rede96 said:
if for example I place two bodies sufficiently far apart, in such a way that they are at rest wrt each other, and the forces acting upon them to keep them together are less than the 'pressure' of expansion, then as I understand it, they will start to recede from each other at the Hubble rate
No. They will start to recede from each other, but if there is a force between them, they won't recede at the Hubble rate at first. Their recession rate will gradually
approach the Hubble rate as time goes on. At least, according to the standard cosmological model, they will; but that model doesn't really apply on small distance scales (see below).
The reason this will happen, in the model, has nothing to do with "space expansion" causing a "pressure". It has to do with the rest of the matter in the universe affecting the two objects. Remember that, in the FRW model, the matter in the universe is a continuous fluid, with the same density everywhere. And the "flow lines" of this fluid are expanding--objects at rest relative to the fluid at different spatial locations will be moving apart. So when you put two objects at rest relative to each other into this fluid, at least one must be moving relative to the fluid. And if there is not enough force between the two objects, then the flow of the fluid will pull them apart, because each one is entrained in the local fluid flowing past it. But if there is at least some force between the two objects, the fluid won't pull them apart at the same rate as the fluid itself is flowing--the objects will pull on each other and counteract some of the fluid's effect. But as the objects get farther apart, the force between them will weaken, so their rate of recession will gradually approach the flow rate of the fluid in general (the Hubble rate).
But, as I've said before, there is a huge problem with all of this if you try to apply it to bound systems on small scales: the matter in the universe is not a continuous fluid! It's not even close. The intuitive model of fluid flow sweeping objects apart is simply
wrong on small distance scales; that isn't what's happening. To see what might happen on small distance scales, we need a model that applies at those scales.
Here's one such model. On average, as viewed from any point, the matter in the universe is spherically symmetric. In particular, if we pick out a bound system, such as the solar system, and draw a boundary around it (say a sphere one light-year in radius centered on the Sun), the matter outside that sphere will be, on average, spherically symmetric. And there is a theorem called the "shell theorem" which says that, if the matter distribution outside some spherical shell is spherically symmetric, it has
no effect on anything inside the shell--we can ignore it completely and just focus on the matter inside the shell when determining what will happen inside the shell. So we can ignore the rest of the matter in the universe when determining what the structure of the solar system will be; we only need to consider the Sun and planets and whatever other objects are large enough to be significant.
The model I just described is what I have been using in this thread. And note that in this model, if the density of dark energy really is constant everywhere, then there is dark energy inside the sphere that bounds the solar system, so it will indeed exert a tiny force and have a tiny effect on the solar system's structure. But the rest of the matter in the universe is not a continuous fluid of the same density everywhere; there isn't any "cosmological fluid" inside the solar system, so it will
not exert any force inside the solar system. The only ordinary matter we have to worry about is the ordinary matter we already know is inside the solar system.