Derivation
The Gibbs free energy total differential natural variables may be derived via Legendre transforms of the internal energy.
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Because S, V, and Ni are extensive variables, Euler's homogeneous function theorem allows easy integration of dU:
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The definition of G from above is
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Taking the total differential, we have
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Replacing dU with the result from the first law gives
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The natural variables of G are then p, T, and {Ni}. Because some of the natural variables are intensive, dG may not be integrated using Euler integrals as is the case with internal energy. However, simply substituting the result for U into the definition of G gives a standard expression for G:
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