Two points, one on you and the other at the edge of the observable universe, will rapidly begin moving away from each-other and will soon be moving away from each-other at greater than the speed of light, then exiting the observable universe from the perspective of one-another. If you place a third point between the two of them, then the new point will see both the “neighbors” moving away at great speed, but neither leaving what is technically observable. If you place a fourth point in between two of those, everything else will be moving away from it, so on and so forth – but this quickly becomes absurd when you think about it as a solid rope.
This is ultimately because objects bound by a local gravitational influence do not expand. This is a pretty core premise of a lot of cosmology, and why any cosmology (where the expansion of the universe is relevant) usually starts by measuring the smallest distances at 500 megaparsecs, wherein you can treat galaxies like point sources of light. At that distance you qualify all of space as homogeneous (because it is beyond the point where space is spotty, and then beyond the point where space is fractal) and you can treat the expansion of the universe as happening everywhere. In this case your rope is made of galaxies separated from each-other by 500 megaparsecs each.
If this rope worked, you could also deploy a rope in space by first sending out a few billion meters of rope and if it’s creating space-energy then I’d imagine it would find higher energy states by pulling out more. Haven’t thought that one through very much but it’s a fun thought that space would suck the rope into the abyss like a big spaghetti.
Wouldn’t very large objects just inherently heat up for no reason?
But that’s not the topic of the conversation. 2nd law of thermodynamics is definitely weird, but if you think it’s wrong we can take bets on different physical bodies. I’ll bet on entropy increasing, you can bet against it. I’ll put down my life savings.
Ergodicity more or less tells us that the likelihood of finding a particular type of state is more or less baked into its multiplicity. There are many more configurations of gas particles in a room where they’re just sort of spread apart evenly than there are where they’re all packed into a corner as tight as you can get them. And I don’t think anybody is telling you “if you measure a system at T=t, then at T=t+dt where dt is almost no time at all, then the state of the system will be entirely random and every atom might have fallen to the floor”. It’s more like, if you measure the state of a room at two periods of time that are greater than the amount of time it might take for the atoms to shuffle around ( a few seconds for a room at 70f, maybe) then you’ve really got no idea what exact system it evolved into. A lot of physics is super hand-wavy like that because the math gets super unsolvable obnoxiously fast.
Interested in disagreements. My source for the thermo stuff is only a couple classes, but I took a lot of independent studies in cosmology with a professor who spent a great deal of his professional life working as or with cosmologists. The universe at very large scales doesn’t behave like it does locally, and building a rope 500 megaparsecs long is just all kinds of broken.