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Published byMagdalen Thomas Modified over 6 years ago
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Chapter 13 Macromolecules in Solution: Thermodynamics and Equilibria
13.1 Fundamentals partial molar quantities partial specific quantities partial molar volume partial specific volume
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Total volume of system
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Chemical Potential (partial molar free energy) G = H –TS =E + PV -TS Gibbs-Duhem Eq.
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The Ideal and Nonideal Solutions
Molar free energy of pure component Valid for
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Entropy change in mixing from Chapter 2
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1: solvent, 2: solute The chemical potential of the solvent should be reduced by adding solute
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Virial coefficient
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Protein aggregation Solute shape
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13.2 Application of the Chemical Potential to Physical Equilibria
Dialysis Equilibrium 1 2 At equilibrium, a(tot) = a(free) + a(bound)
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Osmotic Pressure Pure Solvent Solvent + Solute
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If the solution is very dilute,
Osmotic pressure Y = b a X
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Y = b a X
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