Sections#
equations_of_state – the ideal gas law, van der Waals continuity of liquid and gas, Redlich-Kwong, Peng-Robinson vapor pressures, and Lewis fugacity.
phase_equilibria – the Clausius-Clapeyron vapor-pressure curve and the Gibbs phase rule.
equilibrium – the law of mass action, Gibbs-energy minimization, the van’t Hoff plot, and Le Chatelier’s principle.
thermochemistry – Hess’s law and Nernst’s heat theorem.
mixtures – Raoult’s-law P-x-y diagrams, Henry’s law, van’t Hoff’s osmotic pressure, and Margules activity coefficients.
Equations of state#
The ideal gas law, van der Waals, Redlich-Kwong, and Peng-Robinson equations of state, and Lewis fugacities computed from them.
Andrews and van der Waals: continuity of the liquid and gas states
Redlich-Kwong isotherms of CO2 against van der Waals and the ideal gas
Peng-Robinson: vapor pressures from the acentric factor
Lewis fugacity: the effective pressure of a real gas
Reaction equilibrium#
The law of mass action, Gibbs-energy minimization, the van’t Hoff plot, and Le Chatelier’s principle.
Guldberg and Waage’s law of mass action: Q = K at equilibrium
Gibbs’s equilibrium criterion: minimum total Gibbs energy
Le Chatelier’s principle: equilibrium shifts that oppose a disturbance
Mixtures and colligative properties#
Raoult’s-law P-x-y diagrams, Henry’s law for dilute solutes, van’t Hoff’s osmotic pressure and the colligative properties, and Margules activity coefficients for non-ideal solutions.
Raoult’s law and the P-x-y diagram of an ideal solution
Henry’s law: the dilute-solute limit of a real solution
Margules activity coefficients: deviations from Raoult’s law
Phase equilibria#
The Clausius-Clapeyron liquid-vapor phase boundary, and the Gibbs phase rule.
The Clausius-Clapeyron vapor-pressure curve of water
Thermochemistry#
Hess’s law of constant heat summation and Nernst’s heat theorem: reaction enthalpies built from steps or formation enthalpies, and the behavior of reaction entropies and free energies as the temperature approaches absolute zero.
Hess’s law: reaction enthalpy does not depend on the path
Nernst’s heat theorem: reaction entropy vanishes at absolute zero