Scientific American Supplement, No. 711, August 17, 1889 — John Shaqi
Scientific American Supplement, No. 711, August 17, 1889Various
History
Scientific American Supplement, No. 711, August 17, 1889
Various
Science -- Periodicals
I think we may also say, though I do not remember to have seen the
statement so put, that whenever electric potential is set up
inductively, as in self-induction, mutual induction, induction from
one circuit to another, and induction from magnets or magnetic field,
it is set up by the movement of lines of force laterally across the
body, mass or conductor in which the potential is developed, and that
whenever current is set up in a wire or an existing current prolonged,
or an existing current checked by induction, self-induction, or
induction from magnets, the action is a transfer of energy,
represented by strained lines of force shortening or lessening their
resistance, or lengthening and increasing the resistance in their
paths. The magnetic field is like an elastic spring--it can in one
condition represent stored energy--it can be strained and will store
energy--it can be made to relieve its strain and impart energy.
[Illustration: Fig. 1.]
Let us examine some known phenomena in this light. Take the case of a
simple wire, conveying current, say, in a line away from observer,
Fig. 1. There exists a free field of circular magnetism (so called),
shading off away from the wire, and which is represented by concentric
circles of increased diameter. The superior intensity or strength of
the lines near the wire may also be represented by their thickness.
This is often shown also by crowding the lines near the wire, though I
am disposed to regard Fig. 1 as more nearly expressing the condition,
unless we are to regard the lines as simply indicating a sort of
atmosphere of magnetic effect whose density becomes less as we proceed
outward from the wire, in which case either form of symbol suffices.
The direction of polarization of the lines may be indicated by an
arrow head pointing in a direction of right-handed rotation in the
path of the lines. This is the typical figure or expression for all
forms of simple magnetic circuit--the form of the lines, their length,
position, density, will depend on the shape of the conductor or
conductors (when more than one) and the materials surrounding or in
proximity to the wire or wires.
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