The full title is “Gravitation and Cosmology Principles and Applications of the General Theory of Relativity”. In Chapter 10, section 8, on page 289, he writes:
This Introduction to Physics was just posted on YouTube. It’s nice on plain old inertial frames (although the teacher constantly says “if you believe in inertia,” which I understand is pedagogic shorthand, but sounds weird I think). 13:00 on has nice demos and analytical recaps.
He also mentions centripetal force, not centrifugal, as a fictitious force. Depends on whose point of view (inertial reference frame) is what I take away. But everyone talking about phsics always mentions only centrifugal force as essentially fictional, when in fact it depends whose ox is getting gored, right?
Gravity depends on the stress-energy tensor. In a lot of cases the most important component of the stress energy tensor is the energy density. As Chronos will be by shortly to point out, “relativistic mass” is just a synonym for “total energy”. So it’s not too much of lie to say relativistic mass is what gravitates.
Or to be a little more loose: Mass doesn’t gravitate, energy gravitates – it just happens that most objects we think of as gravitating have the vast majority of their energy locked up as mass so we can ignore the non-mass energy without making too much of an error.
Actually, I would consider that “too much of a lie”. That would seem to imply, for instance, that a particle accelerated up to a sufficiently-ludicrous speed would collapse into a black hole due to its total energy, but this doesn’t happen. I would be comfortable with saying that gravity depends on the entire stress-energy tensor, and I would (usually) be comfortable with approximating the entire stress-energy tensor by just the rest mass portion and saying that gravity depends on mass, but neither of those is the same thing as the total energy, and I can’t think of any situation where it would be reasonable to approximate the entire stress-energy by the total energy, or to say that “gravity results from the total energy”.
Just for giggles I poked around on Wolfram Alpha, and unless I seriously screwed up somewhere you’d need to get a particle up in the neighborhood of 10^9 kilograms before you get a black hole with the same radius as a proton. That’s equivalent to around 10^44 electron volts, which is way outside the range of anything that’s ever been observed.
It’s such a weird scenario that I have no intuition whether it makes more sense for that particle to become a black hole or not, so I’ll trust you that it wouldn’t. It’s always humbling to find out that the universe is even stranger than you imagined.
Chronos’s point wasn’t that black holes can’t be formed from lots of energy. It’s just that it needs to be right kind of energy, namely the energy from the mass of the particle (in the “particle at sufficiently-ludicrous speed” scenario). The total energy of a such a particle is reference-frame dependent, so whether it forms a black hole had better not be governed by the total energy.
Right, because something either is or is not a black hole. You couldn’t have something that is a black hole in one reference frame, but is not a black hole in some other reference frame.
Note, by the way, that if you took two ludicrous-speed particles and aimed them at each other, you could get a black hole out of that one.
Ah right, I forgot that within your reference frame, you don’t gain any energy from accelerating. I was just wondering if we had experimental evidence that this didn’t happen or if it was just theoretical, and it turns out it’s only theoretical but the theory is pretty damn solid. Thanks for clarifying!
Yeah, now that you spell it out, I grok how what I was saying doesn’t make sense. I should think harder before opening my cake-hole. I blame the booze.
Would you agree with the revised statement of: “For normal things, like boulders moving much slower than the speed of light, the S-E tensor (for points within the boulder) is dominated by its (0,0) component, which is in turn dominated by the energy density due to mass density, which is why we get away with thinking of gravity as being generated by mass in such situations”?
It’s clear that when there exists a frame in which all components of the stress-energy tensor T can be neglected but T[sup]00[/sup] then T[sup]00[/sup] is the mass density. Also there must be a limit where the mass M enclosed in a volume V is:
M ≈ ∫[sub]V[/sub] T[sup]00[/sup]dV
Otherwise Newton’s law of gravity wouldn’t work. But of course first of all M must be defined in general relativity and all the conditions for it to reduce to the above must be worked out.