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94 PRACTICAL ORGANIC CHEMISTRY [II.<br />

(compare previous paragraph). The flask is then heated with a small<br />

flame, protected from draughts so as to ensure a uniform heating ; an air<br />

bath (Fig. //, 5, 3) gives better results. The initial heating must not be<br />

hurried as owing to the considerable extra condensation which occurs<br />

whilst the column is warming up, the latter may easily choke with liquid.<br />

Once distillation has commenced, the size of the flame is adjusted so that<br />

the liquid passes over at the rate of one drop every two or three seconds.<br />

Under these conditions fairly efficient fractionation should be obtained.<br />

When the low boiling point fraction has passed over, distillation should<br />

cease. The heating is then slowly increased, and a sharp rise in boiling<br />

point should occur as the second fraction commences to distil; it is<br />

assumed, of course, that the fractionating system is capable of effecting<br />

a sharp fractionation of the components of the mixture. If the set-up is<br />

inefficient, a relatively large intermediate fraction may be obtained. It<br />

is desired to emphasise the fact that the distillation must be conducted<br />

slowly ; no time is usually saved by distilling rapidly since a second<br />

fractionation will then be necessary.<br />

11,17. IMPROVED APPARATUS FOR FRACTIONAL<br />

DISTILLATION<br />

A detailed discussion of the theory underlying modern developments<br />

in fractional distillation is outside the scope of this volume,* but a brief<br />

description of the terms used in discussing fractionating columns and the<br />

chief desiderata of efficient columns will be given. The capacity of a<br />

column is a measure of the quantity of vapour and liquid which can be<br />

passed counter-current to each other in a column without causing it to<br />

choke or flood. The efficiency of a column is the separating power of a<br />

definite length of the column; it is measured by comparing the performance<br />

of the column with that calculated for a theoretically perfect plate<br />

column under similar conditions. A theoretical plate is defined as a<br />

section of a distilling column of such length that the vapour comes to<br />

equilibrium with the liquid, i.e., the vapour leaving the " plate " has the<br />

same composition as the vapour entering it and the vapour ascending<br />

from the " plate " is in equilibrium with the hquid descending from it.<br />

The number of theoretical plates cannot be determined from the dimensions<br />

of the fractionating column ; it is computed from the separation<br />

effected by distillation of a hquid mixture {e.g., benzene and toluene ;<br />

benzene and carbon tetrachloride ; benzene and dichloroethane ; nheptane<br />

and methylci/cZohexane), the vapour and hquid compositions of<br />

which are accurately known.f An ordinary one cm. tube one metre long<br />

might be equivalent to only one theoretical plate, whilst the same tube<br />

filled with a suitable packing can give the equivalent of 20 or more<br />

theoretical plates. A column with 12 theoretical plates is satisfactory<br />

for the <strong>practical</strong> separation of a mixture of benzene and toluene. The<br />

effectiveness of a column depends upon the height as well as upon the<br />

* See, for example, A. Weissberger (Editor), Technique of Organic Chemistry, Volume IV.<br />

Distillation, 1951 (Interscience).<br />

t For experimental details, see, for example, Daniels, Matthews and Williams, Expert*<br />

mental Physical Chemistry, 4th Edition, 1949, p. 95 (McGraw-Hill).

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