There is now an understanding of the electro-magnet, with some idea of
the part it may be made to play in the movement of pieces, parts, and
machines in which it is an essential. It has been explained how soft
iron becomes a magnet, not necessarily by any actual contact with any
other magnet, or by touching or rubbing, but by being placed in an
electric field. It acquired its magnetism by induction; by _drawing
in_ (since that is the meaning of the term) the electricity that was
around it. But induction has a still wider field, and other
characteristics than this alone. Some distinct idea of these may be
obtained by supposing a simple case, in which I shall ask the reader to
follow me.
[Illustration: DIAGRAM THEORY OF INDUCTION]
Let us imagine a wire to be stretched horizontally for a little space,
and its two ends to be attached to the two poles of an ordinary battery
so that a current may pass through it. Another wire is stretched beside
the first, not touching it, and not connected with any source of
electricity. Now, if a current is passed through the first wire a
current will also show in the second wire, passing in an _opposite
direction_ from the first wire's current. But this current in the
second wire does not continue. It is a momentary impulse, existing only
at the moment of the first passing of the current through the wire
attached to the poles of the battery. After this first instantaneous
throb there is nothing more. But now cut off the current in the first
wire, and the second wire will show another impulse, this time in the
_same direction_ with the current in the first wire. Then it is all
over again, and there is nothing more. The first of these wires and
currents, the one attached to the battery poles, is called the
_Primary_. The second unattached wire, with its impulses, is called
the _Secondary_.
Let us now imagine the primary to be attached to the battery-poles
permanently. We will not make or break the circuit, and we can still
produce currents, "impulses," in the secondary. Let us imagine the
primary to be brought nearer to the secondary, and again moved away from
it, the current passing all the time through it. Every time it is moved
nearer, an impulse will be generated in the secondary which will be
opposite in direction to the current in the primary. Every time it is
moved away again, an impulse in the secondary will be in the same
direction as the primary current. So long, as before, as the primary
wire is quiet, there will be no secondary current at all.
There is still a third effect. If the current in the primary be
_increased or diminished_ we shall have impulses in the secondary.
Public-domain text, read in full here on John Shaqi.
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