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Chapter 14 Part III- Equilibrium and Stability. A system with n components and m phases Initially in a non-equilibrium state (mass transfer and chemical.

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Presentation on theme: "Chapter 14 Part III- Equilibrium and Stability. A system with n components and m phases Initially in a non-equilibrium state (mass transfer and chemical."— Presentation transcript:

1 Chapter 14 Part III- Equilibrium and Stability

2 A system with n components and m phases Initially in a non-equilibrium state (mass transfer and chemical reactions may take place) T and P are uniform System is in thermal and mechanical equilibrium with surroundings What changes may happen to the system? What will be the final state of the system?

3 Changes to the system translate to: Heat exchange Expansion work By the second law, what happens to the entropy?

4 dS sys + dS surr > 0 dS sys - dQ/T > 0  dS sys > dQ/T dQ < T dS sys By the first law, dU sys =- PdV sys + T dS sys dU sys + PdV sys < T dS sys, or dU sys + PdV sys -T dS sys < 0

5 Valid for any closed system The inequality determines the direction of change between non-equilibrium states The equality holds for changes between equilibrium states (reversible)

6 dU sys + PdV sys -T dS sys < 0 Special cases: – At V and S constant (dU sys ) SV < 0 – At U and V constant (dS sys ) UV > 0

7 Process at constant T and P dU TP + d(PV) TP –d(TS) TP < 0 d(U+PV-TS) TP < 0 (dG) TP < 0  All irreversible processes at constant T and P tend to decrease the Gibbs free energy

8 Equilibrium criterion For a closed system at constant T and P, the Gibbs free energy is a minimum Given an expression for G, we find the set of composition values that minimize G

9 At equilibrium, differential changes may occur The system is not static !!! At constant T and P changes may happen but they do not change G. Therefore: (dG) TP = 0

10  G mixing = G –  x i G i If the system is stable, G must decrease, therefore G <  x i G i, G –  x i G i < 0 For curve II, the system has a lower G by splitting into two phases than in a single phase (at compositions between x 1  and x 1  )

11 Stability criterion for a single phase binary system At constant T and P,  G and its first and second derivatives must be continuous functions of x 1, and the second derivative must everywhere be positive

12 Alternative stability criterion: Relation to G E Since At constant T and P

13 Other alternative stability criteria Alternative criteria, at constant T and P, valid for each of the components:

14 How the stability criteria affect VLE? How is the criterion for component 2?

15 For an ideal gas mixture, you can show that Then the stability criterion is dy 1 /dx 1 > 0 What does it mean for a y-x diagram?

16 For the liquid phase, at constant T and P Low pressure VLE, assume ideality of gas phase, you can show What can we say about the sign of dP/dx1?

17 Therefore, what is the sign of dP/dy1? What happens at an azeotrope?

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