Kaluza-Klein theory is a unification of electromagnetism and General Relativity. It treats both electromagnetism and gravity as being due to geometry.
http://en.wikipedia.org/wiki/Kaluza-Klein_theory
has more details. I'm afraid I don't know that much more about it than what's in the Wikipedia.
As the wikipedia mentions, KK theory has some difficulties, especially if you try to extend it to cover more forces than just gravity and electromagnetism.
You can certainly ask about magnetism and general relativity in this forum, but you should expect an answer from the standpoint of general relativity if you ask the question in the relativity forum.
You might try asking your question again in the "Strings Branes and LQG" forum if you want an M-theory perspective. M-theory is the latest incarnation of string theory.
http://en.wikipedia.org/wiki/M-theory
It is a "theory of everything" that tries to unify all forces in one theory.
If you have your own personal theories, you should be aware of the PF guidelines about overly speculative posts from the Theory Development forum.
Overly Speculative Posts:
Physicsforums.com strives to maintain high standards of academic integrity. There are many open questions in physics, and we welcome discussion on those subjects provided the discussion remains intellectually sound. Posts or threads of an overly speculative nature will be moved to the Theory Development subforum without notice, where discussion may continue in quarantine. Forum staff may choose to lock threads in the Theory Development subform when they decide the topic has run its course. Advertisements of personal theories and unfounded challenges of mainstream science will not be tolerated anywhere on the site, including the Theory Development subforum. Users may not create threads in the Theory Development subforum.
Basically random speculative theories not based any sort of peer-reviewed scientific thought tend to get moved to the Theory Development forum by the moderators.
As far as test masses in GR go, large masses disturb the fabric of space-time. A small non-spinning test mass will follow a geodesic of the hypothetical space-time that would exist without the test mass being present. This statement can be made more rigorous, for instance MTW discuses it more on pg 1126, "Do the planets and suns really move on geodesics".
In the geometric theory of gravity, gravity is not treated as a force. The density of energy and momentum, given by the stress-energy-tensor, determines the curvature of space-time by the relation
G_uv = 8 Pi T_uv
where the left-hand side is a measure of how space curves, and the right side is the stress-energy tensor that describes how mass, energy, and momentum are distributed.
Treating gravity as a force is a hard habit to break, though. Fortunately, there are a few "bridges" between the geometric formulation of gravity, and the treatment of gravity as a force.
One good bridge is Cartan's reformulation of Newtonian gravity in the formalism of curved-space time. (The geodesic equation and the geodesic deviation equation are other useful "bridges" between gravity-as-a-force and gravity-as-geometry).
As you recall, small non-spinning test masses in GR move along geodesics. It is possible to use the formalism of curved space-time to describe a curved space-time that makes object move exactly as if they were subjected to a force of F = GmM/r^2. We have replaced the idea of forces totally, with the idea of objects following geodesics in a curved space-time. The physical behavior of the bodies remains the same.
This exercise does not introduce anything new, but it helps one to understand GR better. Strong gravity fields in GR actually warp space as well as space-time. (Example: just as clocks tick more slowly near a large mass, the meter is shorter. This gravitational length contraction is an illustration of how the geometry of space near a large mass cannot be flat). The warpage of space is very minor for "weak" fields such as the fields we have in our solar system, but it is important in explaining, for instance, the GR prediction that light from a distant star is bent twice the amount by the suns gravity that Newtonian theory would predict.
The formulation of gravity as curved-space time can naturally incorporate this warping of space into the theory, something that is not possible with the idea of "gravity-as-a-force".