Permanent magnets
Centuries ago, it was discovered that
certain types of mineral rock possessed unusual properties
of attraction to the metal iron. One particular mineral,
called lodestone, or magnetite, is found
mentioned in very old historical records (about 2500 years
ago in Europe, and much earlier in the Far East) as a
subject of curiosity. Later, it was employed in the aid of
navigation, as it was found that a piece of this unusual
rock would tend to orient itself in a north-south direction
if left free to rotate (suspended on a string or on a float
in water). A scientific study undertaken in 1269 by Peter
Peregrinus revealed that steel could be similarly "charged"
with this unusual property after being rubbed against one of
the "poles" of a piece of lodestone.
Unlike electric charges (such as those
observed when amber is rubbed against cloth), magnetic
objects possessed two poles of opposite effect, denoted
"north" and "south" after their self-orientation to the
earth. As Peregrinus found, it was impossible to isolate one
of these poles by itself by cutting a piece of lodestone in
half: each resulting piece possessed its own pair of poles:
Like electric charges, there were only two
types of poles to be found: north and south (by analogy,
positive and negative). Just as with electric charges, same
poles repel one another, while opposite poles attract. This
force, like that caused by static electricity, extended
itself invisibly over space, and could even pass through
objects such as paper and wood with little effect upon
strength.
The philosopher-scientist Rene Descartes
noted that this invisible "field" could be mapped by placing
a magnet underneath a flat piece of cloth or wood and
sprinkling iron filings on top. The filings will align
themselves with the magnetic field, "mapping" its shape. The
result shows how the field continues unbroken from one pole
of a magnet to the other:
As with any kind of field (electric,
magnetic, gravitational), the total quantity, or effect, of
the field is referred to as a flux, while the "push"
causing the flux to form in space is called a force.
Michael Faraday coined the term "tube" to refer to a string
of magnetic flux in space (the term "line" is more commonly
used now). Indeed, the measurement of magnetic field flux is
often defined in terms of the number of flux lines, although
it is doubtful that such fields exist in individual,
discrete lines of constant value.
Modern theories of magnetism maintain that a
magnetic field is produced by an electric charge in motion,
and thus it is theorized that the magnetic field of a
so-called "permanent" magnets such as lodestone is the
result of electrons within the atoms of iron spinning
uniformly in the same direction. Whether or not the
electrons in a material's atoms are subject to this kind of
uniform spinning is dictated by the atomic structure of the
material (not unlike how electrical conductivity is dictated
by the electron binding in a material's atoms). Thus, only
certain types of substances react with magnetic fields, and
even fewer have the ability to permanently sustain a
magnetic field.
Iron is one of those types of substances
that readily magnetizes. If a piece of iron is brought near
a permanent magnet, the electrons within the atoms in the
iron orient their spins to match the magnetic field force
produced by the permanent magnet, and the iron becomes
"magnetized." The iron will magnetize in such a way as to
incorporate the magnetic flux lines into its shape, which
attracts it toward the permanent magnet, no matter which
pole of the permanent magnet is offered to the iron:
The previously unmagnetized iron becomes
magnetized as it is brought closer to the permanent magnet.
No matter what pole of the permanent magnet is extended
toward the iron, the iron will magnetize in such a way as to
be attracted toward the magnet:
Referencing the natural magnetic properties
of iron (Latin = "ferrum"), a ferromagnetic material
is one that readily magnetizes (its constituent atoms easily
orient their electron spins to conform to an external
magnetic field force). All materials are magnetic to some
degree, and those that are not considered ferromagnetic
(easily magnetized) are classified as either paramagnetic
(slightly magnetic) or diamagnetic (tend to exclude
magnetic fields). Of the two, diamagnetic materials are the
strangest. In the presence of an external magnetic field,
they actually become slightly magnetized in the opposite
direction, so as to repel the external field!
If a ferromagnetic material tends to retain
its magnetization after an external field is removed, it is
said to have good retentivity. This, of course, is a
necessary quality for a permanent magnet.
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REVIEW:
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Lodestone (also called Magnetite)
is a naturally-occurring "permanent" magnet mineral. By
"permanent," it is meant that the material maintains a
magnetic field with no external help. The characteristic
of any magnetic material to do so is called retentivity.
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Ferromagnetic materials are easily
magnetized.
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Paramagnetic materials are
magnetized with more difficulty.
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Diamagnetic materials actually tend
to repel external magnetic fields by magnetizing in the
opposite direction.
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