lectric current; and it is doubtful whether a case of electrolyzation can
occur, where, being present, it is not resolved into its first principles.
672. The various oxides, chlorides, iodides, and salts, which I have shown
are decomposable by the electric current when in the liquid state, under
the same general law with water (402.), illustrate in an equally striking
manner the activity, in such decompositions, of elements directly and
powerfully opposed to each other by their chemical relations.
673. On the other hand, bodies dependent on weak affinities very rarely
give way. Take, for instance, glasses: many of those formed of silica,
lime, alkali, and oxide of lead, may be considered as little more than
solutions of substances one in another[A]. If bottle-glass be fused, and
subjected to the voltaic pile, it does not appear to be at all decomposed
(408.). If flint glass, which contains substances more directly opposed, be
operated upon, it suffers some decomposition; and if borate of lead glass,
which is a definite chemical compound, be experimented with, it readily
yields up its elements (408.).
[A] Philosophical Transactions, 1830, p. 49.
674. But the result which is found to be so striking in the instances
quoted is not at all borne out by reference to other cases where a similar
consequence might have been expected. It may be said, that my own theory of
electro-chemical decomposition would lead to the expectation that all
compound bodies should give way under the influence of the electric current
with a facility proportionate to the strength of the affinity by which
their elements, either proximate or ultimate, are combined. I am not sure
that that follows as a consequence of the theory; but if the objection is
supposed to be one presented by the facts, I have no doubt it will be
removed when we obtain a more intimate acquaintance with, and precise idea
of, the nature of chemical affinity and the mode of action of an electric
current over it (518. 524.): besides which, it is just as directly opposed
to any other theory of electro-chemical decomposition as the one I have
propounded; for if it be admitted, as is generally the case, that the more
directly bodies are opposed to each other in their attractive forces, the
more powerfully do they combine, then the objection applies with equal
force to any of the theories of electrolyzation which have been considered,
and is an addition to those which I have take
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