TobyC
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SpectraCat said:I am aware of Noether's theorem, and I understand the derivation of energy conservation based on time symmetry. However, I have always found this hard to rationalize with the second law of thermodynamics, which tells us that time is not symmetric, and that an external observer could tell in which direction time was going by observing the entropy change of the universe. Moreover, I believe that several cosmological theories incorporate time-dependence into the physical constants (Planck's constant, the speed of light, etc.) that are the scaling factors for our physical laws.
So is there an explanation of why these considerations don't affect the assumptions involved in the derivation of energy conservation from time-symmetry in Noether's theorem? Or is it that time-symmetry is only a local (with respect to time) property of the universe, in the sense that Noether's theorem works with generators of infinitesimal translations in time? Are there any ramifications of this for conservation of energy over long (i.e. consmological) time-scales? Or am I just way out in left field (always a possibility)?
Well I'm by no means the best person to answer your questions but I'll give it a go anyway.
Firstly, I don't think the second law of thermodynamics is a fundamental law of the universe in the sense that maxwell's equations are for instance. It is instead a probabilistic law which emerges out of the interactions of many many particles. If you take a video of a glass smashing and play it backwards, what you see is not impossible, it is just exceedingly unlikely. The universe, as it progresses in time, moves from improbable states to probable ones, simply because that's what's more likely, and it is this which gives the universe its apparent time reversal asymmetry, even though the fundamental laws are symmetrical under time reversal.
All that is required to explain the asymmetry in the direction of time is to state that the universe started off in an extremely unlikely state initially (although we don't know why is started off that way) and that is enough to give time a direction, since things will look different depending on whether you are going towards this unlikely initial state or away from it.
However, although I don't know much about quantum theory, I do think it has recently been discovered that certain physical laws (I think maybe the weak force?) are genuinely asymmetric under time reversal at a fundamental level. This still shouldn't make a difference to energy conservation though. This is because in Noether's theorem, energy conservation is a consequence of the fact that the laws of physics are invariant under a translation in time. Whether they are symmetrical under time reversal is a different question, you can have one without the other, and although you are justified in raising these issues about time reversal, I am not aware of any new discoveries which throw time translation symmetry into doubt.
As for energy conservation over cosmological timescales, I think you start getting into weird effects from General Relativity there. Even in Newtonian physics, energy conservation only works if you use an inertial coordinate system, but once you get to General Relativity it is impossible to construct a globally inertial coordinate system, so energy conservation in the traditional sense can only be talked about locally.
I think there are ways of constructing a global definition of energy though, which is conserved, but you can't pin the energy down to a precise location like you can in special relativity for instance.