MichaelW24 said:
Ok, this extra inertial mass should be (gamma - 1)m I think... do you know if this contributes to gravity? Its quite confusing as I was given a hint that the m in F=ma isn't nessecarily the same as the m in, for example, W = mg describing a body's weight.
There area some technicalities that make computing the gravitational field of a moving object difficult, in fact I have a long-standing argument with another poster here on the topic. (Of course I think I'm right :-) - and the other poster might argue that it's easy, but in spite of his arguments I think he's still wrong :-)).
Without going into too much detail, though, like arguing, for instance "what the heck is a gravitational field in GR anyway?", you can think of the gravitational field of a moving mass as being definitely non-uniform. If the particle is moving to the left and right across the page, the field in the direction of motion will be "weak"
(weak field)----->(weak field)
Given the same direction of motion, the field transverse to the direction will be "strong"
(strong field)
----->
(strong field)
(I've drawn two separate diagrams due to the vagaries of ascii art on the system.)
This is reasonably close to the truth by anybodys definition of "gravitational field" that matches the Newtonian definition in the Newtonian limit, and it matches the behavior of the electric field (which exhibits similar but not numerically identical behavior), and should convey the essentials without getting into a great deal of highly technical arguments.
You may recall that there is an intergal of the electric field which gives a conserved charge for the electrostatic case. In the gravitational case, there is an intergal of a pseudo-tensor (which is not actually thought of as a field as far as I know) that gives the "gravitational mass" of a moving particle in an asymptotically flat space-time. This pseudo-tensor does indeed give an ADM mass (as it is called) of gamma*m, where m is the rest mass.
I believe the Bondi mass will also be gamma*m, but I haven't gone through the calculation. (The textbook treatment I have for the Bondi mass is too complex to get a result, and I'd have to order the original paper from Bondi from the library to get a simpler coordinate-based treatement).
The Bondi and the ADM mass are two different definitions of mass in GR. (There is a third sort of mass, the Komar mass, that doesn't apply because it requires a static space-time and the metric of a moving mass is not static).
The fact that GR has the need for three different sorts of mass should serve as a warning that the subject is highly technical, and that the above discussion has only "scratched the surface".