Understanding the Boiling Point: Thermodynamic Proof

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Adding heat to a liquid at its boiling point can either raise its temperature slightly or cause a phase change to vapor, but experiments show that the temperature remains constant until the phase change is complete. This behavior can be explained through the concept of free energy, where the free energy of the liquid is lower below the boiling point and that of the gas is lower above it. At the boiling point, the free energies of both phases are equal, necessitating the conversion of liquid to vapor to minimize free energy when heat is added. While thermodynamics provides a framework for understanding this process, deriving the specific dependence of free energy on temperature requires insights from statistical mechanics. Thus, a complete understanding of phase transitions involves both thermodynamic principles and statistical mechanics.
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If we add a small amount of heat δq to a liquid at its boiling point Tb, it could either increase its temperature a small amount dT = δq/Cv, or suffer a phase change into vapor.

Experimentally, we see that liquids remain at Tb until the phase change is complete, and only then continue increasing their temperature. Why is this?

I want to prove this macroscopically, that is, from thermodynamics, but I don't know where to start. Any leads?
 
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The way you do this is by looking at free energy. Bellow the Tb, the free energy of a liquid is lower. Above, free energy of gas is lower. At Tb, the free energy of the two phases is the same. So to get an absolute lowest free energy, the substance must convert part of liquid to vapor in response to added energy, until there is no more liquid left.
 


Can what you just said be proved from the laws of thermodynamics, without looking up ΔG values on tables?
 


Like I said, if you take for granted that different phases have different rate at which free energy changes with temperature, that's all you need to prove that phase transition happens at a specific temperature for pure substance.

If you want to derive the actual dependence of free energy on temperature, then you need statistical mechanics. As far as I know, thermodynamics by itself is insufficient.
 
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