Experimental Researches in Electricity, Volume 1Faraday, Michael
Science
Experimental Researches in Electricity, Volume 1
Faraday, Michael
Electricity; Electricity -- Early works to 1850
175. The moveable part of the wire was then arranged _below_ the
galvanometer, but so as to be carried across the dip. It affected the
instrument as before, and in the same direction; i.e. when carried from
west to east under the instrument, the marked end of the needle went west,
as before. This should, of course, be the case; for when the wire is
cutting the magnetic dip in a certain direction, an electric current also
in a certain direction should be induced in it.
176. If in fig. 31 _dp_ be parallel to the dip, and BA be considered as the
upper part of the rectangle (171.), with an arrow _c_ attached to it, both
these being retained in a plane perpendicular to the dip,--then, however BA
with its attached arrow is moved upon _dp_ as an axis, if it afterwards
proceed in the direction of the arrow, a current of electricity will move
along it from B towards A.
177. When the moving part of the wire was carried up or down parallel to
the dip, no effect was produced on the galvanometer. When the direction of
motion was a little inclined to the dip, electricity manifested itself; and
was at a maximum when the motion was perpendicular to the magnetic
direction.
178. When the wire was bent into other forms and moved, equally strong
effects were obtained, especially when instead of a rectangle a double
catenarian curve was formed of it on one side of the galvanometer, and the
two single curves or halves were swung in opposite directions at the same
time; their action then combined to affect the galvanometer: but all the
results were reducible to those above described.
179. The longer the extent of the moving wire, and the greater the space
through which it moves, the greater is the effect upon the galvanometer.
180. The facility with which electric currents are produced in metals when
moving under the influence of magnets, suggests that henceforth precautions
should always be taken, in experiments upon metals and magnets, to guard
against such effects. Considering the universality of the magnetic
influence of the earth, it is a consequence which appears very
extraordinary to the mind, that scarcely any piece of metal can be moved in
contact with others, either at rest, or in motion with different velocities
or in varying directions, without an electric current existing within them.
It is probable that amongst arrangements of steam-engines and metal
machinery, some curious accidental magneto-electric combinations may be
found, producing effects which have never been observed, or, if noticed,
have never as yet been understood.
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