nicktacik said:
It would seem intuitive to me, that the moment right after the big bang, should have the same entropy value as the moment right before the 'big crunch',
it does not seem intuitive to me. but people's intuitions differ.
I picture right after bang (or right after inflation if you like it in the story) as very SMOOTH AND UNIFORM
and in the case of gravity a uniform field is the LOWEST ENTROPY.
by contrast, I picture conditions during a crunch as highly lumpy and INHOMOGENEOUS
and in the case of gravity a clumpy irregular field with all kinds of warts pimples and black holes is the HIGHEST ENTROPY
So the question is; does the 2nd law apply in a contracting universe?
Note that I am only familiar with the dS=\frac{dQ}{T} definition of entropy, so please explain any more advanced (ie stat mech) definitions clearly.
conditions at bang (lo entopy) are very different from conditions at crunch (hi entropy) and so, at least in my intuitive picture the 2nd law HOLDS for the entire history of the universe from bang to crunch
you are postulating an unrealistic case where Lambda is zero, in the usual LambdaCDM model we do not expect a crunch, even if Omega > 1 and the universe is spatial closed (as it may very well be).
Roger Penrose has given several talks about applying 2nd Law to Cosmology and if you want to have entropy explained in the context of the gravitational field then you might like to watch and listen to one of his talks, which are online.
Here is a Penrose talk that does the Stat Mech definition with pictures, in the context of cosmology:
http://www.Newton.cam.ac.uk/webseminars/pg+ws/2005/gmr/gmrw04/1107/penrose/
Here Penrose argues that a BOUNCE cosmology is theoretically impossible because entropy is very high at crunch and very low at bang---so how do you bounce from crunch to bang without violating 2nd Law and abruptly setting entropy back to zero, essentially.
This argument is flawed because you have different observers watching the crunch and watching the bang, with different macrostates mapping the phase space. However it is only his argument against bounce that I believe is flawed. The rest of what he has to say is correct, valuable, and very well presented!