Magnetism in Solids

ferromagnetism

/ FER-oh-mag-net-iz-um /

This is the magnetism you grew up with: the fridge magnet, the compass needle, the horseshoe magnet in a toy box. Unlike the timid responses of most matter, a ferromagnet pulls hard, and — this is the magic — it keeps its magnetism even after you take the original magnet away. It remembers.

The secret is that the atomic moments in iron, cobalt, and nickel do not wait for an outside field to line up. A quantum push between neighbors, the exchange interaction, makes each atom want to point the same way as the atoms beside it. Below a certain temperature this agreement spreads through the whole crystal, and vast numbers of moments lock into a single direction all on their own — spontaneous alignment, no external field required.

Ferromagnetism matters because that self-sustaining order is what makes practical magnets, electric motors, transformers, and hard-disk storage possible. One honest subtlety: a fresh piece of iron usually shows no external magnetism at all, because it splits into many regions called domains that point different ways and cancel. You magnetize it by coaxing those domains to agree — which is why a 'non-magnetic' nail can suddenly become a magnet after you stroke it with one.

Stroke a steel needle a few dozen times in one direction with a bar magnet, then float it on a cork in water. It swings to point north — you have turned the needle's domains into agreement and made a working compass.

Stroking aligns a steel needle's domains, leaving it permanently magnetized.

Iron is the famous ferromagnet, yet most iron compounds — rust, for instance — are not ferromagnetic at all. What matters is not the element alone but how the atoms are arranged and spaced, which sets whether the exchange interaction pushes neighbors to agree or to oppose.

Also called
铁磁性