In many materials, the spin of each electron cancels out that of another electron in the
same atom with which it is “paired,” resulting in no net magnetic field. Ferromagnetism
results from the net magnetic field created by unpaired electron spins. For example,
each iron atom contains four electrons with uncancelled spins, giving the iron atom a
net dipole moment.
In ferromagnetic materials, the spins of the electrons of one atom interact with the spins
of electrons of neighboring atoms. This interaction, called exchange coupling, is
quantum mechanical in nature. As a result of exchange coupling, the magnetic dipoles
of atoms within a ferromagnetic material tend to align in the same direction.
When the magnetic dipole moments of ferromagnetic atoms align, the result is a
magnetic domain, a region in a material where there is a net magnetic field. Magnetic
domains can be seen under powerful microscopes, often with the aid of a technique
called magnetic force microscopy. In the color micrograph above, domains are given
false colors to be more easily seen in the image. Typical domains have a diameter
about one-third that of a human hair. This can be best seen in the small inset
micrograph that shows the magnetic domains in a sample of carbon steel. Even small
amounts of magnetic materials contain vast numbers of domains. A domain may
contain 10^12 to 10^15 atoms, but since a cubic centimeter of iron contains about 2.5×10^19
atoms, there are still a large number of domains.
There is a good question here: Why are not all iron objects magnets? The reason is that
although domains have magnetic fields, they point in random directions unless they
have been subjected to an external magnetic field. This is shown in Concept 2. The
random nature of their directions means there is no net magnetic field in the substance.
However, when the ferromagnetic material is placed in an external magnetic field, a
process occurs that results in the material gaining its own overall magnetic field. This
happens because the external field exerts a torque on the magnetic dipoles.
The magnetic field overcomes the tendency of the dipoles to stay aligned with their
neighbors, and causes them to align with the field. Unaligned dipoles bordering
domains that are aligned with the field steadily become “converted” to the new
orientation. This causes the domains aligned with the external field to expand. This is
shown in Concept 3, where the domains shown in Concept 2 have combined to form
three domains.
Since there is a tendency for the dipoles to remain aligned, when the external magnetic
field is removed, the domains (and the dipoles that make them up) remain aligned. This
means the material now has its own magnetic field. In short, a magnet has been
created.
An external magnetic field can cause non-ferromagnetic materials to develop their own
magnetic field. These other forms of magnetism are called diamagnetism and
paramagnetism. However, ferromagnets are distinct and quite useful for two reasons.
First, a ferromagnet retains its magnetic field after the external field is removed. A
refrigerator magnet, or the information stored on a VCR tape, both rely on the longevity
of ferromagnets. The other forms of magnetism disappear after the external magnetic
field is removed.
Second, the magnetic field created by ferromagnetic materials is typically orders of
magnitude stronger than that found in the other forms of magnetism in most materials.
This makes ferromagnets useful for a wide range of everyday applications.
Random domains
Unaligned domains mean no net
magnetic field
In external magnetic field
In external magnetic field, B 0
·domains aligned to external field grow
Magnetic field removed
Substance maintains magnetic field
28.7 - Magnetic fields and charged particles
Magnetic fields exert forces on moving, electrically
charged particles.
This phenomenon makes for a good demonstration in
a physics class. A current-carrying wire is placed near
a magnet. The magnet exerts a force on the electrons
moving in the wire, which causes the wire to move
toward or away from the magnet. When the current is
turned off, the magnetic field stops exerting a force on
the wire.
The images on the screens of traditional televisions
and computers are the result of electrons being
accelerated by an electric field, subsequently being
“steered” by magnetic fields, and then striking the
screen to create light of different colors at specific
locations. If you were to place a magnet close to such a system, you would distort the image. However, we do not recommend you do this, as it
could cause expensive or irreversible damage!
TV tube. A gun (far left) accelerates electrons across a potential difference.
Electromagnets (brown) steer the moving charges to light up screen pixels.
(^510) Copyright 2000-2007 Kinetic Books Co. Chapter 28