The Phase Rule and Its ApplicationsFindlay, Alexander
Science
The Phase Rule and Its Applications
Findlay, Alexander
Chemistry, Physical and theoretical; Phase rule and equilibrium; Solution (Chemistry)
Phases.--Before proceeding farther we shall first consider what exactly is
meant by the terms _phase_ and _component_. We have already seen (p. 5)
that a heterogeneous system is made {9} up of different portions, each in
itself homogeneous, but marked off in space and separated from the other
portions by bounding surfaces. These homogeneous, physically distinct and
mechanically separable portions are called _phases_. Thus ice, water, and
vapour, are three phases of the same chemical substance--water. A phase,
however, whilst it must be physically and chemically homogeneous, need not
necessarily be chemically simple. Thus, a gaseous mixture or a solution may
form a phase; but a heterogeneous mixture of solid substances constitutes
as many phases as there are substances present. Thus when calcium carbonate
dissociates under the influence of heat, calcium oxide and carbon dioxide
are formed. There are then _two_ solid phases present, viz. calcium
carbonate and oxide, and one gas phase, carbon dioxide.
The _number of phases_ which can exist side by side may vary greatly in
different systems. In all cases, however, there can be but one gas or
vapour phase on the account of the fact that all gases are miscible with
one another in all proportions. In the case of liquid and solid phases the
number is indefinite, since the above property does not apply to them. The
number of phases which can be formed by any given substance or group of
substances also differs greatly, and in general increases with the number
of participating substances. Even in the case of a single substance,
however, the number may be considerable; in the case of sulphur, for
example, at least eight different solid phases are known (_v._ Chap. III.).
It is of importance to bear in mind that equilibrium is _independent of the
amounts_ of the phases present.[13] Thus it is a familiar fact that the
pressure of a vapour in contact with a {10} liquid (_i.e._ the pressure of
the saturated vapour) is unaffected by the amounts, whether relative or
absolute, of the liquid and vapour; also the amount of a substance
dissolved by a liquid is independent of the amount of solid in contact with
the solution. It is true that deviations from this general law occur when
the amount of liquid or the size of the solid particles is reduced beyond a
certain point,[14] owing to the influence of surface energy; but we have
already (p. 5) excluded such cases from consideration.
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