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Iii 1831, Professor Henry, one of our American philosophers,
was the first to discover this peculiar action of a long conductor
when extended, and also, when coiled into a helix, as so modify-
ing or increasing the current of a single galvanic pair at the
moment when it ceases to flow. He was the first to employ coils
of metallic ribbon for obtaining sparks and shocks from a single
galvanic pair. By this means the brilliancy and power of the
spark are very greatly increased whenever the circuit is broken.
Thus far had this branch of science advanced when in the same
year Professor Faraday, of England, discovered that an electric
current, as well as a magnet, is able by induction to develop elec-
tric currents in conducting wires. This he proved by placing on
an insiilating plane two parallel conducting wires very near to
each other, but without touching. The two ends of one of
these wires are connected with the poles of a galvanic battery,
so that it in fact becomes the connecting wire between the two
poles of that battery. The two ends of the other wire are con-
nected with the extremities of a sensitive galvanometer, simply
to judge of the electric movement in this wire, if any, by the
deviations of the needle of the instrument. At the moment
the battery current commenced to flow through the first wire,
the needle of the instrument is seen to deviate at first, then to
quiver and oscillate, and finally to come back to an equilibrium,
which remains at zero, just as it was before the current was let
on the first wire; and thus it remains undisturbed as long as
the current of the battery continues to traverse the neighboring
wire; but the instant the current is interrupted in the first
wire, the needle suffers another deflection, and this in a con-
trary direction to that which occurred at the closure of the
current. Thus he proved that the galvanic current which
coiirses through the one wire, determines an instantaneous but
opposite current in the other wire at the moment when it begins
to flow, and another equally instantaneous reverse current at the
moment when it ceases.
Dr. Faraday was led to suppose, from the manifest analogy
existing between the properties of ?nagnets and those of electro-
dynamic coils or cylinders, that the same results would be obtained