Circular argument in the first law of thermodynamics ?

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The discussion centers on the interpretation of the first law of thermodynamics and its relationship to the definition of heat. It argues that the first law, expressed as dE=dQ-dW, is not circular if heat is treated as an axiomatic definition. The first law is phenomenological, emphasizing that energy does not spontaneously arise, and the distinction between heat and work can be arbitrary based on the system's degrees of freedom. The conversation highlights the difference between fine-grained and coarse-grained entropy, noting that practical applications often rely on the latter. Ultimately, the clarity of the first law hinges on understanding these definitions and their implications in thermodynamic systems.
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According to Caratheodory, the first law of thermodynamics (dE=dQ-dW) could be derived from the definition of heat (dQ=dE-dW), whether this form a circular argument or tautology ? How to clarify the confusion between the first law of thermodynamics and the definition of heat,and capture the true meaning of the first law of thermodynamics?
 
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It's not circular if the definition of heat is taken to be axiomatic (provided without proof as a starting point for defining the rules of a system). It would be circular if the definition of heat were simply acquired from the first law.

The first law is phenomenological; it captures the observation that energy never seems to arise on its own in the middle of nowhere. Note that the work part can contain a variety of terms, though: chemical, mechanical, electrical, magnetic, etc.
 
Heat is defined by specifying what degrees of freedom of the system are going to be treated in a statistical way. Usually we specify one or two degees of freedom that are not treated statistically. The energy associated with changing these degrees of freedom is then, by definition, work.

But in principle, the partitioning of energy change between heat and work is completely arbitrary. If you keep track of the exact state of a system then the entropy is zero and unitary time evolution then causes the entropy to stay zero at all times. This is called the "fine grained entropy". In practice we use what is called the "coarse grained entropy", which is larger than zero as a result of not keeping track of all the degrees of freedom in the system.
 
"The amount of work required to change the state of an otherwise adiabatically isolated system depends only on the initial and final states, and not on the means by which the work is performed, or on the intermediate stages through which the system passes." http://ocw.mit.edu/OcwWeb/Physics/8-333Fall-2007/LectureNotes/index.htm
 
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