- #36
PeterDonis
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Quantum Immortal said:The GEM that is meant here, is the ones that look the same with attractive EM. Period!
Not if the equations say differently. See below.
Quantum Immortal said:He defines E=-a
Doesn't matter; his equation for ##\vec{\nabla} \cdot \vec{E}_g## is what makes positive masses repel other positive masses. See below.
Quantum Immortal said:I think the 4 is at the wrong place in the wiki.
I think it doesn't belong there at all, since, as I noted, the paper Jonathan Scott linked to, which actually goes through the derivation of GEM equations in the weak field, linear approximation from the EFE, does not have the 4. (Neither does the paper you linked to, but it has other problems; see below.)
Quantum Immortal said:The paper has no 4. Its just straight out attractive EM-like...
Not having the factor of 4 doesn't make gravity attractive in that model. The sign in its equation for ##\vec{\nabla} \cdot \vec{E}_g## is the opposite of that in the paper Jonathan Scott linked to. That makes a *big* difference; see below.
Quantum Immortal said:Why some people here are ready to believe, that the author and springer were so incompetent, as to use a repulsive model of gravity
Well, that's what the equations in the paper you linked to say; see below. As for why the paper passed review, lots of papers pass review that are later found to have errors in them. Since the author of the paper does not explicitly compute whether or not gravity is attractive in his model (he just assumes it), and since his main point was to compute perihelion precession, it may simply be that none of the reviewers thought to check; they assumed that he was correct about gravity being attractive, and just checked his computations of the precession.
Quantum Immortal said:with half the speed of light as propagation speed?
I believe Bill_K was referring to the Wiki page, not the paper you linked to. The factor of 4 in the ##\vec{\nabla} \times \vec{B}_g## equation on the Wiki page is what makes gravitational waves propagate at half the speed of light. As noted above, neither the paper you linked to nor the paper Jonathan Scott linked to have that factor of 4, so it looks to me like gravity waves in both of those papers would propagate at the speed of light, as expected.
Quantum Immortal said:And if the wiki article says something supportive, we are extremely critical, "don't trust the wiki".
"Don't trust the wiki" is, as I noted to Jonathan Scott, *always* good advice.
Quantum Immortal said:But if it says something negative, we take it at face value...
I don't think anyone in this thread has taken anything the Wiki page says at face value; I know that I've repeatedly said I want to see other derivations before accepting the equations it gives as correct (and now, of course, other derivations have shown its equations to be wrong in having the factor of 4 in the last one). So I don't know what you're complaining about here.
Quantum Immortal said:The GEM that is meant here, is the ones that look the same with attractive EM. Period!
You might have "meant" that, and so might the author of the paper you linked to, but you don't get to just declare it by fiat. You have to actually look at the math.
Look at the paper Jonathan Scott linked to; the sign difference in the equations that I described above is obvious. Now look at Maxwell's Equations, which are known to predict like charges repelling, not attracting. Which paper matches the sign in Maxwell's Equations?
Quantum Immortal said:These calculations, could have been made over 100 years ago. If I'm correct, back at a time that only the orbit of mercury was an observable problem. So, if the paper is correct, it would mean that GEM would have been a complete theory back then, before GR, before modern SR even. What is done in GEM is so simple, that its impossible that no one thought about it. So, what's going on?
I can't say why the Heaviside paper wasn't picked up on, but one hypothesis is that the pathway he was suggesting to modifying Newton's Laws just wasn't one that enough physicists were ready to follow. The pathway that Einstein used--first show that the kinematics of Newton's theory have to be modified, with SR, before tackling the dynamics, with GR--was apparently one that worked better.