Here no doubt the sources of electrical excitement are the points of
contact of the zinc and platinum, where, as we see by our last article,
we have electrical separation produced. But this of itself would not
produce a current, for an electrical current implies very considerable
energy, and must be fed by something. Now, in the voltaic battery we
have two things which accompany each other, and which are manifestly
connected together. In the first place we have the combustion, or
at least the oxidation and dissolution, of the zinc; and we have,
secondly, the production of a powerful current. Now, evidently, the
first of these is that which feeds the second, or, in other words, the
energy of chemical separation of the metallic zinc is transmuted into
that of an electrical current, the zinc being virtually burned in the
process of transmutation.
170. Finally, as far as we are aware, the energy of chemical separation
is not directly transmuted into radiant light and heat.
_Electrical Separation._
171. In the first place the energy of electrical separation is
obviously transmuted into that of _visible motion_, when two oppositely
electrified bodies approach each other.
172. Again, it is transmuted into a _current of electricity_, and
ultimately into heat, when a spark passes between two oppositely
electrified bodies.
It ought, therefore, to be borne in mind that when the flash is seen
there is no longer electricity, what we see being merely air, or some
other material, intensely heated by the discharge. Thus a man might
be rendered insensible by a flash of lightning without his seeing the
flash--for the effect of the discharge upon the man, and its effect in
heating the air, might be phenomena so nearly simultaneous that the man
might become insensible before he could perceive the flash.
_Electricity in Motion._
173. This energy is transmuted into that of _visible motion_ when two
wires conveying electrical currents in the same direction attract each
other. When, for instance, two circular currents float on water, both
going in the direction of the hands of a watch, we have seen from Art.
100 that they will move towards each other. Now, here there is, in
truth, a lessening of the intensity of each current when the motion is
taking place, for we know (Art. 104) that when a circuit is moved into
the presence of another circuit conveying a current, there is produced
by induction a current in the opposite direction; and hence we perceive
that, when two similar currents approach each other, each is diminished
by means of this inductive influence--in fact, a certain amount of
current energy disappears from existence in order that an equivalent
amount of the energy of visible motion may be produced.
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