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have shown, by the increase of number in the pairs that com-
pose the compound battery, but without an increase of size.
We conclude, then, that a galvanic current is great in quan-
tity, and capable for chemical action, if produced by a single
pair or more, much in proportion to the size and action of the
pair if connected with a thick wire. The density, tension, and
intensity of the current for passing over and through poor con-
ductors will be much in proportion to the number of the series,
and the smaller size of the wire connections and conductors.
The efficiency of every battery depends upon good contacts.
This is mentioned particularly, because the greatest and most
frequent failures, partial failures, or differences of results, arise
from this want of exact care.
There is another method for increasing the electro-motive
force of even a small galvanic current of a single pair, as well
as some modified kind of intensity; but this must be reserved
for the next chapter.
Derived currents, spoken of by authors, are those that are
obtained by a sort of by-path, namely, when the conductor of a
closed circuit is conveying a galvanic current, this is termed the
primary current. If, now, we add a short and nearly parallel
conductor by making contact at its metallic ends, on the route
of the primitive wire, a portion of the current will pass along
the second wire, provided it is not much longer nor smaller, nor
otherwise a poorer conductor, than the primary wire. And this
is termed a derived current. The author, however, finds no use
for such in therapeutics.
Electric Heat.
Heat can be produced by an obstructed or retarded current
of electricity, as, for instance, where a large quantity current is
led by a wire too small to convey it all freely, or through a poor
conductor, as platinum. It may be evolved by the disruptive
discharge between the two poles of a galvanic battery, where
disintegration is effected, and the particles of one pole pass over
to the other pole, with the evolution of intense heat and light.