The second law of thermodynamics tells us that the entropy of a closed system always increases, so all natural processes tend to increase uncertainty. However, in 1874, a new challenge was posed to the definition of entropy, known as Gibbs' paradox. This paradox causes us to rethink the nature of entropy and calls into question our current understanding of thermodynamics. In this discussion, we will analyze the connotation of this paradox in depth and find its solution.
Gibbs' paradox is based on the quantification problem of the entropy of an ideal gas. When the differentiability of particles is not taken into account, the expression of entropy will not meet the scalability. This means that under certain circumstances the entropy of a system can appear to decrease, thus violating the second law of thermodynamics. Specifically, if you have two identical containers of gas, and when the partition between the two containers is opened to allow the gases to mix, entropy calculations predict that the entropy of this combined system will not be twice the original entropy, This creates the source of the paradox.
When two identical gas containers are mixed, a contradiction arises in the calculation of entropy based on the definition of non-expansive entropy, which casts doubt on the correctness of this definition of entropy.
When considering the entropy of an ideal gas, we need to understand that in a six-dimensional phase space, the state of the gas is determined by the momentum and position of the particles. Calculating the number and range of available states in this multidimensional space is the basis of entropy, but is complicated by the indistinguishability of particles. So when we mix gases by absorbing or releasing particles, we have to rethink the definition of entropy.
If the indiscernibility of particles is not taken into account, the definition of entropy will lead to a misunderstanding of macroscopic state changes.
The key to solving Gibbs' paradox is to assume that gas particles are indistinguishable. This means that when calculating entropy, we should treat all states changed by particle exchange as the same state. This assumption is therefore particularly important when approximating changes in entropy for large numbers of particles. In this way, we are able to avoid the non-scalability problem of entropy and thus make the calculation of entropy reflect reality.
Related to Gibbs' paradox, we also need to consider the hybrid paradox. This paradox emphasizes that if two different gases are mixed, there will be an increase in entropy, but if the two gases are identical, the entropy will not change after mixing. This comparison reveals that the definition of entropy is somewhat subjective, as different gases can be viewed from any experimental or internal state perspective.
Depending on different definitions of entropy, the same mixing process can lead to completely different entropy changes, which highlights the complexity of the relativistic nature of entropy.
The rise of quantum theory provides a new perspective for understanding Gibbs' paradox. According to quantum theory, particle indistinguishability is fundamentally a natural phenomenon and not simply a limitation of experimental technology. This theoretical framework not only helps to clarify the nature of entropy in the microscopic world, but also promotes a bridge between thermodynamics and statistical mechanics, forming a more comprehensive set of physical perspectives.
At the intersection of current scientific understanding of entropy and thermodynamics, we cannot help but ask, what other physical phenomena will trigger new paradoxes in the future to challenge the boundaries of our understanding? Is this indeed the final frontier of thermodynamics, or is it a prelude to further exploration? We look forward to future answers.