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Termodinamica 2

Università degli Studi di MILANO-BICOCCA scienza dei materiali 2025
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  • Gibbs' Phase Rule:
    • For non-reactive systems with F phases and C components, the number of degrees of freedom (variance, V) is given by V = C + 2 - F.
    • This rule quantifies how many intensive variables (like pressure, temperature, or composition) can be independently varied while maintaining phase equilibrium.
  • Derivation of Phase Rule:
    • System Descriptors: A single phase is described by P, T, and C-1 independent molar fractions, totaling C+1 intensive variables. For F phases, there are F(C+1) total variables.
    • Equilibrium Constraints: Thermal, mechanical, and chemical equilibrium conditions impose (C+2)(F-1) constraints on the system.
    • Variance Calculation: V = F(C+1) - (C+2)(F-1), which simplifies to V = C + 2 - F.
  • Examples of Phase Rule Application:
    • For a single component (H2O, C=1): V=2 for one phase, V=1 for two coexisting phases, and V=0 for three coexisting phases (triple point).
  • Systems with Chemical Reactions:
    • If R independent chemical reactions occur, the variance is further reduced, and the formula becomes V = C + 2 - F - FR.
  • Clapeyron Equation (Monocomponent Systems):
    • Describes the P(T) coexistence curve between two phases (α and β) for a single component (C=1).
    • Derived from the equality of chemical potentials (dµα = dµβ) and the Gibbs-Duhem relation (dµ = -SdT + VdP).
    • The equation is dP/dT = L / (T(Vα - Vβ)), where L is the latent heat of transition and ΔV is the molar volume change.
  • Clausius-Clapeyron Equation (Gas-Phase Approximation):
    • A simplification of the Clapeyron equation used when one phase is a gas (e.g., liquid-gas transition).
    • It applies two approximations: the gas behaves ideally (V_gas ≈ RT/P) and its molar volume is significantly larger than the condensed phase (V_gas >> V_condensed).
    • These approximations lead to dP/dT = LP / (RT²), which can also be written as d(lnP)/dT = L / (RT²). This is crucial for understanding vapor pressure curves.
  • P-V Isotherms and Phase Transition:
    • P-V diagrams illustrate phase transitions, showing regions of constant pressure during condensation (e.g., gas to liquid).
    • The validity of the ideal gas model at high temperatures and low pressures justifies the approximations used in the Clausius-Clapeyron equation for those conditions.

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