LizR wrote:
On 7 November 2014 13:29, Bruce Kellett <[email protected] <mailto:[email protected]>> wrote:

    meekerdb wrote:
        On 11/6/2014 4:08 PM, Bruce Kellett wrote:
            meekerdb wrote:

                You seem to overlook that the "expansion" is very likely
                just tautological, i.e. it is nomologically necessary
                that the AoT points in the direction of bigger.

            No, it points in the direction of higher entropy.

        Sure, but the physics is such that entropy must increase in the
        direction of expansion - the two are linked (that's what I meant
        by "nomologically necessary").

    I disagree. There is no necessary connection between the expansion
    and the increase in entropy. The total possible entropy might
    increase with expansion, but if we are always a long way below the
    total possible for a given volume, the entropy could increase
    whether the universe were actually expanding or contracting.
    Anything else and you are necessarily committed to a reversal of the
    arrow of time if the universe begins to re-contract at some point.

This may be why the AOT exists, now that we've discovered dark energy. A recontracting universe may not have one, because the two cancel out, so anthropically we find ourselves in a U with Dark Energy. (Just a thought.)

I don't think that makes much sense -- how can arrows-of-time cancel out?

As far as we know the thermodynamic AOT isn't due to fundamental physics. That is, entropy isn't a fundamental feature of physics (despite that famous quote from Arthur Eddington) but an emergent one. Below a certain .level of "coarse graining" it disappears. At the very fine scale (eq particle) all interactions are reversible and it is impossible to define entropy (except for bound states - these emerged at an earlier stage of the universe from a collection of unbound states in which all interactions were time-symmetric - see below).

Just because something is emergent does not mean that it is not fundamental. Sure, the AoT arises, with entropy, when you coarse-grain things. But there is very probably a deep connection with QM here -- you only get definite results for quantum experiment when you coarse-grain. That is what the partial trace of the density matrix, needed to go from the initial pure state to the final state mixture, is actually doing. It amounts to ignoring certain information because it is lost in the coarse-graining. Entropy arises in the same way -- you ignore certain microscopic information in the interests of the larger picture. The second law -- increasing entropy -- then follows as a matter of statistics. So it is as fundamental as getting a particular result in a quantum experiment -- and it is hard to get more fundamental than that!


Hence logically you need to connect the thermodynamic AOT to something that *is* fundamental, or at least more so, to explain why it exists. The expansion is a possible reason and given that it's THE major feature of the entire universe that is time-asymmetric, it looks like an obvious candidate. Plus, even to a bear of little brain like me, the links aren't particularly obscure, although there are some obscure details involved (but that's only because we, or at least I, don't know everything about everything).

Generically, expansion cools aggregates of particles. It does this by separating out particles according to velocity - a particle that is moving faster than average in a region tends to leave it and move to a region where the average speed is nearer to its own velocity. This effectively cools the particle, and hence all the particles cool as expansion proceeds. Also, matter gets less dense, which is also important in generating an AOT since it allows structures like galaxies to form from an almost uniform matter background.

This is not how it works in cosmology. The expansion is uniform, so it does not separate particles according to velocity. That would probably not even work if the expansion were of a hot gas into empty space. And the cosmological expansion most definitely is not like that!

Cosmological expansion works in different ways depending on whether the matter in the universe is in the form of radiation, or of particles. If it is radiation, the expansion stretches the wavelength as well as decreasing the density, so the energy content falls off like r^{-4} rather than r^{-3} that we have for particles. The density of particles decreases because they get spread out, but their relative velocities do not change.

In the beginning, all matter was very energetic, in the extreme relativistic domain, so everything was effectively radiation, and cooled by that law (1/r^4). But since matter and anti-matter annihilated to produce photons, the number of photons dominated over the number of particles, so the 1/r^4 cooling continued. Once it reached a temperature below the ionization energy of Hydrogen atoms, atoms were able to form. The universe suddenly became transparent. The radiation from this time is what we now see as the CMB.


Let's start at the quark soup era. Things are a big vague before that.

Expansion cools the soup, and eventually collision energies drop enough for nucleons to form without being blown apart by subsequent collisions. This is an early (perhaps the earliest) example of how a system that is in equilibrium, and in which all interactions are time-symmetric, can change to one in which there is some structure simply by expanding and hence cooling it.

Expansion cools the nucleons, until nuclei can form...
Expansion cools the nuclei, until ionised atoms can form...
Expansion cools the atoms, until neutral atoms can form...

As outlined above, this is not really correct.


Expansion now allows a more or less uniform gas to clump into larger scale structures by amplifying any existing inhomogeneities. This allows stars etc to form, and eventually us, without introducing any new physics; all the large scale structure is emergent from time-symmetric physics operating on mass-energy during a non-time-symmetric cosmological expansion.

Again, the facts are rather different. Gravity comes into the picture, and gravity can only work on pre-existing inhomogeneities. But the large scale clumps are gravitationally bound, so they take no more part in the overall expansion. They do not, therefore, cool further because of expansion. The only way primeval clouds of gas can clump further is if they lose energy. Charged particles can lose energy because when they collide they can radiate. The radiation is not gravitationally bound, so that energy is lost to the system, which cools - ultimately enough to coalesce into stars and planets. Electromagnetic interactions producing radiation are essential for this further cooling and clumping. We see a dramatic instance of the effect of not having a simple cooling mechanism in the more-or-less uniform distribution of dark matter throughout galaxies. Dark matter was part of the initial inhomogeneities that gave rise to galaxies, but it lacked the possibility of radiating away energy, so it could not clump further. It does cool very slowly by evaporative processes, but it is essentially unclumped, even now.

These process are all described by time-reversible dynamics, of course, but quantum-level coarse graining is still necessary, so statistics and the thermodynamic arrow are universal in these processes.


(Another way to look at this is that the expansion is producing more available states for the universe to move into, effectively raising the entropy ceiling. This means an expanding universe can never reach a state of equilibrium - this is particularly clear during the BB fireball, which I would say is very near to equilibrium for a lot of the time.)

As mentioned above, that homogeneity assumption is as unjustified as the past hypothesis of low entropy in the initial state.


The above sketches how you get the components of the entropy gradient. Each stage is reversible except for black hole formation (which is another topic since it may also violate unitarity, and may generally need more investigation). But if we ignore gravitational collapse, we can definitely get an AOT from expansion + time-symmetric physics.

PS as a side issue, note that in gravitational collapse, you effectively get a mini-big-crunch which illustrates some of the features of time reversal. In particular, note that in normal time, objects are constrained to have certain types of pasts - what we can lower entropy. In gravitational collapse, objects are constrained to have a certain type of future - it is physically impossible to avoid certain outcomes (at least assuming GR is correct "all the way down" - which admittedly violates the BH information paradox...) With the usual caveats, this at least suggests that time would indeed reverse in a collapsing universe.

Black hole formation does not lead to reduced entropy. One of the fundamentals of BH physics is the Bekenstein bound, which states that the BH is the highest entropy state for an amount of matter equal to the mass of the BH.

But even this is overturned by Hawking radiation. Hawking radiation also increases the total entropy of the system, so in the very far distant future, when everything has collapsed into BHs and evaporated again, the entropy is even higher than if the total universe were a single black hole! The final state of the universe is a very high entropy deSitter space.

Cheers,
Bruce

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