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I have heard that identical distinguishable classical particles having different ''statistics''.It is the limit of quantum case.Then we mix many parts(cells) of identical gases, the total entropy increases.I can not derive this limit from quantum particles to classical particles(please help me).I only know that by the thisness of classical particles we can ''paint'' each classical particle with one ''colour'',so that when we mix many cells of identical gases,the entropy will increase.

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A. Neumaier
Please spend more time formulating proper questions (and edit your initial post!): The paradox is called after Gibbs, not Gibb. Distinguishable particles cannot be identical (which would make them indistinguishable). If you mix quantities of the same gas, nothing happens; the entropy doesn't increase.

Thus your question is very unclear. However, the answer may well be already here: https://en.wikipedia.org/wiki/Gibbs_paradox; [Broken] so please study this first. If this is not sufficient then (with considerably more work to do for you) here: http://www.mdpi.org/lin/entropy/gibbs-paradox.htm

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I will be more carefull!After reading Reichl carefully I think I might understand the resolution of Gibbs paradox.But I do not understand why there are identical classical particles because classical particles are distinguishable.Then if we mix many parts of same gas the entropy would increase.

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vanhees71
Gold Member
I'd say the Gibbs paradox has been already solved before the discovery of quantum theory by Boltzmann in introducing a ##1/N!## when counting the single-particle microstates in a classical phase-space volume. The idea behind it is indeed the indistinguishability of particles with the same intrinsic properties (where with intrinsic properties I mean those that characterize the particle's properties in its rest frame; classically that's mass and perhaps rotational degrees of freedom in the rigid-rotator model of molecules).

The real problem with classical statistical physics is that there's no natural phase-space measure and no way to definitely count the single-particle microspace in a classical single-particle phase-space volume. This is only resolved by the introduction of Planck's constant, providing a natural scale of the dimension of action, and the quantum definition of states.

For an elementary treatment, see

http://fias.uni-frankfurt.de/~hees/publ/kolkata.pdf

Sects. 1.5 and 1.8 for the (semi-)classical and quantum treatment of the entropy.

Then depending on conceptional choice of considering classical particles as identical or distinguishable particles(having same intrinsic properties),we would have entropy increasing or not changing of the mixing of many cells of same gas.That resolves Gibbs paradox.Is this right?

A. Neumaier
Then depending on conceptional choice of considering classical particles as identical or distinguishable particles(having same intrinsic properties),we would have entropy increasing or not changing of the mixing of many cells of same gas.That resolves Gibbs paradox.Is this right?
There is only one correct choice, and that resolves the problem: On must treat the classical particles as indistinguishable by weighting the contributions appropriately. This was Gibbs' solution (found at a time when only classical mechanics existed).

Then where is the wrong of the application of reason for mixing different gases to the same gases that leads to the paradox.In Reichl page 66 the reason is general not depending on the types of gases.

DrDu
I think that there are several solutions to the Gibbs paradox. One involves recognition of the indistinguishability of identical quantum particles. But the paradox is also resolvable for distinguishable classical particles: The point is that we don't know which particle is in which container even before mixing the two gasses. So entropy doesn't increase on mixing. If we would measure which particle is in which box, we would accumulate a lot of information which would be converted into entropy on deletion of the memory after mixing.

dextercioby
I agree with many solutions to Gibbs paradox.But I mean I would like to find out ''the wrong point'' in the argue leading to the paradox,because the argue is general.

vanhees71
Gold Member
There is only one correct choice, and that resolves the problem: On must treat the classical particles as indistinguishable by weighting the contributions appropriately. This was Gibbs' solution (found at a time when only classical mechanics existed).
Interesting, I thought it was Boltzmann who solved the problem, but I'm not sure. One should find some book/paper on the history of statistical mechanics.

vanhees71
Gold Member
Then where is the wrong of the application of reason for mixing different gases to the same gases that leads to the paradox.In Reichl page 66 the reason is general not depending on the types of gases.
Of course, there's no paradox, if the gases in the two halves of the container are different originally and then mixed by taking (adiabatically) out the divider wall, because the state measurably changes from the two different particles separated ("ordered") to them being mixed and in complete thermal equilibrium ("less ordered"), i.e., the entropy must grow. If the two gases are made of the same particles, then nothing changes in the thermodynamical state when the divider wall is adiabatically taken out, and thus the entropy should not change.

The solution is to put appropriate factors ##1/N_i!##, ##i## labeling the different species of the molecules making up the gases in the mixture.

A. Neumaier
Interesting, I thought it was Boltzmann who solved the problem, but I'm not sure. One should find some book/paper on the history of statistical mechanics.
The wikipedia article on Gibbs' paradox mentions Boltzmann (''correct Boltzmann counting'') but gives no reference to his work. Jaynes refers to Gibbs 1875 for the resolution.

In Reichl's book page 66,she write down the Gibbs free energy of mix gases,then calculate entropy through it.But Gibbs potential is additive,so entropy is also additive despite of the same type of gases.Then it leads to paradox.I would like find out the ''wrong'' in this argue,

A. Neumaier
In Reichl's book page 66,she write down the Gibbs free energy of mix gases,then calculate entropy through it.But Gibbs potential is additive,so entropy is also additive despite of the same type of gases.Then it leads to paradox.I would like find out the ''wrong'' in this argue,
In the version I have (2nd ed. 1998), she discusses the Gibbs paradox in Section S2.B p.72ff and refers for its resolution to quantum mechanics. Jaynes article linked to in post #12 gives Gibbs' classical resolution.

The Gibbs potential G(P,T.n1,...)=Sigma(njRT(Phi(T)+lnP+lnxj)),then what is wrong with partial pressure(xj) of identical particles?The increasing of entropy is result of xj.

A. Neumaier
You can find yet another discussion of Gibbs' paradox in my online book, pp.237-239. But I am not going to do for you the work of understanding one of the explanations offered (by Reichl, Jaynes, or my book).

By the way, you still haven't corrected the title of your thread. (Click on thread tools at the top of page 1 to make the correction.)

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The no answer still help me understand the Gibbs paradox,because it make me rethinking!
I do not know how to correct the title of post 1,because having not the edit function.
Thank you very much for your great helps.

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A. Neumaier