Appletons' Popular Science Monthly, January 1900: Vol. 56, November, 1899 to April, 1900 — John Shaqi
Appletons' Popular Science Monthly, January 1900: Vol. 56, November, 1899 to April, 1900Various
Science
Appletons' Popular Science Monthly, January 1900: Vol. 56, November, 1899 to April, 1900
Various
Science -- Periodicals; Technology -- Periodicals
Electricity and magnetism are two forces that are intimately associated
with each other, and, although radically different, it is difficult,
if not impossible, to obtain one without the other, although it is a
simple matter to make one inactive under certain conditions. It is very
generally understood that a magnet possesses the power of attraction,
and that it will draw toward it pieces of iron, steel, and other
magnets. The laws governing the attractive properties of magnets,
however, are not so well understood, and many are not aware of the fact
that under certain conditions one magnet will repel another, but such
is nevertheless the case.
[Illustration: FIGS. 1, 2, 3.--DIAGRAMS ILLUSTRATING THE ATTRACTION AND
REPULSION OF MAGNETS.]
In Fig. 1 the lower outline, _M_, represents a magnet fixed in
position, and the upper bar represents another magnet arranged to
swing freely around the pivot _a_. A magnet, as is generally known,
will arrange itself in a north-to-south position if suspended from its
center, like a scale beam, and allowed to swing freely, and the same
end will always point toward the north. On this account the ends of a
magnet are called its poles, and the one that will point toward the
north is designated the north pole, while the other one is the south
pole. The terms north and south poles were applied to magnets centuries
ago, but at the present time the ends are more commonly designated as
positive and negative. In Fig. 1 it will be noticed that the stationary
magnet has its positive end upward, and this attracts the negative end
of the swinging magnet. If the order of the poles is reversed, so that
the positive of the swinging magnet will come opposite the positive of
the stationary one, then there will be a repulsive action instead of an
attraction, as is shown in Fig. 2. If the two negative ends were placed
opposite, the effect would be the same. From this we see that to obtain
an attraction we must place the magnets so that opposite poles come
together, and that by reversing the order we obtain a repulsive action.
If the swinging magnet is replaced by a bar of iron, as is shown in
Fig. 3, there will be an attraction, no matter what end of the magnet
may be uppermost, thus showing that either end of a magnet will attract
a bar of iron. The explanation of these different actions is that when
two magnets are brought into proximity to each other each one exerts
its force without any regard to the other, and if the two are set
to act together they will attract one another, but if set to act in
opposition they will repel. When one of the bars is not a magnet, but
simply a piece of iron or steel, this bar, having no attractive or
repulsive force of its own, can only obey the attractive action of the
other, which is the only one that exerts a force.
[Illustration: FIGS 4, 5.--DIAGRAMS ILLUSTRATING THE METHOD OF
OBTAINING ROTARY MOTION WITH MAGNETS.]
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