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 41
Kerson Huang. Potential energy Potential energy d Separation Separation Fig . 2.8 . Typical intermolecular poten- tial . Fig . 2.9 . Idealized intermolecular poten- tial . In most substances the potential energy between two molecules as ...
Kerson Huang. Potential energy Potential energy d Separation Separation Fig . 2.8 . Typical intermolecular poten- tial . Fig . 2.9 . Idealized intermolecular poten- tial . In most substances the potential energy between two molecules as ...
Page 275
... potential . In the quantum theory of scattering it is known that at low energies the scattering of a particle by a potential does not depend on the shape of the potential , but depends only on a single parameter obtainable from the ...
... potential . In the quantum theory of scattering it is known that at low energies the scattering of a particle by a potential does not depend on the shape of the potential , but depends only on a single parameter obtainable from the ...
Page 279
... potential Fig . 13.2 . Wave function in an attractive potential with negative scattering length . where no is by definition the S - wave phase shift . For k → 0 , Y∞ ( r ) 014 const . ( 1 + tan rie ) kr ( 13.21 ) In general no is a ...
... potential Fig . 13.2 . Wave function in an attractive potential with negative scattering length . where no is by definition the S - wave phase shift . For k → 0 , Y∞ ( r ) 014 const . ( 1 + tan rie ) kr ( 13.21 ) In general no is a ...
Contents
THE LAWS OF THERMODYNAMICS | 3 |
SOME APPLICATIONS OF THERMODYNAMICS | 33 |
THE PROBLEM OF KINETIC THEORY | 55 |
Copyright | |
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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