Concept:
During a phase change of a pure substance occurring at constant temperature ($T$) and pressure ($P$), the two phases coexist in thermodynamic equilibrium.
Let us examine how the different thermodynamic properties behave during a phase transition like boiling water to steam:
• Specific Internal Energy ($u$) & Specific Enthalpy ($h$): Heat (latent heat) must be added or removed to break intermolecular bonds during a phase transition. This causes a discontinuous jump in internal energy and enthalpy ($\Delta h = \Delta h_{\text{latent}} \neq 0$).
• Specific Entropy ($s$): Because heat is transferred, the molecular disorder changes ($\Delta s = \frac{\Delta h_{\text{latent}}}{T} \neq 0$).
• Specific Gibbs Free Energy ($g$): The criterion for phase equilibrium at constant $T$ and $P$ requires the chemical potential ($\mu$) of both coexisting phases to be equal. For a pure component, the chemical potential is identical to the specific Gibbs free energy:
\[
g_{\text{phase 1}} = g_{\text{phase 2}} \implies \Delta g = 0
\]
Step 1: Apply the fundamental property relation for Gibbs Free Energy.
The fundamental differential equation for $g$ is:
\[
dg = v \, dP - s \, dT
\]
During a phase transition, both temperature and pressure are fixed, so $dP = 0$ and $dT = 0$. This confirms that $dg = 0$, meaning the specific Gibbs free energy remains continuous and unchanging as a molecule transitions from one phase to another.