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Then Clapeyron equation is:
So: dP/dt is (+) but much smaller than S – L boundary.
Assuming ideal behavior we know that: Vm(g)=RT/P, then the final Clausius Clapeyron Equation would be:
Assuming ideal behavior we know that: Vm(g)=RT/P, then the final Clausius Clapeyron Equation would be:
And if we assume that the change in enthalpy is almost constant: