gregtomko said:
I am asking about the energy needed to cause the acceleration of the expansion.
Drakkith said:
Hmm. Would there even need to be an expenditure of energy? Or just a force? It isn't that objects are getting pushed away from each other, gaining velocity in space, but that space is expanding in between them.
gregtomko said:
What is the difference between objects gaining separation in space, and space expanding between objects?
Drakkith said:
For one, an object cannot exceed the speed of light as measured by traveling through local space. (Non-expanding space around massive objects) However, two galaxies can be receding from one another at a rate greater than the speed of light because neither are traveling through local space anywhere close to that speed. Instead space itself is expanding between them, carrying them apart.
gregtomko said:
I thought relativity excluded that possibility. Doesn't time skew as the rate of those galaxies separation increases?
Drakkith said:
No, because they are not traveling through local space at near the speed of light. If we could cut away all the space between us and that galaxy it would be traveling very close to our own speed.
There is no acceleration on the mass itself, the acceleration is only causing the rate of expansion to increase. IE how fast a volume of space expands to a certain size, say double it's current volume.
gregtomko said:
If the stars aren't actually accelerating away from each other, I can see how there would be no way to calculate the energy needed. That is definitely where my confusion arises. That was the whole basis of the question. Thanks so much for your input! I think you cleared this up.
This is a good discussion about something that confuses a lot of us. I put the quotes all together so I could reflect and maybe add some comments, or others could comment. Actually I hit the wrong key and lost my first set of comments, so I'll just post this and try to return to it later.
It is right that a largescale uniform pattern of expanding distances is not like ordinary motion. Nobody gets anywhere. It does not involve ordinary kinetic energy (except in the small local random motion of galaxies which we can neglect). Accelerating the expansion of geometry does not involve inputting kinetic energy. You can consider the galaxies as sitting still and just the distances between all of them increasing by some percentage per unit time.
Actually maybe I don't need to say more because if you read what Drakkith is saying here he is getting the important idea across very clearly. You don't have to worry about putting in kinetic energy to the galaxies because they are not going anywhere. The distances between them are just expanding, by a small annual percentage which amounts to 1/140 of one percent per million years.
If you pick two galaxies at random from all those we can see with the Hubble telescope then typically the distance between them will be so great that even 1/140 of one percent growth in a million years means the distance is increasing faster than c. But this is of no great concern. It is just result of the small percentage expansion in geometry that commonly features in solutions to the Einstein Field Equation (EFE). The EFE governs how geometry evolves and how it interacts with matter. It's our basic law of gravity (having replaced Newton's), well-tested, accurate and the best we have so far. It develops singularities at very high density and people are working on ways to fix that. It says basically that gravity=geometry and to describe gravity properly you need to describe how geometry evolves (both of its own accord and in interaction with matter.)
Whatever universe you live in, if you buy the EFE then you are likely to get a little bit of distance expansion (or contraction) into the bargain. Can't think of any way to say this better, at the moment, than what Drakkith already said. Good conversation. Thanks to Greg T for asking the questions.
Also Twofish is making an important point about the absence of an energy conservation law in expanding geometry. I guess part of that point is that for small distances, even say the size of the galaxy, or the distances to the nearest galaxies, those distances are so small that the percentage expansion is negligible. 1/140% per million years is like nothing. So to good approximation we can neglect expansion of distances and treat geometry as static. And we therefore have energy conservation (likewise to the same good approximation.) It is at larger distance scales where that static approximation is no longer good that we have to acknowledge problems with the definition and conservation of energy.