ngkamsengpeter:
When you have an individual electron, it behaves like a bar magnet (it has an intrinsic magnetic dipole moment). Usually electrons prefer* to pair up with another electron with the magnet pointing the other way - so the pair of electrons together has no magnetic dipole, they effectively neutralize each other (*this is because of the quantum mechanical principle of Pauli exclusion). In many atoms you have only such pairs of electrons, so the whole atom has no magnetic dipole. But for example, if there are an odd number of electrons* (example Alumnium, 13 electrons), there is at least one 'unpaired' electron, at the whole atom will have the magnetic dipole of this one electron; the whole atom will act as a bar magnet and respond to external magnetic fields. This is an example of
paramagnetism.
*this is not necessary but common
This is a very weak effect - aluminum
is attracted to magnets, but only slightly. When you deal with everyday magnetic materials, such as iron, a far stronger effect is involved.
Instead of
one atom acting individually as a little bar magnet, occasionally you have
millions of atoms deciding to align with each other and reinforce each others' magnet dipoles - a magnetic
domain. These are basically much bigger bar magnets, and are responsible for the strong magnetizibility of
ferromagnets like iron. This can happen (the magnetic domains) if certain criteria regarding the solid's structure and bond lengths are satisified.