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Handbook of Solvents - George Wypych - ChemTech - Ventech!

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21.2 Ionic liquids 1461<br />

be used. This lack <strong>of</strong> predictive power and the overall general lack <strong>of</strong> physical property data<br />

in the literature will inevitably slow the transfer <strong>of</strong> ionic liquid technology into industrial<br />

processes.<br />

21.2.2 FUNDAMENTAL PRINCIPLES OF THE FORMATION OF ROOM<br />

TEMPERATURE IONIC LIQUIDS<br />

A number <strong>of</strong> detailed reviews and articles have been published recently on the theory and<br />

development behind ionic liquid technology. 15-25 However in order to develop a greater understanding<br />

and appreciation <strong>of</strong> these solvents, we will summarize the main points here.<br />

Therefore the purpose <strong>of</strong> this section is to give an introduction to the nature and properties<br />

<strong>of</strong> room-temperature ionic liquids, with particular emphasis being placed upon their potential<br />

as solvents for industrially relevant catalytic reactions, and (more generally) for clean<br />

technology.<br />

21.2.2.1 Development <strong>of</strong> ionic liquids<br />

To begin with, the melting point <strong>of</strong> a salt is related to its lattice energy. In fact, if one was to<br />

plot the lattice energy <strong>of</strong> a series <strong>of</strong> salts, for instance the Group 1 halides, against the melting<br />

points in Kelvin, then one can see that there is reasonable linearity between the melting<br />

point and the lattice energy (see Figure 21.2.1).<br />

Although not particularly accurate, this simple approach will give an estimated melting<br />

point <strong>of</strong> the Group 1 salts if the lattice energy is known. The deviations from this treatment<br />

are frequent and are usually due to other forms <strong>of</strong> bonding within the structure, as shall<br />

be explained later. The first theoretical treatment <strong>of</strong> lattice energy began with Born and<br />

Landé, and was then further developed by Kapustinskii 28 into the what is know as the<br />

“Kapustinskii equation” (eqn. [21.2.1]):<br />

+ −<br />

287. 2vZ<br />

Z ⎛ 0. 345 ⎞<br />

U = ⎜ −<br />

r ⎜<br />

1 ⎟<br />

⎝ r ⎟<br />

0 0 ⎠<br />

[21.2.1]<br />

where:<br />

U lattice energy<br />

v number <strong>of</strong> ions per molecule<br />

r0 sum <strong>of</strong> ionic radii<br />

Z + ,Z -<br />

charge <strong>of</strong> the ionic species<br />

Therefore by increasing the value <strong>of</strong> r0, i.e., by using larger anionic and cationic components<br />

in the salt, it is possible to lower this energy and therefore reduce the melting point.<br />

This effect is shown Table 21.2.1.<br />

Table 21.2.1. Melting points 27 <strong>of</strong> various inorganic salts, melting points given in ºC<br />

Anion Lithium Sodium Potassium Rubidium Caesium<br />

Fluoride 842 988 846 775 682<br />

Chloride 614 801 776 718 645<br />

Bromide 550 747 734 693 636<br />

Iodide 450 661 686 647 626<br />

From this one can clearly see that as we increase both the size <strong>of</strong> the anion and the cation,<br />

the melting point decreases. From the Kapustinskii equation one must also note that by

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