In addition to moving charges, another source of magnetic fields that we are going to talk about are permanent magnets. These are the magnets that probably you have seen, have experience with, and already know about (i.e. refrigerator magnets, the Earth, the traditional U-shaped magnets, etc.). While these are much more frequently used in everyday life, permanent magnets are actually quite complicated and are an area of current research. These notes will show how we simplify and model permanent magnets, their magnetic field vectors and how we can actually measure magnetic fields.

Motion of nucleus and electrons in an atom

In the last two pages of notes, we developed a fairly thorough understanding of how moving charges create magnetic fields. We will leverage this along with what we know about atoms to create a model of how materials can be turned into magnets.

In an atom, we know that there is a large, positive nucleus surrounded by the smaller, negative electrons, which are constantly moving around the nucleus. Since each electron has a charge, it produces a magnetic field as it moves around the nucleus (if we model the electron path as a counter-clockwise circle then using the right hand rule, the magnetic field would point up). In addition to the electrons moving around the nucleus, the electron itself is spinning on its axis (much like how the Earth is spinning on its axis while traveling around the sun), which also creates a magnetic field. Finally, the protons within the nucleus can also spin on their axes, which also would create a magnetic field.

This means that within an atom there are at least 3 (more if there are more electrons/protons) sources of magnetic field simply from the way that the charged particles are moving. For each atom then, we can say that there is a net magnetic field that would point in a certain direction (typically represented by a small B-field arrow).

Net magnetic field on an atom

Randomized magnetic fields sum to a net magnetic field of zero

If every atom has a magnetic field from its moving charges, why is everything not a magnet? For a non-magnetic material (like plastic, wood, glass, etc.) the direction of the magnetic field for every atom is randomized (shown in the figure to the right). When you take the add up the magnetic field vectors from all the atoms in the material, you get a net magnetic field of zero.

Magnetic fields from atoms point in the same direction in permanent magnets

In contrast to non-magnetic materials, permanent magnets (also called ferromagnets) are materials where the magnetic fields from all the atoms point in (roughly) the same direction (seen in the figure above). This is usually accomplished by putting the material in a very strong magnetic field (typically from a large current rather than another ferromagnet). It is possible for the field from each of the atoms to start to randomize (or un-align themselves) but this generally takes a very long time for a permanent magnet. (There are also other kinds of magnetic materials besides ferromagnets, such as diamagnets, paramagnets, and antiferromagnets - but we won't talk about those in this class.)

Magnetic field vectors in induced magnets with time

There are also some materials that will become “temporary magnets” if exposed to a magnetic field. In this case the material starts out with randomized magnetic fields from its atoms. When this material is placed near a strong external magnetic field the fields from all the atoms start to align with that external field. When the external magnetic field is taken away, the magnetic fields from the atoms remain aligned for some time before returning to their randomized directions. You may have seen this when you place a nail near a strong magnet. The nail will become a magnet for a time and be able to pick up other nails; however it does not remain a magnet indefinitely.

For a demonstration of how you can create a temporary magnet, you can check out this youtube video.

Magnetic field modeled by iron filings around a bar magnet

One kind of magnet that we will refer to often is a bar magnet, which usually refers to a straight rectangular ferromagnet with a constant, strong magnetic field (whereas a permanent magnet can generally have more varied shapes - like a disk, u-shape, coil, etc.). Since a bar magnetic is generally a ferromagnet, this means that all the little magnetic fields from the atoms are aligned and point in the same direction, resulting in a larger, net magnetic field outside the material. If you happen to drop some iron filings around a bar magnet, the filings will align themselves with the net magnetic field of the bar magnet (shown to the sid