Experimental Researches in Electricity, Volume 1Faraday, Michael
Science
Experimental Researches in Electricity, Volume 1
Faraday, Michael
Electricity; Electricity -- Early works to 1850
234. But if the current of electricity were made to cease for a while, and
magnetic poles were used instead to give direction to the needles, and make
them take the same position as when under the influence of the current,
then they must be arranged as at fig. 41; the marked and unmarked poles
_ab_ above the wire, being in opposite directions to those _a'b'_ below. In
such a position therefore the magnetic curves between the poles _ab_ and
_a'b'_ have the same general direction with the corresponding parts of the
ring magnetic curve surrounding the wire NP carrying an electric current.
235. If the second wire _pn_ (fig. 40.) be now brought towards the
principal wire, carrying a current, it will cut an infinity of magnetic
curves, similar in direction to that figured, and consequently similar in
direction to those between the poles _ab_ of the magnets (fig. 41.), and it
will intersect these current curves in the same manner as it would the
magnet curves, if it passed from above between the poles downwards. Now,
such an intersection would, with the magnets, induce an electric current in
the wire from _p_ to _n_ (114.); and therefore as the curves are alike in
arrangement, the same effect ought to result from the intersection of the
magnetic curves dependent on the current in the wire NP; and such is the
case, for on approximation the induced current is in the opposite direction
to the principal current (19.).
236. If the wire _p'n'_ be carried up from below, it will pass in the
opposite direction between the magnetic poles; but then also the magnetic
poles themselves are reversed (fig. 41.), and the induced current is
therefore (114.) still in the same direction as before. It is also, for
equally sufficient and evident reasons, in the same direction, if produced
by the influence of the curves dependent upon the wire.
237. When the second wire is retained at rest in the vicinity the principal
wire, no current is induced through it, for it is intersecting no magnetic
curves. When it is removed from the principal wire, it intersects the
curves in the opposite direction to what it did before (235.); and a
current in the opposite direction is induced, which therefore corresponds
with the direction of the principal current (19.). The same effect would
take place if by inverting the direction of motion of the wire in passing
between either set of poles (fig. 41.), it were made to intersect the
curves there existing in the opposite direction to what it did before.
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