misogynisticfeminist said:
I understand that no conclusive theory on magnetism has been formulated yet. But i was wondering if it did answer this question.
If the electrons orbiting the nucleus give a magnetic material its magnetic properties. Then why of all atoms would Iron or nickel be the few which possesses magnetic properties?
There are several issues and miconceptions here, and this question should have been posted in the condensed matter section.
First of all, let's make sure we are clear that the theory of magnetic FIELDS are well-known and certainly VERY conclusive. I know you did not ask about fields, but I want to make sure those who are reading this do not get confused between the concept of magnetic fields and "magnetism", which is the magnetic properties of MATTER.
Secondly, "magnetic properties" is highly ambiguous. There are several "magnetic properties" of matter: paramagnetism, diamagnetism, ferromagnetism, antiferromagnetism, etc. What you are asking by bringing out the example of iron and nickle is ferromagnetism.
Thirdly, we know the origin on why things have all these 'ism. It is due to the presence or absence of a "magnetic moment" of the valence shell.
Fourthly, the issue isn't that such magnetic moment exist, but rather, why are there LONG-RANGE ordering of these moments over a substantial size of the material. Ferromagnetism requires a net and FIXED allignment of a gazillion of these magnetic moments even without an external magnetic field, whereas paramagnetism only causes such long range ordering only in the presence of an external magnetic field.
Fifth, to answer the fourth point, you have to know many-body theory. Whenever there are any long range ordering involving a gazillion particles, it automatically means that there are a gazillion interactions that somehow produces a lowering of an energy for a favorable state, at a particular temperature. This isn't easy. In many instances, we only learn what kinds of parameters to use only after we know how the system behave, and then learn from that system when we apply it to a similar system. So in most of these, it is still very much a phenomenology.
Sixth, look up an example of the Ising model. It will tell you why, even in a simple 2D array of spins, that by simply changing slightly the nature and range of coupling of each spin, you can end up with an entirely different magnetic ordering for the system.
This is why, if I give you a bunch of magnetic spins, and ask you to tell me what is the ground state magnetic system you will end up with, you will not be able to answer my question - no one can, at least not for the most generalized situation. The theory of magnetism is known to the extent that we know what we still do not know yet.
Zz.