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Experimental Researches in Electricity, Volume 1 by Michael Faraday
page 14 of 785 (01%)
everywhere touch, except that a sheet of thick paper was interposed. One of
these wires was connected with the galvanometer, and the other with a
voltaic battery. The first wire was then moved towards the second, and as
it approached, the needle was deflected. Being then removed, the needle was
deflected in the opposite direction. By first making the wires approach and
then recede, simultaneously with the vibrations of the needle, the latter
soon became very extensive; but when the wires ceased to move from or
towards each other, the galvanometer-needle soon came to its usual
position.

19. As the wires approximated, the induced current was in the _contrary_
direction to the inducing current. As the wires receded, the induced
current was in the _same_ direction as the inducing current. When the wires
remained stationary, there was no induced current (54.).

20. When a small voltaic arrangement was introduced into the circuit
between the galvanometer (10.) and its helix or wire, so as to cause a
permanent deflection of 30° or 40°, and then the battery of one hundred
pairs of plates connected with the inducing wire, there was an
instantaneous action as before (11.); but the galvanometer-needle
immediately resumed and retained its place unaltered, notwithstanding the
continued contact of the inducing wire with the trough: such was the case
in whichever way the contacts were made (33.).

21. Hence it would appear that collateral currents, either in the same or
in opposite directions, exert no permanent inducing power on each other,
affecting their quantity or tension.

22. I could obtain no evidence by the tongue, by spark, or by heating fine
wire or charcoal, of the electricity passing through the wire under
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