For first order phase transition at constant t anf p the gibbs function
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In the absence of latent heat and volume change above the critical point the surfaces of the Gibbs free energy G for the liquid and the gas phase do not intersect any more. Instead the system passes continuously along a single G-surface.
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In the absence of latent heat and volume change above the critical point the surfaces of the Gibbs free energy G for the liquid and the gas phase do not intersect any more. Instead the system passes continuously along a single G-surface.
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