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Published byCarol Hardy Modified over 6 years ago
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} C = 1 F = 2 P = 1 Gibbs phase rule F = C – P + 2
F: # degrees of freedom C: # components P: # phases
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} C = 1 F = 1 P = 2 Gibbs phase rule F = C – P + 2
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} C = 1 F = 0 P = 3 Gibbs phase rule F = C – P + 2
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} C = 1 F = -1 P = 4 Gibbs phase rule F = C – P + 2
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} C = 2 F = 3 P = 1 Gibbs phase rule F = C – P + 2
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} C = 2 F = 3 P = 1 Gibbs phase rule F = C – P + 2 Composition xA
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} C = 2 F = 3 P = 1 Gibbs phase rule F = C – P + 2 Pressure 1 Temp.
Composition xA
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} C = 2 F = 3 P = 1 Gibbs phase rule F = C – P + 2 Pressure 3 allowed
Temp. Composition xA
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C = 2 Partial molar volume
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Partial molar quantities
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C = 2 Partial molar volume Gibbs-Duhem equation
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Thermodynamics of mixing perfect gases/liquids
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Thermodynamics of mixing liquids
Ideal mixing (Raoult)
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Thermodynamics of mixing liquids
Non-ideal mixing
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Temperature-composition diagrams
GE >> 0 vapour GE = 0 liquid Non-ideal solutions GE < 0 GE << 0
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Temperature-composition diagrams
GE >> 0 Non-ideal solutions vapour GE = 0 liquid GE < 0 GE << 0
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