Statistical MechanicsUnlike most other texts on the subject, this clear, concise introduction to the theory of microscopic bodies treats the modern theory of critical phenomena. Provides up-to-date coverage of recent major advances, including a self-contained description of thermodynamics and the classical kinetic theory of gases, interesting applications such as superfluids and the quantum Hall effect, several current research applications, The last three chapters are devoted to the Landau-Wilson approach to critical phenomena. Many new problems and illustrations have been added to this edition. |
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Page x
... Ensemble , 143 7.3 Derivation of Thermodynamics , 147 7.4 Equipartition Theorem , 149 7.5 Classical Ideal Gas , 151 7.6 Gibbs Paradox , 153 ... Ensemble , 165 8.5 Equivalence of the Canonical Ensemble and the Grand Canonical x Contents.
... Ensemble , 143 7.3 Derivation of Thermodynamics , 147 7.4 Equipartition Theorem , 149 7.5 Classical Ideal Gas , 151 7.6 Gibbs Paradox , 153 ... Ensemble , 165 8.5 Equivalence of the Canonical Ensemble and the Grand Canonical x Contents.
Page 165
... GRAND CANONICAL ENSEMBLE We begin a study of the equivalence between the grand canonical ensemble and the canonical ensemble ... Canonical Ensemble and Grand Canonical Ensemble 165 Density Fluctuations in the Grand Canonical Ensemble,
... GRAND CANONICAL ENSEMBLE We begin a study of the equivalence between the grand canonical ensemble and the canonical ensemble ... Canonical Ensemble and Grand Canonical Ensemble 165 Density Fluctuations in the Grand Canonical Ensemble,
Page 167
... grand canonical ensemble have the same number of particles N. Then the grand canonical ensemble is trivially equivalent to the canonical ... CANONICAL ENSEMBLE AND THE GRAND CANONICAL Canonical Ensemble and Grand Canonical Ensemble 167.
... grand canonical ensemble have the same number of particles N. Then the grand canonical ensemble is trivially equivalent to the canonical ... CANONICAL ENSEMBLE AND THE GRAND CANONICAL Canonical Ensemble and Grand Canonical Ensemble 167.
Contents
THE LAWS OF THERMODYNAMICS | 3 |
SOME APPLICATIONS OF THERMODYNAMICS | 33 |
THE PROBLEM OF KINETIC THEORY | 55 |
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absolute zero approximation assume assumption atoms average becomes Boltzmann Bose calculate called canonical ensemble classical collision complete condition consider constant contains coordinates corresponds defined definition denoted density depends derivation determined discussion distribution effect eigenvalues elements energy ensemble entropy equal equation equilibrium excited exists expansion external fact Fermi field finite given ground Hamiltonian heat Hence ideal independent integral interaction lattice levels limit liquid magnetic mass matrix mean molecular molecules momentum n₁ obtain occupation operator particles partition function phase physical positive possible potential pressure probability problem properties quantity quantum quantum mechanics region represented respectively result satisfies shown in Fig solution specific statistical mechanics temperature theorem theory thermodynamic transformation transition unit V₁ V₂ valid volume wave function