Welcome to PF;
It looks like you have a lot of study to do. A rigorous treatment would be beyond the scope of these forums but we may be able to give you an idea to go on with.
JamesClarke said:
I`m not a physics expert and have loads of questions about electro magnetism, both classical and quantum.
Well I don't think anybody is an "expert" in quantum mechanics ... but some people do do it for a living.
Looking through your questions, it looks like you are having trouble keeping the different models straight. You should realize that you are talking about different ways of describing reality here.
What is a field made of? in classical it is essentially nothing but how does the force from the charge propagate through empty space. In quantum it says that its a cloud of virtual photons but how do these photons "know" how to stay within the boundary of the field.
The classical EM field is a consequence of Maxwel's equations.
It is a kind of metaphore we use to relate the motions of charges in one part of space with those of another.
There are philosophical problems with this - you have mentioned the main one: "how does the force get from one place to another?" ... this is the "action at a distance" problem. Classical theory does not answer this problem - "them's just the rules". (You should ask yourself why action at a distance is such a problem anyway: how is it that you come to expect interactions to be local and how close together do two things have to get before you are happy with their interactions? Perhaps all interactions are "at a distance" anyway - just that some of the distances are too small to see?)
Field theory attempts to get around this by having a particle
mediate the interaction. There is no mystery about how material objects get from A to B after all, or that they can make things happen when they get there.
In the Field Theory, the EM-field metaphore is no longer needed. We refer to an EM-
interaction mediated by photons, and described by Feynman diagrams, instead. Field Theory
supplants classical electromagnetism.
The Field of Field Theory is not "made up of" photons, and it is not the same as the EM-Field. The Field of FT is statistical in nature ... and that makes it hard to think about.
When a charged object enters a field how does the object that mediates the field know that an object is there that it can react with?
It doesn't. All a charge knows is that it has encountered a photon.
Classical offers no explanation(i think)
That would be broadly correct - the classical model allows for action to happen at a distance ... it seems that charged objects can recognize each other over large distances and react accordingly.
At this level it is unusual to use forces at all - we'd normally refer to energies and potentials. A charge will follow the local gradient of the EM-potential "downhill". This way a charge need know as much about EM physics as the ball on a slope needs to know about gravity.
quantum says the photons are fired at each other.
No it doesn't - that would imply there is someone doing the aiming. A better picture would be for photons to be fired off at random in all directions from something like an electron.
How do the photons from around the field know that a charged particle has entered it
They don't know anything about the charge until it gets close.
if no information has been conveyed to them?
Depends what you mean by "information".
how does the example of throwing a ball between 2 boats explain attraction?
Try it and see. Though that would be for
repulsion iirc. Texts using the thrown vs swapped balls analogy (and that is all it is) are usually pretty good at describing this. Hint: Law of conservation of momentum.
How are the virtual photons generated?
They just are - those are the rules.
You may want to look up "self energy of the electron" to get a better idea about what these models are trying to describe. Photons are being released and absorbed all the time in this model.
what about conservation of energy? Where does the energy come from that keeps generating these photons?
energy can come from the object's kinetic energy for example ... releasing a photon slows it down.
but we have to be careful here because Field theory is relativistic ... and an electron that is stationary wrt the observer, releases a photon, it is no longer stationary: photon and electron head off in opposite directions by conservation of momentum: how are we to account for conservation of energy? That what you mean?
There are two major positions here.
1. conservation of energy can be violated provided the time-scale is sufficiently small. If the energy violation is ΔE then it is OK as long as it lasts ##\Delta t \leq \hbar/\Delta E## ... a result that agrees well with the observed ranges for the various interactions.
2. conservations laws are strictly observed - the "virtual" particles are just that -
virtual. They are an artifact of the way the calculations are carried out. (Look up "perturbation theory"). There are lots of situations where we do some intermediate steps in our calculations without the intervening steps having any physical, literal, reality. Long division, for example.
Wikipedia takes position (1),
here's an example of position (2).
Bear in mind that these are only
models, not reality, and that physics, as with all science, is a work in progress: there are no ultimate answers here (The Guide not withstanding.).
I have loads more questions.
I can imagine.
I am conscious that the replies I have given are going to be inadequate - and, in some sense, downright wrong. (I brace myself for people saying what a mess I'm talking.)
None of the answers here are likely to be very satisfying anyway - you should realize that whole books are written on the themes you have introduced. The best anyone can do is point, hopefully, in the direction of more understanding. The amount of mileage you get out of all this depends entirely on your willingness to learn.
Have fun.