?<br />

10.2.1.2.3 Density functional theory<br />

Parr and al. 12 gave in 1988 a theoretical support to the absolute hardness. In the density functional<br />

theory two basic parameters were introduced. Any chemical system can be characterized<br />

by its chemical potential, µ, and its absolute hardness, η. The chemical potential<br />

measures the escaping tendency <strong>of</strong> an electronic cloud, while absolute hardness determines<br />

the resistance <strong>of</strong> the species to lose electrons. The exact definitions <strong>of</strong> these quantities are:<br />

∂<br />

∂<br />

μ = η<br />

∂<br />

∂<br />

⎛ ⎞<br />

⎜ ⎟ =<br />

⎝ ⎠<br />

⎛ 2<br />

E<br />

1 E ⎞<br />

and ⎜<br />

⎟<br />

2<br />

N<br />

2<br />

⎟<br />

⎝ N ⎠<br />

ν ν<br />

[10.2.3]<br />

where :<br />

µ chemical potential<br />

η absolute hardness<br />

E electronic energy<br />

N number <strong>of</strong> electrons<br />

ν potential due to the nuclei plus any external potential.<br />

However, according to frontier orbital method, 13 the relationship between η and the<br />

HOMO and LUMO energies is reduced to:<br />

1<br />

η≈− −<br />

2<br />

( E E )<br />

HOMO LUMO [10.2.4]<br />

where :<br />

η absolute hardness<br />

EHOMO energy level <strong>of</strong> the HOMO orbital<br />

ELUMO energy level <strong>of</strong> the LUMO orbital.<br />

Of course the absolute s<strong>of</strong>tness is the reciprocal <strong>of</strong> the absolute hardness. The apparent<br />

success <strong>of</strong> the density-functional theory is to provide two parameters from which we can<br />

calculate the number <strong>of</strong> electrons transferred, resulting mainly from the charge transfer between<br />

two molecules, i.e., from electrons flow until chemical potential reaches an equilibrium.<br />

As a first approximation, the number <strong>of</strong> electron transferred is given 14 by:<br />

N Trans<br />

μ −μ<br />

=<br />

2<br />

B A<br />

( η −η<br />

)<br />

A B<br />

[10.2.5]<br />

where:<br />

Ntrans number <strong>of</strong> electrons transferred<br />

µ A chemical potential <strong>of</strong> the acid<br />

µ B chemical potential <strong>of</strong> the base<br />

ηA absolute hardness <strong>of</strong> the acid<br />

ηB absolute hardness <strong>of</strong> the base.<br />

This number varies from 0 to 1 and it is in most cases a fractional number. As an<br />

example 15 for the interaction between Cl2 and substituted aromatic compounds, Ntrans varies

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