vincentchan said:
here is one of the newest research done by last year...
http://arxiv.org/PS_cache/gr-qc/pdf/9303/9303025.pdf
go to page 15 and read the conclusion...
edit: the 10th line..."in the accelerated frame..." don't want to quote every thing, read...
You didn't explain how what I said contradicted the articles I quoted/referanced.
I've already read the article the you referred to. The author contradcits a lot of physics in that article. For example; the author assumes, using his own intuition or whatever, that some forms of the equivlance principle don't apply. Since the equivalence principle is a postulate then only experimentation can determine whether it is correct or not - not calculation.
The author asserts
Since the particle is radiating energy which can be detected and used, conservation of energy suggests that the radiated energy must be furnished by the rocket — we must burn more fuel to produce a given accelerating worldline than we would to produce the same worldline for a neutral particle of the same mass.
This contradicts previous conclusions. For example; An extra force must be used to accelerate a charged particle over a non-charged particle. This extra force is known in the literature as the "self-force" acting on the particle. This also is known as the "radiation reaction force."
Details - The power radiated by an accelerating charge is given (in esu units) by P = (2/3)q
2/c[sup3[/sup](
a)
2. To account for this energy loss modify Newton's equation by adding in an extra force
Frad. Suppose the force on a non-charged particle of the same (rest) mass is (in the non-relativistic limit)
Fext = m
a. A particle with charge q and mass m is then given by
Fext +
Frad = m
a. By demanding that energy be conserved this demands
Frad = mTd
a /dt (where T is a constant and I'm too lazy to type it in

). If the particle is uniformly accelerated then the radiative force is zero. Thus if you have a particle in a uniformly accelerating frame of reference and you're also at rest in that frame then the weight of the particle is independant of the charge. Hence the authors assertions are in contradiction with the assertions I've just stated.
Its also be shown that the weight of a particle depends on the spacetime curvature. That means that a charged particle at rest on, say, the Earth will have a different weight (i.e. smaller required support force) than the same particle at rest in a uniform g-field.
The paper is newer. That doesn't mean that its better.
Pete