Why heat can't be expressed as exact differential function?

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SUMMARY

Heat and work cannot be expressed as exact differential functions due to their dependence on the path taken during a process. In contrast, internal energy is a state function, defined as an exact differential function, which depends on multiple thermodynamic coordinates. The relationship can be represented mathematically as ##U = U(S,x_1,...,x_n)##, indicating that internal energy requires n+1 coordinates for its complete description. This distinction is crucial for understanding thermodynamic potentials and their representations, such as Helmholtz free energy.

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manimaran1605
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(1) Why differential of work, heat can't be expressed as exact differential function?
(2) How differential of internal energy is an exact differential function and how it is a function of any
two of thermodynamics coordinates?
 
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manimaran1605 said:
(1) Why differential of work, heat can't be expressed as exact differential function?

Because work and heat individually depend on the path taken or process considered. There are countless examples of this all around you.

manimaran1605 said:
(2) How differential of internal energy is an exact differential function and how it is a function of any
two of thermodynamics coordinates?

Internal energy is defined to be a state function, there's nothing deeper to it. It wouldn't even make sense to call it internal energy if it wasn't a state function. Also it isn't true that the internal energy is necessarily a function of only two thermodynamic coordinates. In general ##U = U(S,x_1,...,x_n)## where ##x_i## are a set of generalized coordinates so one requires ##n+1## coordinates, including ##S## in the usual energy representation, and performing Legendre transforms to go to e.g. the Helmholtz or Gibbs representations will not change this. In the Helmholtz representation for example we would have ##F = F(T,x_1,...,x_n)## where ##F## is as usual the Helmholtz free energy. Of course the choice of ##S## for ##U## and the choice of
##T## for ##F## are just a matter of convenience for that specific thermodynamic potential and its associated fundamental relation (although not necessarily convenient for experiment). Indeed I can just as well write ##U = U(T,x_1,...,x_n)## if I wish by inverting ##S## as a function of ##T## but I still need ##n+1## variables.

Mathematically, ##U## is entirely determined by the equations of state and the heat capacity.
 
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