01 January 1970 7 3K Report

Logical Contradiction of Theorem 2 of Thermodynamics

Second Theorem of Thermodynamics: The natural process of isolated system always proceeds in the direction of increasing entropy, and the equilibrium state corresponds to the state of maximum entropy.

The second theorem of thermodynamics has a limitation on the object of study: isolated system. The following is an isolated system, but the second theorem of thermodynamics has some problems in its application: there are two cups of water A B on the table, there are a lot of charges suspended in the water, and the outside world treats them.

Without effect, they can be regarded as isolated systems as a whole. According to the second theorem of thermodynamics, the system should have a stable equilibrium state. We can see from part: For example, A, which is affected by B's electricity, can not be regarded as an isolated system, whether it has a stable state, it is very problematic. The same is true of B. Different research results may exist in the same research object, which can only explain the shortcomings of the theory for such research object.

Whether the system is stable or not depends on the physical equation and experimental determination. The physical equation should include heat and electricity.

1) Poisson equation

2) p=A*exp(-qu/kT)

Solving the equation is difficult, it is non-linear, intuitively speaking, the possibility of solution is small. This shows that the second theorem of thermodynamics can only be applied to systems without long-range interactions.

However, the interaction of gravity between celestial bodies cannot be ignored. It will also destroy the isolation of the system. Any galaxy is disturbed by other galaxies, and the second theorem of thermodynamics is not applicable. When the second law of thermodynamics was just established, people applied it to the universe and obtained the theory of cosmic thermal death. From the above discussion, the cosmic thermal death theory is meaningless, because the second law of thermodynamics is a finite law.

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